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<strong>Engine</strong> <strong>Titanium</strong> <strong>Consortium</strong><br />

Quarterly Report<br />

January 1, 2002 – March 31, 2002<br />

Lisa Brasche, Bruce Thompson, ISU<br />

Andy Kinney, HW<br />

Thadd Patton, John Halase, GE<br />

Kevin Smith, Jeff Umbach, P&W<br />

on behalf of the <strong>Engine</strong> <strong>Titanium</strong> <strong>Consortium</strong> team<br />

June 1, 2002


Table of Contents<br />

TASK 1.1: NICKEL-BASED ALLOY INSPECTION ............................................................................................. 2<br />

SUBTASK 1.1.1: FUNDAMENTAL PROPERTY MEASUREMENTS FOR NICKEL BILLET ........................ 2<br />

SUBTASK 1.1.2: INSPECTION DEVELOPMENT FOR NICKEL BILLET..................................................... 13<br />

TASK 1.2: TITANIUM BILLET INSPECTION....................................................................................................... 20<br />

SUBTASK 1.2.1: INSPECTION DEVELOPMENT FOR TITANIUM BILLET................................................. 20<br />

TASK 1.3: TITANIUM FORGING INSPECTION .................................................................................................. 34<br />

SUBTASK 1.3.1:<br />

FUNDAMENTAL PROPERTY MEASUREMENTS FOR TITANIUM<br />

FORGINGS ....................................................................................................................... 34<br />

SUBTASK 1.3.2: INSPECTION DEVELOPMENT FOR TITANIUM FORGINGS.......................................... 54<br />

TASK 2.1: INSPECTION DEVELOPMENT FOR ROTATING COMPONENTS ................................................... 70<br />

SUBTASK 2.1.1: DEVELOPMENT OF UT CAPABILITY FOR INSERVICE INSPECTION .......................... 70<br />

SUBTASK 2.1.2: EDDY CURRENT PROBE EVALUATION AND IMPLEMENTATION ............................... 70<br />

TASK 2.2: INSPECTION DEVELOPMENT TRANSITIONS TO AIRLINE MAINTENANCE ................................ 70<br />

SUBTASK 2.2.1: APPLICATION OF ETC TOOLS IN OVERHAUL SHOPS – EC SCANNING.................... 70<br />

SUBTASK 2.2.2: HIGH SPEED BOLTHOLE EDDY CURRENT SCANNING............................................... 71<br />

SUBTASK 2.2.3:<br />

ENGINEERING STUDIES OF CLEANING AND DRYING PROCESS IN<br />

PREPARATION FOR FPI ................................................................................................. 77<br />

TASK 3.1: POD METHODOLOGY APPLICATIONS ........................................................................................... 86<br />

SUBTASK 3.1.1: POD OF ULTRASONIC INSPECTION OF BILLETS ........................................................ 86<br />

SUBTASK 3.1.2: POD OF ULTRASONIC INSPECTION OF TITANIUM FORGINGS ................................. 98<br />

SUBTASK 3.1.3: POD OF EDDY CURRENT INSPECTIONS IN THE FIELD.............................................. 106<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 1


Project 1:<br />

Task 1.1:<br />

Subtask 1.1.1:<br />

Production Inspection<br />

Nickel-based Alloy Inspection<br />

Fundamental Property<br />

Measurements <strong>for</strong> Nickel Billet<br />

Team Members:<br />

HW: Andy Kinney, Waled Hassan<br />

ISU: Frank Margetan, Bruce Thompson,<br />

Ron Roberts<br />

GE: Ed Nieters, Mike Gigliotti, Lee<br />

Perocchi, Jon Bartos, Mike Keller, Richard<br />

Klaassen, John Halase, Dave Copley<br />

PW: Jeff Umbach, Bob Goodwin, Andrei<br />

Degtyar, Harpreet Wasan<br />

Students: L. Yu<br />

Program initiation date: June 15, 1999<br />

Objectives:<br />

• To establish the basic ultrasonic properties of nickel-based alloy billet materials (Expected to be<br />

IN718, and one or more of Waspaloy, IN901, R95, or IN100) and relevant inclusions as an<br />

appropriate foundation <strong>for</strong> selection of ultrasonic inspection approaches.<br />

• To manufacture and characterize flat bottom hole (FBH), synthetic inclusion, and real defect<br />

standards to provide data <strong>for</strong> determining defect detectability and developing improved<br />

inspections.<br />

• To improve the understanding of the relationship of defect size, shape, and composition on<br />

defect detectability in Ni alloys.<br />

Approach:<br />

Alloy Selection: Several alloys have been selected <strong>for</strong> fundamental property measurements with<br />

IN718 selected to receive the primary focus. Alloys to be considered include Waspaloy, IN100,<br />

IN901, and R95. Sample design and fabrication <strong>for</strong> properties measurements will be initiated by<br />

the team members. A list of the types of melt-related defects encountered at the billet stage in<br />

Ni-based alloys, defect morphology in the <strong>for</strong>ged condition, and importance to life management will<br />

be generated by RISC. The importance of defect parameters (size, concentration, morphology,<br />

presence of voids) on detectability and life will be determined through discussion with the lifing and<br />

materials communities.<br />

Sample Fabrication: The sequence of manufacturing the properties specimens and the specimen<br />

configuration will be planned to yield as much data as possible on properties as a function of depth<br />

and orientation. Novel configurations of coupons, and sequences of coupon extraction and<br />

characterization will be considered. Sample fabrication procedures will be coordinated with the<br />

Inspection Systems Capability Working Group to ensure use by both groups<br />

The proposed billet coupon scheme is shown in Figure 1. Because backscattered noise levels are<br />

strongly dependent on details of the metal microstructure, they can be used to guide the selection<br />

of coupon locations. From low and high noise regions, a "strip" specimen will be cut along the billet<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 2


diameter, with transverse dimensions of<br />

approximately 1.5" x 1.5". This specimen<br />

would initially be used <strong>for</strong> property<br />

measurements in the axial and hoop<br />

directions at various depths. The strip<br />

specimen would then be sliced into a<br />

series of coupons and be used <strong>for</strong> property<br />

measurements in the radial direction. The<br />

team will agree on the final specimen<br />

configuration early in the program, using<br />

the approach described here as a starting<br />

point. Similar schemes will also be used<br />

to study ultrasonic properties in the axial<br />

and hoop directions as a function of<br />

position. Results of the anisotropy<br />

measurements will be provided to the<br />

Inspection Systems Capability Working<br />

Group <strong>for</strong> incorporation into the noise<br />

models and ultimately will be used to<br />

predict the change in POD as a function of<br />

position. The data will also provide<br />

guidance in design of transducers and<br />

optimal inspection parameters <strong>for</strong> nickel<br />

billet in subtask 1.1.2.<br />

Ultrasonic Property Measurements:<br />

Baseline ultrasonic properties (velocity,<br />

attenuation, and backscattered noise) of<br />

nickel billets will also be gathered <strong>for</strong><br />

Axial Position<br />

Circumferential Position<br />

determination of the impact of properties on inspectability. Samples will be selected to address<br />

beam variability, with the expected sample set to include approximately 16 samples <strong>for</strong> each alloy.<br />

In Phase I, the ultrasonic properties of titanium billets were found to vary with position and<br />

inspection parameters, and similar variations are expected in nickel alloy billets and <strong>for</strong>gings.<br />

Selection of billets <strong>for</strong> properties specimens will be based on an initial screening inspection.<br />

Ultrasonic property measurements of the base alloys will provide the necessary noise distribution<br />

data <strong>for</strong> use by the Inspection Systems Capability Working Group in generating POD estimates <strong>for</strong><br />

nickel billet. Signal distributions will be generated using FBH, synthetics, and the natural defects<br />

fabricated as defined above. Data on the natural defects will be used to develop and validate the<br />

flaw response and noise models and to generate the POD estimates <strong>for</strong> nickel billet in 3.1.1.<br />

Measurements on billet coupons will allow the team to assemble a more comprehensive picture of<br />

ultrasonic property variations within the billet, and to better understand the effect of these variations<br />

on inspectability. Correlations will be sought between the property variations with variations in the<br />

metal microstructure as revealed by optical micrographs and SEM studies. After assessing the<br />

Billet<br />

Hoop<br />

Measurement<br />

Axial<br />

measurement<br />

“Strip”<br />

Specimen<br />

(~ 1.5” x 1.5” x D)<br />

(b)<br />

High<br />

Noise<br />

(a)<br />

Radial<br />

Measurement<br />

Ref.<br />

Mark<br />

Low<br />

Noise<br />

2nd-stage coupons<br />

Figure 1. (a) C-scan map of backscattered noise<br />

versus position, showing locations of high-noise and<br />

low-noise "strip" specimens. (b, c). Specimen and<br />

smaller sub-coupons will be used to study depth<br />

dependence of ultrasonic properties in the three<br />

orthogonal inspection directions.<br />

(c)<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 3


findings <strong>for</strong> the first billet studied, the coupon manufacturing procedure will be refined as necessary<br />

<strong>for</strong> subsequent billets and <strong>for</strong>gings.<br />

Synthetic Inclusion Samples: Synthetic inclusions will be embedded into Ni test standards <strong>for</strong> the<br />

purpose of evaluating the inspection sensitivity of ultrasonics on melt-related defects. The team will<br />

review the findings from the metallurgical analysis on the naturally occurring defects to identify the<br />

candidate inclusion types <strong>for</strong> sample manufacture. Construction methods will be developed at<br />

GE-CRD to chemically manufacture the synthetic inclusions and to embed the inclusions into Ni<br />

alloy test blocks. After the successful development of synthetic inclusion manufacturing methods,<br />

three blocks containing synthetic inclusions of different geometry and composition will be<br />

manufactured. The types of inclusions will be determined by the team based on the ability to<br />

manufacture the synthetic inclusions, the criticality of the defect to part life, and the sensitivity of the<br />

inspection to the composition and geometry of the defect type.<br />

The team will ultrasonically evaluate the synthetic inclusion samples to determine the sensitivity of<br />

the inspections <strong>for</strong> detecting and characterizing melt-related defects. This data will be used <strong>for</strong> the<br />

validation of computer-based flaw models and <strong>for</strong> the generation of POD curves <strong>for</strong> Ni alloy billets.<br />

Defect Characterization: Samples will also be acquired with real defects potentially to include dirty<br />

white spots, segregation (freckles), and slag (from ESR), reflecting both VIM/VAR and<br />

VIM/ESR/VAR material defects in 718 and Waspaloy. The initial ef<strong>for</strong>t will focus on evaluation of<br />

natural defects to establish typical compositions and properties and their detectability. Six samples<br />

will be evaluated using a limited ultrasonic characterization and a simplified metallographic process.<br />

Ultrasonic measurements will be per<strong>for</strong>med at two stages:<br />

• original samples prior to sectioning<br />

• defects machined to regular shapes<br />

Characterization data will be used to optimize the inspection development ef<strong>for</strong>ts of 1.1.2, provide<br />

data <strong>for</strong> validation of flaw models and provide input <strong>for</strong> generation of POD <strong>for</strong> nickel billet in 3.1.1.<br />

Results will be included in the final report.<br />

Objective/Approach Amendments: Objective and approach remain as originally proposed in July<br />

1998.<br />

Progress (January 1, 2002 – March 31, 2002):<br />

Several consortium conference calls were conducted during the quarter to discuss the details of the<br />

subtask. A number of technical issues were discussed and decisions reached. The technical<br />

issues and discussions are summarized into two primary areas, (1) Property Measurements, and<br />

(2) Metallographic Microstructure which are discussed separately below.<br />

Property Measurements<br />

A primary goal of the Ni billet Fundamental Studies subtask is to determine, <strong>for</strong> representative Nialloy<br />

billets, the manner in which ultrasonic properties depend on inspection direction and position<br />

within the billet. The inspection properties of interest are the sonic velocity, attenuation, and<br />

backscattered grain noise level, with the latter two properties strongly dependent on the inspection<br />

frequency. Results of the property measurements will later be used by the Production and<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 4


Reliability subtasks to better estimate inspection sensitivities and POD values <strong>for</strong> Nickel billet<br />

inspections. .<br />

During the quarter, work continued on four “strip coupons” cut from representative Ni alloy billets<br />

and designated<br />

• GFMA : From a high-noise site of a 10”-diameter IN718 GFM-<strong>for</strong>ged billet.<br />

• VdieA : From a high-noise site of a 10”-diameter IN718 V-die-<strong>for</strong>ged billet.<br />

• VdieB : From a low-noise site of the above billet.<br />

• WaspA : From a high-noise site of a 10”-diameter Waspaloy billet.<br />

Figure 1a shows the nominal geometries <strong>for</strong> each strip coupon (used <strong>for</strong> UT measurements in the<br />

axial and hoop directions) and the “baloney slices” that were later cut from the strip coupons (used<br />

<strong>for</strong> UT measurements in the radial direction). Ultrasonic data acquisition on all coupons has been<br />

completed, although analysis of the data is ongoing.<br />

Metallographic Microstructure<br />

A related goal of the subtask is to correlate the measured ultrasonic properties with the local billet<br />

microstructure. To this end, small metallographic coupons from selected billet sites have been<br />

polished and etched to reveal the grain structure, and grain size distributions have been measured<br />

from micrographs. During the Jan-Mar quarter, the majority of the research ef<strong>for</strong>t was spent<br />

completing the metallographic measurements and analyses. We now have deduced grain size<br />

in<strong>for</strong>mation from 12 metallography coupons (4 sites x 3 views) <strong>for</strong> each of the four Ni-alloy strips.<br />

Labels and locations of the metallographic coupons in a typical strip are shown in Figure 1b.<br />

Two different methods, illustrated in Figure 2, were used to deduce average grain diameters from a<br />

given micrograph. The first, known as the Mean Chord Length (MCL) method is equivalent to: (1)<br />

drawing a straight line through the micrograph; (2) noting where the line crosses grain boundaries;<br />

(3) calculating the average length of the straight segments which lie within a single grain; and (4)<br />

multiplying this average chord length by 1.5 to obtain a grain diameter estimate. A computer<br />

program operating on a digital image of the grain boundaries is used to “draw” all possible lines in<br />

either the horizontal (X) or vertical (Y) direction. The conversion factor of 1.5, which translates from<br />

2D images to 3D diameters, is believed to be appropriate <strong>for</strong> equiaxed grains of the kind seen in<br />

these billets.<br />

In an alternative approach, known as the “P(L) Method”, one determines the probability P that a line<br />

segment of length L, randomly placed on the micrograph, lies entirely within a single grain . Again a<br />

computer program is used to generate the line segments and to decide whether a given segment<br />

crosses a grain boundary. Again the method can be applied separately in the X and Y directions of<br />

Figure 2. The X or Y analysis of a micrograph yields a probability-versus-length curve, P(L). This<br />

curve is then fit to an exponential function P(L) = exp(-L/b), and 2b is used as an estimate of the<br />

mean grain diameter. Typical measured P(L) curves do not exactly follow an exponential function,<br />

leading to some uncertainty in the fitting parameter “b” and the associated grain diameter estimate.<br />

To document this uncertainty, we per<strong>for</strong>m separate fits to different regions of the measured P(L)<br />

curve . This is illustrated in Figure 3, where fits to the “low L’’ and “high L” halves of the data are<br />

shown <strong>for</strong> one case. In practice we per<strong>for</strong>m separate fits to 10 overlapping regions of the<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 5


measured P(L) curve, and tabulate the minimum, maximum, and mean values of “b” thus obtained.<br />

We note that P(L) curves, sometimes referred to as two-point correlation functions, are of interest<br />

because they appear in a direct manner in certain models of ultrasonic attenuation and<br />

backscattered grain noise.<br />

In all of the cases examined, the grain cross-sections seen in the micrographs have roughly similar<br />

average dimensions in the X and Y directions, indicating an equiaxed grain structure. This is<br />

demonstrated in Figure 4 <strong>for</strong> the MCL method. The P(L) analysis similarly finds nearly equiaxed<br />

grain diameters. As shown in Figures 5 and 6, the two methods generally yield similar average<br />

grain diameters. When a given micrograph is analyzed, the MCL estimate usually falls in between<br />

the minimum and maximum estimates from the P(L) method. As shown in Figure 6, the average<br />

grain diameter estimate from the P(L) method tends to be about 5% below that of the MCL method.<br />

Since the grains appear to be equiaxed and the two analysis methods yield similar diameter<br />

estimates, we average over the two analysis directions [X and Y] and over the two methods [MCL<br />

and average P(L)] to arrive at an overall grain diameter estimate <strong>for</strong> each micrograph.<br />

One step in the analysis of each micrograph is the construction of a tracing showing only the true<br />

grain boundaries. When such tracings are made, so-called “twin boundaries” are intentionally<br />

excluded, since it is believed that they do not significantly contribute to attenuation and backscattered<br />

noise. Our goal is to correlate the grain diameter estimates with ultrasonic properties.<br />

Absolute errors in grain diameter estimates are believed to mainly arise from two factors: (1) the<br />

process of identifying “non-twin” grain boundaries is somewhat subjective; and (2) a given<br />

micrograph containing a few hundred grains represents only a very minute fraction of the specimen<br />

volume that is insonified in a given ultrasonic measurement.<br />

During the quarter, ef<strong>for</strong>ts were made to correlate the measured grain diameters at various billet<br />

sites with the ultrasonic attenuation values measured earlier. Figure 7 displays the attenuation<br />

values at 7.5 MHz <strong>for</strong> all measurement sites and inspection directions. Absolute attenuation values<br />

are believed to be accurate to within about +/-0.0015 N/cm or +/-0.03 dB/inch. Given this level of<br />

accuracy, one sees that at a given site in a given specimen, the ultrasonic attenuation is quite<br />

isotropic. For three of the specimens (strip coupons) the attenuation drops significantly as one<br />

approaches the OD from the billet center. For the fourth specimen (V-die-A), the attenuation<br />

increases as the OD is approached. The correlation between measured attenuation values and<br />

measured grain diameters is shown in Figure 8. Significant scatter is seen about the general trend.<br />

This is believed to be primarily due to the fact that the grain size determinations were made using<br />

only a very small fraction of the grains contained within the ensonified volume. Nonetheless, a<br />

general trend is seen of the same shape as that expected <strong>for</strong> equiaxed, untextured, pure Nickel<br />

grains.<br />

In the upcoming quarter, the ongoing analysis of all backscattered grain noise data will be<br />

completed, and figures similar to Figures 7-8 will be generated showing the dependence of noise<br />

FOM on position and its correlation with average grain diameter.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 6


Axial<br />

“rough cut” coupon <strong>for</strong><br />

use in metallography<br />

Billet<br />

1”-thick “slice”<br />

coupons<br />

“strip coupon” <strong>for</strong> UT<br />

property measurements<br />

possible sites <strong>for</strong><br />

metallography<br />

Hoop<br />

Radial<br />

“Strip”<br />

Coupon<br />

(~ 2” x 2” x 10”)<br />

(a)<br />

J K<br />

L<br />

G<br />

H<br />

I<br />

D<br />

E<br />

F<br />

A<br />

B<br />

C<br />

Polished face: Axial<br />

Polished face: Radial<br />

Polished face: Hoop<br />

(b)<br />

10”<br />

Figure 1. Geometries of “strip” and “slice” coupons from Ni-alloy billets. (b) Locations and<br />

designations of the 12 small metallography coupons, A-L.<br />

100 µm<br />

L<br />

100 µm<br />

Twin<br />

boundaries<br />

L<br />

Twin<br />

boundaries<br />

Y<br />

S1<br />

Waspaloy<br />

Coupon K<br />

S2<br />

S3<br />

S4<br />

L<br />

Waspaloy<br />

Coupon K<br />

L<br />

L<br />

X<br />

MCL Method<br />

Lines are drawn. Average of the<br />

chord lengths (Sj) is calculated.<br />

P(L) Method<br />

For a given length L, line segments of<br />

that length are randomly placed on the<br />

image. Some cross grain boundaries,<br />

some do not. Count each type.<br />

Figure 2. The two methods used to analyze micrographs. Each method leads to an estimate of the<br />

average grain diameter.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 7


1.2<br />

1.0<br />

0.8<br />

V-DIE-A coupon "D" (axial view)<br />

Measured P(L) - x&y combined<br />

Low-L exponential fit (b = 11.50 microns)<br />

High L exponential fit (b = 9.26 microns)<br />

P(L)<br />

0.6<br />

0.4<br />

0.2<br />

0.0<br />

0 10 20 30 40 50 60<br />

L (microns)<br />

Figure 3. Examples of exponential fits to a measured P(L) curve. The blue curve is a fit to the<br />

lower half of the data (0 < L < 27 microns). The red curve is a fit to the upper half of the data (27 <<br />

L < 54 microns).<br />

Estimate along Y-direction .<br />

160<br />

140<br />

120<br />

100<br />

80<br />

60<br />

40<br />

20<br />

GRAIN DIAMETER ESTIMATES<br />

USING THE MCL METHOD<br />

GFMA<br />

V-DIE-A<br />

V-DIE-B<br />

WASP<br />

Equiaxed Grains<br />

(in microns)<br />

Estimate along Y-direction .<br />

40<br />

35<br />

30<br />

25<br />

20<br />

15<br />

10<br />

5<br />

GRAIN DIAMETER ESTIMATES<br />

USING THE MCL METHOD<br />

GFMA<br />

V-DIE-A<br />

V-DIE-B<br />

Equiaxed Grains<br />

(in microns)<br />

0<br />

0 20 40 60 80 100 120 140<br />

Estimate along X-direction<br />

0<br />

0 5 10 15 20 25 30 35 40<br />

Estimate along X-direction<br />

Figure 4. Comparisons of average grain diameters in the X and Y directions of the micrographs<br />

using the Mean Chord Length Method. Results are shown <strong>for</strong> analyses of 12 micrographs <strong>for</strong> each<br />

of 4 billet “strips”. The right-hand panel is a blow-up of the small diameter region where the IN718<br />

values lie.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 8


Ave. Grain Diameter (microns) .<br />

30<br />

25<br />

20<br />

15<br />

10<br />

5<br />

0<br />

V-die B Metallography Results<br />

(Sorted by increasing MCL)<br />

Fitting exponentials [exp(-L/b)] to<br />

different regions of the P(L) data<br />

leads to three different estimates of b:<br />

highest b, low est b, and average b.<br />

MCL = Mean Chord Length.<br />

D from 1.5*MCL<br />

D from 2*(ave b)<br />

D from 2*(low b)<br />

D from 2*(high b)<br />

I H L G E J C D K F A B<br />

Metallography Coupon<br />

Figure 5. Comparisons of average grain diameters as estimated by the MCL and P(L) methods.<br />

Results (averaged over X and Y) are shown <strong>for</strong> the 12 V-die-B micrographs. For the P(L) method,<br />

high, low , and average estimates are given, resulting from fitting exponentials to different regions<br />

of the P(L) curve.<br />

P(L) ESTIMATE (microns) .<br />

160<br />

140<br />

120<br />

100<br />

80<br />

60<br />

40<br />

20<br />

0<br />

GRAIN DIAMETER ESTIMATES<br />

(Averaged over X and Y)<br />

GFMA<br />

V-DIE-A<br />

V-DIE-B<br />

WASP<br />

TRENDLINE<br />

y = 0.9461x<br />

R2 = 0.9796<br />

0 20 40 60 80 100 120 140 160<br />

MCL ESTIMATE (microns)<br />

Figure 6. Comparisons of average grain diameters as estimated by the MCL and average-P(L)<br />

methods <strong>for</strong> the 4 x 12 micrographs analyzed. A best-fit trendline through the data is also shown.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 9


Attenuation (dB/in) .<br />

Waspalloy Attenuation at 7.5 MHz<br />

4.00<br />

3.50<br />

Axial<br />

3.00<br />

Hoop<br />

2.50<br />

Radial<br />

2.00<br />

1.50<br />

1.00<br />

0.50<br />

0.00<br />

0" 1" 2" 3" 4"<br />

(center)<br />

Measurement Site<br />

Attenuation (dB/in) .<br />

0.35<br />

0.30<br />

0.25<br />

0.20<br />

0.15<br />

0.10<br />

0.05<br />

0.00<br />

GFM-A Attenuation at 7.5 MHz<br />

Axial<br />

Hoop<br />

Radial<br />

0" 1" 2" 3" 4"<br />

(center)<br />

Measurement Site<br />

Attenuation (dB/in) .<br />

0.35<br />

0.30<br />

0.25<br />

0.20<br />

0.15<br />

0.10<br />

0.05<br />

0.00<br />

V-Die-A Attenuation at 7.5 MHz<br />

Axial<br />

Hoop<br />

Radial<br />

0" 1" 2" 3" 4"<br />

(center)<br />

Measurement Site<br />

Attenuation (dB/in) .<br />

V-Die-B Attenuation at 7.5 MHz<br />

0.16<br />

0.14<br />

0.12<br />

0.10<br />

0.08<br />

0.06<br />

0.04<br />

0.02<br />

0.00<br />

Axial<br />

Hoop<br />

Radial<br />

0" 1" 2" 3" 4"<br />

(center)<br />

Measurement Site<br />

Figure 7. Measured attenuation values at 7.5 MHz <strong>for</strong> the Ni billet specimens. Results are shown<br />

<strong>for</strong> three orthogonal inspection directions. The distance from each measurement site to the billet<br />

center is indicated.<br />

Attenuation at 7.5 MHz (dB/in)<br />

7<br />

6<br />

5<br />

4<br />

3<br />

2<br />

1<br />

Correlation Between Measured Attenuation and<br />

Measured Average Grain Diameter<br />

GFM-A<br />

VDIE-A<br />

VDIE-B<br />

Wasp<br />

JT model <strong>for</strong> pure Ni<br />

Waspaloy Trendline<br />

Note : tw in boundares<br />

w ere not counted as bona<br />

fide grain boundaries.<br />

Attenuation at 7.5 MHz (dB/in)<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

Correlation Between Measured Attenuation and<br />

Measured Average Grain Diameter<br />

GFM-A<br />

VDIE-A<br />

VDIE-B<br />

Wasp<br />

JT model <strong>for</strong> pure Ni<br />

IN718 Trendline<br />

Note : tw in boundares<br />

w ere not counted as bona<br />

fide grain boundaries.<br />

Vdie_A<br />

coupons<br />

H, I, L<br />

0<br />

0 20 40 60 80 100 120<br />

Estimated Grain Diameter (microns)<br />

0.0<br />

0 10 20 30 40<br />

Estimated Grain Diameter (microns)<br />

Figure 8. Correlation between measured attenuation at 7.5 MHz and estimated average grain<br />

diameter. Right panel shows a blow-up of the region near the plot origin. The prediction of the Joe<br />

Turner Attenuation Model (<strong>for</strong> pure Nickel) is shown <strong>for</strong> comparison, along with a trend lines<br />

through the data with the same shape as the model curve.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Plans (April 1, 2002 – June 30, 2002):<br />

Ongoing analysis of all backscattered grain noise data will be completed.<br />

Milestones:<br />

Original<br />

Revised<br />

Description<br />

Status<br />

Date<br />

Date<br />

Fundamental properties of nickel billet<br />

3 months 6 months<br />

(Waspaloy)<br />

6 months<br />

(Waspaloy)<br />

Finalize sample configuration and manufacturing<br />

sequence. (All)<br />

Initiate sample fabrication. (GE, PW; GE to supply<br />

IN718, PW to supply Waspaloy)<br />

6 months Coordinate with RISC to generate list of<br />

melt-related defects and provide to Inspection<br />

Development and Inspection Systems Capability<br />

teams. Identify preferred defect types <strong>for</strong> study.<br />

Initiate acquisition of naturally occurring<br />

melt-related defects. (All)<br />

Complete<br />

Complete<br />

Complete<br />

18 months 42 months Metallographically evaluate natural defects. Synthetic defects selected<br />

First natural defect identified and<br />

evaluation initiated in Dec. 2000<br />

30 months Establish methods <strong>for</strong> manufacturing synthetic<br />

defects and <strong>for</strong> embedding synthetic and natural<br />

defects in IN718 (GE).<br />

24 months Complete property measurement samples. (GE,<br />

PW)<br />

36 months Complete synthetic inclusion standards with<br />

representative variation in type, geometry, and<br />

chemistry. (GE)<br />

36 months Complete characterization of property samples and<br />

provide to 3.1.1 <strong>for</strong> development of flaw response<br />

and noise models and <strong>for</strong> generation of the noise<br />

distribution <strong>for</strong> nickel. Includes ultrasonic velocity,<br />

attenuation, noise, microstructure. (ISU with<br />

support from GE, PW,AS)<br />

Coordinate results with 1.1.2 in the inspection<br />

design and implementation. (ISU with support from<br />

GE, PW,AS)<br />

42 months Report of ultrasonic properties (sound velocity,<br />

attenuation, and backscattered noise) and types of<br />

defects of concern in IN718 , Waspaloy, and IN901.<br />

(All)<br />

24-42<br />

months<br />

Validate noise models in cooperation with 3.1.1.<br />

(All)<br />

42 months Complete ultrasonic characterization of melt-related<br />

defects and provide results to 3.1.1. (All))<br />

54 months Report of characterization of defects and ultrasonic<br />

properties (sound velocity and acoustic impedance)<br />

as a function of composition <strong>for</strong> defects in IN718.<br />

(All)<br />

60 months Representative sample blocks and synthetic<br />

inclusion samples (All)<br />

Complete<br />

Synthetic dirty white spot, freckle,<br />

and white spot defects prepared<br />

Acoustic measurements initiated at<br />

ISU<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Deliverables:<br />

Fundamental properties of nickel billet.<br />

Report of ultrasonic properties (sound velocity, attenuation, and backscattered noise) and types of<br />

defects of concern in IN718, Waspaloy, and IN901.<br />

Report of characterization of defects and ultrasonic properties (sound velocity and acoustic<br />

impedance) as a function of composition <strong>for</strong> defects in IN718.<br />

Representative sample blocks and synthetic inclusion samples.<br />

Metrics:<br />

Assessment of ultrasonic properties <strong>for</strong> typical nickel alloys and characterization of melt-related<br />

defects that support the needs of inspection development, POD estimation, and life management.<br />

Major Accomplishments and Significant Interactions:<br />

Date<br />

June 16, 1999<br />

December 21,<br />

1999<br />

Description<br />

Technical Kick-off Meeting in West Palm Beach, FL<br />

Telecon with Special Metals and Sandia National Lab personnel to discuss their experience with Ni<br />

defects and initiate discussions on obtaining natural Ni defect samples<br />

Publications and Presentations:<br />

Date<br />

Description<br />

2002 Pranaam Haldipur, F. J. Margetan, Linxiao Yu, and R. B. Thompson, "A study of Ultrasonic<br />

Property Variations Within Jet-<strong>Engine</strong> Nickel Alloy Billets", Rev. of Prog. in QNDE, Vol.21,<br />

eds. D.O. Thompson and D.E. Chimenti, (AIP, Melville NY, in press)<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Project 1:<br />

Task 1.1:<br />

Subtask 1.1.2:<br />

Production Inspection<br />

Nickel-based Alloy Inspection<br />

Inspection Development <strong>for</strong><br />

Nickel Billet<br />

Team Members:<br />

HW: Andy Kinney, Waled Hassan<br />

ISU: Ron Roberts, Bruce Thompson, Frank<br />

Margetan<br />

GE: Ed Nieters, Dave Copley, Mike Keller,<br />

Jon Bartos, Richard Klaassen, John Halase<br />

PW: Jeff Umbach, Bob Goodwin, Andrei<br />

Degtyar, Harpreet Wasan<br />

Students: none<br />

Program initiation date: June 15, 1999<br />

Objectives:<br />

• To apply technology developed in Phase I <strong>for</strong> titanium billet inspection to improve nickel billet<br />

inspection.<br />

• To per<strong>for</strong>m factory inspection of approximately 100,000 pounds of nickel alloy billet, primarily<br />

INCO718, to #1 FBH sensitivity using a multizone inspection system with digital acquisition to<br />

provide necessary field experience that facilitates implementation decisions.<br />

• To determine applicability of multizone technique to Waspaloy.<br />

• To provide the billet industry and OEMs with demonstration of improved sensitivity inspection<br />

using FBH standards as the metric with a goal of #1FBH sensitivity in 10” INCO718 billets and<br />

#2.5FBH sensitivity in 10” Waspaloy billet.<br />

• To provide necessary data to the Inspection Systems Capability team <strong>for</strong> estimation of POD <strong>for</strong><br />

nickel billet, including cut-up data generated in the pilot lot inspection.<br />

Approach:<br />

Initial Assessment: A kickoff meeting involving the subtask team members will be held at the<br />

program onset to reiterate the plans of the task and establish a means of sharing in<strong>for</strong>mation and<br />

data, including necessary support of Task 3.1.1. The current plan of concentrating on INCO718<br />

and Waspaloy to sensitivities of #1FBH and #2.5FBH sensitivity respectively will be verified as the<br />

correct targets and requirements <strong>for</strong> signal-to-noise measurements will be determined. The<br />

number and types of calibration standards will be discussed and design of the standards will be<br />

initiated. Any significant change agreed on by the team will be presented to ETC management.<br />

Production calibration standards <strong>for</strong> the nickel alloys, presumably 10” diameter, as agreed upon in<br />

the initial planning meeting will be manufactured. An evaluation of current capability of<br />

conventional inspections will be per<strong>for</strong>med as a baseline <strong>for</strong> both INCO718 and Waspaloy using the<br />

production calibration standards rather than relying on the nominal values stated in respective<br />

specifications.<br />

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Small Diameter Billet Assessment: Assessment of small diameter inspection will also be completed<br />

by Honeywell. Honeywell will per<strong>for</strong>m studies using billets of < 8” diameter The objective will be to<br />

apply technology developed in Phase II <strong>for</strong> larger Ni billet to improve nickel billet inspection in the<br />

stated diameter of interest to small engine manufacturers. Feasibility demonstration will be<br />

conducted in the laboratory environment using small nickel alloy billet and multizone transducers<br />

developed <strong>for</strong> the smallest of the large diameter billets. Sensitivity analysis (#FBH) will be<br />

conducted <strong>for</strong> various small diameter billets. A comparison will be made with the standard<br />

spherical focus approach. Results will be provided to the Inspection Systems Capability Working<br />

Group to allow POD estimates.<br />

Baseline Assessment: Inspection development will be per<strong>for</strong>med with the calibration standards<br />

using existing multizone transducers to occur at PW and GE facilities to ensure hands-on<br />

involvement by the parties responsible <strong>for</strong> final implementation recommendations. Scans and<br />

associated measurements will be used to determine the focal depth of each transducer, measure<br />

the axial beam profile and beam cross-section, and compare these results to model predictions.<br />

Signal-to-noise ratio will be determined <strong>for</strong> the FBH targets. The need <strong>for</strong> new transducers will be<br />

evaluated based on these scans and model results. New transducers will be designed and built if<br />

results indicate that the existing transducers do not produce a focal zone at the required depth or of<br />

the required beam diameter, and if modeling indicates that significant improvement could be<br />

obtained by re-design. Additional funding will be sought <strong>for</strong> transducer fabrication at that time if the<br />

team agrees that the proposed benefits are substantial.<br />

Laboratory Demonstration: After inspection development <strong>for</strong> each alloy is completed, a laboratory<br />

demonstration of billet inspections with optimized transducers will be provided <strong>for</strong> the ETC<br />

members. Sensitivity to #1FBH in INCO718 and to #2.5FBH in Waspaloy will be demonstrated and<br />

plans made <strong>for</strong> pilot inspection.<br />

Factory Demonstration: A factory pilot inspection of approximately 100,000 pounds will be planned<br />

to determine the sensitivity level that can be consistently achieved in production and to identify any<br />

barriers to implementation. The first step will be <strong>for</strong> the team to identify an industry partner(s) to<br />

per<strong>for</strong>m the pilot inspection, much as RMI worked with the consortium in Phase I in the inspection<br />

of titanium billet. A detailed plan will identify the particular specifications of INCO718 to be<br />

inspected, i.e., VIM/VAR and/or VIM/ESR/VAR, and the number of material suppliers.<br />

Investigations per<strong>for</strong>med in the nickel fundamental studies Task 1.1.1, will provide in<strong>for</strong>mation to<br />

determine the need to include two types of INCO718 in the pilot inspection. If the defect types<br />

found in the two materials and the ultrasonic characteristics are the same, then there will not be a<br />

need to include both in the factory pilot inspection. The extent of inclusion of Waspaloy will also be<br />

planned. Procedures <strong>for</strong> inspection, evaluation of data, and investigation of indications will be<br />

defined. It is expected that eight finds will be cut-up and evaluated using a process similar to that<br />

described in AC 33.15. It is expected that each OEM will participate in the destructive<br />

characterization of indications with two planned <strong>for</strong> Waspaloy and six planned <strong>for</strong> IN718. The team<br />

will also agree on parameters needed to determine the cost impact of implementing the higher<br />

sensitivity inspection as compared to conventional inspection. The pilot lot evaluation of 100,000<br />

pounds of billet with the optimum transducers will occur in cooperation with a multizone inspection<br />

source and nickel alloy material suppliers. <strong>Evaluation</strong> of 5 to 10 heats of material is expected.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Since application of multizone technique is expected to be more straight<strong>for</strong>ward <strong>for</strong> INCO718, most<br />

of the pilot work will be per<strong>for</strong>med with that alloy. The application of #2.5FBH sensitivity to<br />

Waspaloy is expected to be more complex but an inspection technique should be ready to<br />

substitute <strong>for</strong> the last 25% of the pilot lot. The data will be evaluated and reported. Results of the<br />

pilot inspection and of any cut-ups will be provided to Task 3.1.1 <strong>for</strong> use in developing POD<br />

estimates <strong>for</strong> nickel billet. Cost and detection sensitivity assessments necessary <strong>for</strong> life<br />

management and implementation decisions will be gathered. Components of cost assessment will<br />

have been agreed on by the team and will likely include such items as system cost, longevity of<br />

equipment, recurring equipment costs, daily operational/inspection costs, and costs associated with<br />

false calls. In conjunction with the pilot lot inspection, a demonstration of the higher sensitivity<br />

inspection <strong>for</strong> INCO718 and Waspaloy will be presented to the OEMs and industry. A final report in<br />

the required FAA <strong>for</strong>mat will be provided.<br />

Objective/Approach Amendments: Objective and approach remain as originally proposed in July<br />

1998.<br />

Progress (January 1, 2002 – March 31, 2002):<br />

Several consortium conference calls were conducted during the quarter to discuss the details of the<br />

subtask. A number of technical issues were discussed and decisions reached. The technical<br />

issues and discussions are summarized into two primary areas, (1) Pilot Billet Inspection, and (2)<br />

Waspaloy Standard and discussed separately below.<br />

Nickel Billet Pilot Inspection<br />

A request was <strong>for</strong>warded to a production facility to bid on the multizone inspection of 75,000 lbs. of<br />

Inconel and 25,000 lbs. of Waspaloy. The ETC will purchase the multizone inspection of this 10-<br />

inch diameter material calibrating on the Nickel standards developed earlier. During this pilot<br />

program the ETC will purchase a select number of indications found with multizone with preference<br />

given to those that were not rejected with conventional inspection and per<strong>for</strong>m ultrasonic and<br />

metallographic characterization <strong>for</strong> POD studies and future inspection implementation decisions.<br />

As soon as the purchase order is in place the Inconel standard will be sent to the production site.<br />

Waspaloy Standard<br />

At the laboratory demonstration last quarter, the Waspaloy standard was found to have some<br />

surface irregularities that prompted a more detailed investigation. Surface metrology data revealed<br />

a periodic surface irregularity with amplitude of about 5 mils and consisting of 27 cycles around the<br />

circumference of the standard. Figure 1 shows the surface metrology data taken with a dial<br />

indicator around the circumference. The two major lobes are a result of the axial split line running<br />

through the center of the standard and were expected in the measurement.<br />

To evaluate the ultrasonic impact of this surface condition, a zone 5 transducer was used to create<br />

a C-scan of the machined surface on the interior of the billet standard. Figure 2 shows these<br />

surfaces highlighted in red. The resultant C-scan in Figure 3 shows the significant amplitude<br />

variation on the inner backwall caused by the surface irregularities.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Under normal circumstances one would expect the C-scan image to show fairly uni<strong>for</strong>m amplitude<br />

around the circumference indicating that the sound intensity was consistent. The fluctuating<br />

intensity seen on the C-scan is at the same frequency as the surface irregularities.<br />

ISU also modeled the effects of the surface on the ultrasonic signal and produced the graph in<br />

Figure 4. This study convinced the team to pursue having the Waspaloy standard machined or<br />

polished to remove the surface condition prior to using at the production site.<br />

Waspaloy Std. Surface Profile<br />

50<br />

Mils (1/1000 inch)<br />

40<br />

30<br />

20<br />

10<br />

0<br />

-10<br />

0 100 200 300 400<br />

Degrees<br />

Figure 1. Surface Profile of Waspaloy Standard 27 peaks and valleys.<br />

Figure 2. Diagram of Waspaloy standard highlighting inspection surface in red.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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3.15” 3.6”<br />

4.05”<br />

circumference<br />

axial<br />

Zone 5 transducer gated on FBH backwall<br />

Figure 3. Ultrasonic C-scan of Inner Backwall.<br />

Signal <strong>for</strong><br />

Smooth Surface<br />

Figure 4. ISU model of signal strength in focal zone due to surface condition.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Plans (April 1, 2002 – June 30, 2002):<br />

Begin inspection of Inconel and Waspaloy billet with Multizone as part of the pilot lot.<br />

Start metallographic sectioning of indications identified in the pilot inspection.<br />

Milestones:<br />

Original<br />

Date<br />

Revised<br />

Date<br />

Description<br />

Nickel billet inspection development<br />

3 months Kickoff meeting to verify selection of materials and<br />

target sensitivities, initiate design of calibration<br />

standards and establish metrics <strong>for</strong> cost and<br />

sensitivity assessment. Coordination with<br />

Inspection Systems Capability Working Group will<br />

occur to ensure necessary data <strong>for</strong> later POD<br />

studies. (All)<br />

24 months Assessment of sensitivity <strong>for</strong> small diameter billet.<br />

Data to be provided to Task 3.1 to enable POD<br />

assessment. (HW)<br />

24 months Complete modeling and laboratory testing of<br />

existing transducers on calibration standards <strong>for</strong><br />

INCO718 and assess need <strong>for</strong> new transducers.<br />

(GE, ISU).<br />

24 months Complete modeling and laboratory testing of<br />

existing transducers on calibration standards <strong>for</strong><br />

Waspaloy and assess need <strong>for</strong> new transducers.<br />

(PW, ISU)<br />

Status<br />

Complete<br />

Complete<br />

18 months Complete calibration standards. (GE, PW) Complete<br />

22 months Assessment of conventional inspections <strong>for</strong><br />

baseline. (GE, PW). Data to be provided to Task<br />

3.1 to enable POD assessment. (All)<br />

24 months 30 months Complete logistics of pilot lot inspection including<br />

establishing agreements with multizone inspection<br />

source and billet suppliers and establishing means<br />

of acquiring necessary cost data. (GE, PW)<br />

30 months Per<strong>for</strong>m laboratory demonstration <strong>for</strong> ETC<br />

members. (GE, PW)<br />

36 months Complete factory evaluation of approximately<br />

100,000 pounds of billet. Per<strong>for</strong>m demonstration<br />

<strong>for</strong> OEMs and industry at inspection facility. (GE,<br />

PW, ISU)<br />

38 months Evaluate any finds to determine necessary size<br />

parameters <strong>for</strong> POD assessment. (GE, ISU, PW)<br />

42 months Complete cost comparison of higher sensitivity<br />

multiple zone inspection with conventional<br />

inspection. (GE, PW)<br />

55 months Complete final report including sensitivity and cost<br />

comparison assessments. (All)<br />

55 months Report of laboratory and factory evaluations<br />

including sensitivity data <strong>for</strong> use by the Inspection<br />

Systems Capability Working Group and cost<br />

assessments. Calibration standards and fixed focus<br />

transducers.<br />

Complete – new transducers not<br />

needed to meet program goal<br />

Complete – new transducers not<br />

needed to meet program goal<br />

Complete<br />

PIA is in place. Logistics planning is<br />

proceeding<br />

Complete<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Original<br />

Date<br />

Revised<br />

Date<br />

Description<br />

60 months Calibration standards and fixed focus transducers<br />

(if fabricated).<br />

Status<br />

Deliverables:<br />

Laboratory demonstration and factory evaluation of multizone inspection including supplier<br />

demonstration.<br />

Report of laboratory and factory evaluations including sensitivity data <strong>for</strong> use by the Inspection<br />

Systems Capability Working Group and cost assessments.<br />

Calibration standards and fixed focus transducers.<br />

Metrics:<br />

Demonstration of #1FBH sensitivity inspection <strong>for</strong> INCO718 billet up to 10” diameter and #2.5FBH<br />

sensitivity <strong>for</strong> Waspaloy up to 10” diameter.<br />

Factory demonstration will include target of 90 cubic inches per minute scanning rate <strong>for</strong> multizone<br />

inspection.<br />

Major Accomplishments and Significant Interactions:<br />

Date<br />

June 16, 1999<br />

Description<br />

Technical Kick-off Meeting in West Palm Beach, FL<br />

Publications and Presentations:<br />

Date<br />

Description<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Project 1:<br />

Task 1.2:<br />

Subtask 1.2.1:<br />

Production Inspection<br />

<strong>Titanium</strong> Billet Inspection<br />

Inspection Development <strong>for</strong><br />

<strong>Titanium</strong> Billet<br />

Team Members:<br />

HW: Andy Kinney, Waled Hassan<br />

ISU: Bruce Thompson, Ron Roberts, Frank<br />

Margetan<br />

GE: Dave Copley, Wei Li, Mike Keller, Jon<br />

Bartos, Richard Klaassen, John Halase<br />

PW: Kevin Smith, Jeff Umbach, Bob<br />

Goodwin, Andrei Degtyar, Harpreet Wasan<br />

Students: none<br />

Program initiation date: June 15, 1999<br />

Objectives:<br />

• To provide a procedure to account <strong>for</strong> attenuation effects such that the variation between<br />

calibration and inspection sensitivity is minimized.<br />

• To demonstrate the ultrasonic equipment and techniques required to inspect titanium alloy<br />

billets to #1FBH sensitivity <strong>for</strong> 10” diameter and below.<br />

• To provide an initial assessment of sensitivity at diameters greater that 10”.<br />

Approach:<br />

Transducer Design Models: The design models will be reevaluated in detail to determine reasons<br />

<strong>for</strong> discrepancies between predicted and measured transducer behavior observed during Phase I<br />

work. This reevaluation will focus initially on assessing how well the input parameters used <strong>for</strong> the<br />

models represent the physical behavior of the transducers. It is planned to begin with<br />

characterization of piezo-electric elements prior to the addition of backing materials, and then<br />

attempt to compare model predictions with experiment at subsequent stages of the manufacturing<br />

process. This will involve working closely with a transducer manufacturer with one potential source<br />

identified. Based on this exercise, modifications will be made to model input parameters or to the<br />

model code to improve the prediction accuracy. Attention will also be paid to selection of<br />

transducer materials with consistent and measurable properties, <strong>for</strong> example the machining of<br />

lenses from solid material rather than using cast-in-place epoxy. Results will be shared with<br />

transducer manufacturers to allow improvements in future products both <strong>for</strong> ETC and the broader<br />

ultrasonic transducer user community.<br />

Inspection of 10” Diameter Billet: Fixed focus inspection will be the primary technique in this task.<br />

If this approach proves inadequate to meet program objectives, viable phased array technologies<br />

will be reviewed to select a candidate technique with the most potential <strong>for</strong> meeting the program<br />

objectives in consultation with the FAA.<br />

Improved fixed focus transducers <strong>for</strong> 10” diameter billet will be designed. Results from Phase I<br />

measurements (at 2.25” and 4.05” depths) will be used to identify the best combination of focal spot<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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diameter and frequency, and this in<strong>for</strong>mation will be used to design the complete set of<br />

transducers. 1 Phase I work indicates that frequency and bandwidth should be increased from those<br />

of the current production transducers which are 5MHz frequency and approximately 50%<br />

bandwidth. Two sets of the improved-design transducers will be purchased. A distance-amplitude<br />

correction (DAC) capability <strong>for</strong> the multizone instrumentation is being developed external to the<br />

ETC program with details to be shared with the ETC. This is expected to improve sensitivity by 1 or<br />

2 dB by ameliorating the current situation where high noise in the focal plane of the transducer<br />

limits sensitivity at the near and far ends of the depth-of-field.<br />

Laboratory Demonstration on 10” Diameter Billet: Scans will be per<strong>for</strong>med on the ETC 10”<br />

diameter standards using the above transducers, and with DAC capability added to current<br />

multizone instrumentation. Work will be per<strong>for</strong>med at GE QTC, with support provided to other<br />

<strong>Consortium</strong> members to participate in the measurements. The FBH amplitudes, noise levels, and<br />

FBH signal-to-noise ratios will be evaluated and compared with measurements made on production<br />

5MHz transducers during Phase I. A determination will be made of whether sensitivity level meets<br />

the #1FBH goal in all regions of the billet. Results will be provided to 3.1.1 <strong>for</strong> incorporation in the<br />

modeling and reliability ef<strong>for</strong>ts.<br />

Honeywell will also per<strong>for</strong>m a sensitivity assessment on smaller diameter billets using billets of


system will be at GE, and evaluation of any other systems would be at a location to be agreed upon<br />

by the technical team. Arrangements will be made to accommodate full team participation <strong>for</strong> all of<br />

these evaluations. The laboratory scan results will be reviewed to identify a preferred configuration<br />

<strong>for</strong> factory demonstration and potential implementation. The review will consider inspection<br />

per<strong>for</strong>mance, equipment cost and complexity, operating speed, and other implementation factors.<br />

A hybrid system using fixed focus <strong>for</strong> the outer zones and phased array <strong>for</strong> the center will be<br />

considered as part of this evaluation.<br />

If the final approach agreed to by the technical team <strong>for</strong> factory demonstration includes phased<br />

arrays, additional work will be done to refine the sensor design <strong>for</strong> the selected array approach.<br />

Manufacturer’s engineering specifications <strong>for</strong> the array system design (element geometry,<br />

lens/mirror geometry, etc.) will be input into an array system computational simulation. Theoretical<br />

system per<strong>for</strong>mance will be compared to laboratory measurements of array system response.<br />

Discrepancies between model and experiment will be traced to underlying causes and resolved.<br />

Models will then be used to optimize the design and set up <strong>for</strong> specific test standards targeted <strong>for</strong><br />

study including larger diameter billets.<br />

Factory <strong>Evaluation</strong>: The multizone configuration will be used to per<strong>for</strong>m factory evaluation of five<br />

heats of 10” diameter titanium at a production inspection facility. Cost and detection sensitivity<br />

assessments necessary <strong>for</strong> life management and implementation decisions will be gathered.<br />

Components of cost assessment will include such items as system cost, longevity of equipment,<br />

recurring equipment costs, daily operational/inspection costs, and costs associated with false calls.<br />

<strong>Evaluation</strong> will include cut-ups of any finds. Details of metallography will depend on how many<br />

indications are found, but it is anticipated that all finds will be evaluated to determine cause, and<br />

one will be step-polished to obtain detailed sizing in<strong>for</strong>mation.<br />

Factory Demonstration: An industry-wide demonstration of the multizone system will be scheduled.<br />

OEMs and titanium billet producers will be invited.<br />

Assessment of Large Diameter Billet (>10” dia): Assessment of the sensitivity at larger diameters<br />

will use 13” and 14” diameter standards. Existing 13” standards will be used, and a 14” chord block<br />

standard with near-centerline targets will be designed and built. Initial assessment will be made to<br />

baseline conventional inspection sensitivity either using transducers borrowed from suppliers, or by<br />

requesting suppliers to per<strong>for</strong>m the evaluation in-house. <strong>Evaluation</strong> of zoned fixed-focus capability<br />

will use existing multizone transducers. <strong>Evaluation</strong> will follow a plan to be agreed by consortium<br />

members. If the targeted 4x sensitivity improvement over conventional inspection has been<br />

achieved <strong>for</strong> 13” and 14” diameters, the results will be documented and no further work pursued. If<br />

improvement is still needed, a plan will be <strong>for</strong>mulated following the best approaches (phased array<br />

or improved fixed focus) identified <strong>for</strong> 10” diameter billet. The plan will be presented to the FAA as<br />

continued work is expected to require funding redirection.<br />

Attenuation Compensation Procedures: The current procedures used to measure and compensate<br />

<strong>for</strong> material attenuation will be evaluated and improved. The current procedure <strong>for</strong> the multizone<br />

inspection uses a pre-inspection of four short sections (1” long) of the billet to obtain an average<br />

backwall echo amplitude. This is compared with an average backwall amplitude measured on the<br />

calibration standard and the difference is used to calculate an attenuation compensation factor in<br />

decibels per inch. A transducer focused at the billet center is used to make the measurements.<br />

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The drawback of this method is that it ignores the effects of distortion of the ultrasonic beam during<br />

propagation through the metal microstructure. Phase I work has shown that beam distortion can be<br />

a major contributor to the response from flaws and backwalls. Even when beam distortion effects<br />

are minor and energy loss dominates, the material attenuation is found to vary significantly with<br />

position in a given billet in conjunction with noise banding as was shown in Figure 6. The effects of<br />

noise banding and nonuni<strong>for</strong>m attenuation can lead to an incorrect measurement of flaw response,<br />

and a true inspection sensitivity different from that assumed from calibration. The current<br />

attenuation compensation technique will be evaluated by applying it to several billet segments, then<br />

drilling a number of flat-bottom or side-drilled holes into the sections, and comparing the measured<br />

amplitudes of those holes to those expected from the attenuation analysis. Improvements will focus<br />

on selection of a transducer which will minimize the effects of beam distortion and provide an<br />

attenuation estimate which enables good prediction of the hole echo amplitudes.<br />

Billet Specification: The specification <strong>for</strong> billet inspection (AMS 2628) will be updated to reflect<br />

improvements achieved by this subtask. Results will also be reported in required FAA <strong>for</strong>mat.<br />

Objective/Approach Amendments: Objective and approach remain as originally proposed in July<br />

1998.<br />

Progress (January 1, 2002 – March 31, 2002):<br />

Several consortium conference calls were conducted during the quarter to discuss the details of the<br />

subtask. A number of technical issues were discussed and decisions reached. The technical<br />

issues and discussions are summarized into three primary areas, (1) Attenuation-Compensation,<br />

(2) 10” Billet Transducers and (3) 14” Chord Block Transducer and discussed separately below.<br />

One goal of Subtask 1.2.1 is to critically examine existing methods <strong>for</strong> attenuation compensation<br />

during billet inspection, and, if necessary, recommend improvements. Existing methods typically<br />

use the average strengths of back-wall echoes to estimate the attenuation difference between a<br />

billet under inspection and a calibration standard. During the Jan-Mar quarter, a series of<br />

experiments were per<strong>for</strong>med to determine how well back-wall (BW) amplitude variations mirror the<br />

amplitude variations <strong>for</strong> an array of nominally-identical small internal defects. The measurements<br />

were carried out at GEAE and Honeywell, and results were analyzed at ISU.<br />

A 15”-long section of 6"-diameter Ti 6-4 billet was obtained which displayed large variations in BW<br />

amplitude during scanning. These variations presumably arise from differences in the local<br />

"effective" attenuation of the billet, with both energy loss and microstructure-induced beam<br />

distortion effects contributing to that attenuation. A series of #4 FBHs were drilled 0.3” deep into<br />

the OD of the billet, some at locations having large BW amplitudes, and others at locations having<br />

small BW amplitudes. The billet section was then inspected using several transducers (with<br />

different beam sizes at the back wall) to determine the degree of correlation between the FBH<br />

amplitudes and the nearby BW amplitudes. Initial measurements at GEAE used two 5-MHz fixedfocused<br />

transducers: (1) a multizone probe designed to focus near the center of 6"-diameter billet<br />

when operated at a 3” water path; and (2) a multizone probe designed to focus near the center of<br />

13" billet, with the water path modified to 6.6” so as to best focus the beam near the BW of the 6"<br />

billet under study. Additional inspections were made at Honeywell using a 114-element, 5-MHz,<br />

phased-array transducer. The array transducer was used to simulate inspections <strong>for</strong> two other<br />

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fixed-focus transducers that were not readily available. We note that 6"-diameter billet was chosen<br />

<strong>for</strong> these initial experiments because existing transducers were available which could approximately<br />

focus a sound beam near the back wall in such a billet (one of the focal conditions of chief interest).<br />

#4 FBHs were then chosen to simulate internal defects, because such targets were large enough to<br />

be easily seen <strong>for</strong> the range of focal conditions being investigated.<br />

C-scan images <strong>for</strong> four measurement trials are shown in the upper panels of Figures 1-4,<br />

respectively. The upper-left panel of each figure shows the rectified peak amplitude of the BW<br />

echo as a function of position <strong>for</strong> a full-round inspection of the 15”-long billet section. The upperright<br />

panel displays images of the FBHs, obtained by per<strong>for</strong>ming a second scan at increased gain,<br />

using a time gate that enclosed the FBH echoes, but excluded the BW echoes. Annotations on the<br />

upper panels list the peak FBH amplitudes and the average BW amplitudes in small regions<br />

centered about each FBH location. In all cases, the listed amplitudes are the percentage of Full<br />

Screen Height (FSH). One notices in each figure that the BW and FBH both amplitudes vary<br />

considerably, and that large (small) FBH amplitudes are usually associated with large (small) BW<br />

amplitudes at similar positions.<br />

The correlation between FBH and BW amplitudes is further illustrated in the lower panels of Figures<br />

1-4. For each of the four inspections, the absolute amplitudes of the BW and FBH signals have<br />

been adjusted to have a mean value of 50% FSH <strong>for</strong> the suite of FBH targets. These rescaled<br />

amplitudes are shown in the lower-left panel, with the principal FBH targets numbered 1-13 (from<br />

top to bottom and left to right in the C-scan images). The lower-right panels display "correlation<br />

plots" of the rescaled FBH amplitudes versus the rescaled BW amplitudes. If there were perfect<br />

correlation between the two types of echoes, the plotted points would all fall along a straight line<br />

passing through the origin and having a slope of unity. In each case, a best-fit line through the<br />

origin is shown, and its slope is seen to be close to the ideal value of 1 in each case. Overall, the<br />

BW and FBH amplitudes were found to be generally well correlated, with the degree of correlation<br />

being largest when the beam was focused near the FBH targets.<br />

The results summarized in Figures 1-4 indicate that BW echoes can be used to track attenuation<br />

variations within a billet. Presumably, BW echoes can also be used to ascertain the attenuation<br />

difference between a billet under inspection and a calibration standard. Because of the significant<br />

variation in BW and FBH amplitudes with billet position, the results suggest that attenuation<br />

compensation procedures should make use of extreme BW amplitude data values rather than only<br />

average values.<br />

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Back-Wall Scan<br />

FBH scan<br />

20%<br />

39%<br />

61%<br />

51%<br />

59%<br />

47%<br />

65% 64%<br />

20%<br />

7%<br />

23%<br />

20%<br />

47%<br />

49%<br />

93%<br />

80%<br />

75%<br />

55%<br />

68%<br />

34%<br />

38%<br />

30%<br />

73%<br />

59%<br />

13%<br />

22% 12%<br />

66%<br />

65%<br />

24%<br />

21%<br />

(a)<br />

(b)<br />

68%<br />

Amplitude (%FSH)<br />

(c)<br />

Comparison of Normalized<br />

BW and FBH variations<br />

(6" Multizone Probe)<br />

100<br />

BW 6"MZ<br />

90<br />

FBH 6"MZ<br />

80<br />

70<br />

60<br />

50<br />

40<br />

30<br />

20<br />

10<br />

Average <strong>for</strong> all sites = 50%<br />

0<br />

0 1 2 3 4 5 6 7 8 9 10 11 12 13 14<br />

Measurement Site<br />

FBH Amplitude (% FSH)<br />

(d)<br />

Correlation Between Norm'ed<br />

BW and FBH variations<br />

(6" Multizone Probe)<br />

100<br />

90<br />

y = 1.0243x<br />

80<br />

R 2 = 0.565<br />

70<br />

60<br />

50<br />

Trendline thru origin<br />

40<br />

30<br />

20<br />

10<br />

0<br />

0 10 20 30 40 50 60 70 80 90 100<br />

BW Amplitude (% FSH)<br />

Figure 1. Measurements on a Ti 6-4 billet segment using a 5-MHz 6”-multizone probe focused near<br />

the billet center. (a) C-scan of back-wall amplitude. (b) C-scan gated on FBH targets drilled into the<br />

billet OD. (c) Scaled BW and FBH amplitudes. (d) Correlation between BW and FBH amplitudes.<br />

Beam diameters (-6 dB) near the back wall are approximately 250 mils x 610 mils (axial x hoop).<br />

For panels (a) and (b), the horizontal direction is parallel to the billet axis.<br />

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Back-Wall Scan<br />

FBH scan<br />

20%<br />

57%<br />

49%<br />

48%<br />

48% 48%<br />

58% 59%<br />

22%<br />

13%<br />

18%<br />

20%<br />

28%<br />

31%<br />

79%<br />

64% 91%<br />

66% 94%<br />

27%<br />

31%<br />

42%<br />

79%<br />

82%<br />

33% 33%<br />

15%<br />

64% 70%<br />

22%<br />

19%<br />

(a)<br />

(b)<br />

87%<br />

Amplitude (%FSH)<br />

(c)<br />

Comparison of Normalized<br />

BW and FBH variations<br />

(13" Multizone Probe)<br />

90<br />

BW 13"MZ<br />

80<br />

FBH 13"MZ<br />

70<br />

60<br />

50<br />

40<br />

30<br />

20<br />

10<br />

Average <strong>for</strong> all sites = 50%<br />

0<br />

0 1 2 3 4 5 6 7 8 9 10 11 12 13 14<br />

Measurement Site<br />

FBH Amplitude (% FSH)<br />

(d)<br />

90<br />

80<br />

70<br />

60<br />

50<br />

40<br />

30<br />

20<br />

10<br />

0<br />

Correlation Between Norm'ed<br />

BW and FBH variations<br />

(13" Multizone Probe)<br />

y = 0.9909x<br />

R 2 = 0.6086<br />

Trendline thru origin<br />

0 10 20 30 40 50 60 70 80 90 100<br />

BW Amplitude (% FSH)<br />

Figure 2. Measurements on a Ti 6-4 billet segment using a 5-MHz 13”-multizone probe focused<br />

near the billet back wall, following the style of Figure 1. Beam diameters (-6 dB) near the back wall<br />

are approximately 150 mils x 540 mils (axial x hoop).<br />

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56%<br />

Back-Wall Scan<br />

84%<br />

FBH scan<br />

42%<br />

43%<br />

58%<br />

49%<br />

43%<br />

46%<br />

43%<br />

44%<br />

54%<br />

48%<br />

16%<br />

19%<br />

19%<br />

32%<br />

40%<br />

32%<br />

73%<br />

73%<br />

69%<br />

61%<br />

74%<br />

77%<br />

73%<br />

44%<br />

46%<br />

44%<br />

44%<br />

81%<br />

72%<br />

24%<br />

(a)<br />

(b)<br />

Comparison of Normalized<br />

BW and FBH variations<br />

(5-MHz Phased Array; Focused in Middle; Trial 2)<br />

Correlation Between Norm'ed<br />

BW and FBH variations<br />

(5-MHz Phased Array; Focused in Middle; Trial 2)<br />

80<br />

80<br />

Amplitude (%FSH)<br />

(c)<br />

70<br />

60<br />

50<br />

40<br />

30<br />

20<br />

BW PA-foc_middle<br />

10<br />

FBH PA-foc_middle<br />

Average <strong>for</strong> all sites = 50%<br />

0<br />

0 1 2 3 4 5 6 7 8 9 10 11 12 13 14<br />

Measurement Site<br />

FBH Amplitude (% FSH)<br />

70<br />

y = 1.0117x<br />

60<br />

R 2 = 0.6684<br />

50<br />

40<br />

30<br />

20<br />

10<br />

(d)<br />

0<br />

0 10 20 30 40 50 60 70 80 90 100<br />

BW Amplitude (% FSH)<br />

Trendline thru origin<br />

Figure 3. Measurements on a Ti 6-4 billet segment using a 5-MHz phased-array transducer<br />

focused near the billet center, following the style of Figure 1. Beam diameters (-6 dB) near the<br />

back wall are approximately 400 mils x 600 mils (axial x hoop).<br />

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63%<br />

Back-Wall Scan<br />

74%<br />

FBH scan<br />

58%<br />

40%<br />

64%<br />

60%<br />

59%<br />

57%<br />

42%<br />

61%<br />

68%<br />

47%<br />

33%<br />

37%<br />

35%<br />

37%<br />

57%<br />

56%<br />

64%<br />

71%<br />

68%<br />

55%<br />

69%<br />

66%<br />

64%<br />

48%<br />

49%<br />

46%<br />

38%<br />

66%<br />

66%<br />

36%<br />

(a)<br />

Amplitude (%FSH)<br />

(c)<br />

Comparison of Normalized<br />

BW and FBH variations<br />

(5-MHz Phased Array; Focused on Backwall; Trial 1)<br />

80<br />

70<br />

60<br />

50<br />

40<br />

30<br />

20<br />

10<br />

FBH PA-foc_at_back<br />

Average <strong>for</strong> all sites = 50%<br />

0<br />

0 1 2 3 4 5 6 7 8 9 10 11 12 13 14<br />

Measurement Site<br />

BW PA-foc_at_back<br />

FBH Amplitude (% FSH)<br />

(b)<br />

Correlation Between Norm'ed<br />

BW and FBH variations<br />

(5-MHz Phased Array; Focused on Backwall; Trial 1)<br />

80<br />

70<br />

y = 1.005x<br />

R 2 60<br />

= 0.7744<br />

50<br />

40<br />

30<br />

(d)<br />

Trendline thru origin<br />

20<br />

10<br />

0<br />

0 10 20 30 40 50 60 70 80 90 100<br />

BW Amplitude (% FSH)<br />

Figure 4. Measurements on a Ti 6-4 billet segment using a 5-MHz phased-array transducer<br />

focused near the billet back wall, following the style of Figure 1. Beam diameters (-6 dB) near the<br />

back wall are approximately 200 mils x 380 mils (axial x hoop).<br />

<strong>Evaluation</strong> of Transducers<br />

The two 7.5 MHzF/10 aperture elliptical transducers were evaluated in more detail than the<br />

preliminary evaluation reported in the previous quarterly. Frequency measurements were made<br />

using the echoes from #2FBH targets in 10” diameter calibration standards. Tables 1 and 2<br />

compares these frequency measurements with those supplied by the manufacturer, which had<br />

been measured on a flat brass target, located at the near focal point, in water.<br />

In order to assess the per<strong>for</strong>mance relative to the #1FBH sensitivity program goal, a number of<br />

scans were made using the 10 inch diameter Ti 64 ETC standards, which contain targets of various<br />

diameters down to 0.4 mm (1/64 inch). These scans were done as closely as possible to<br />

production inspection conditions, with the exceptions that the scan index was reduced to 0.01” in<br />

order to capture the peak signals, and the gate length was reduced where necessary to avoid back<br />

surface signals in the gate. For the zone 2 transducer, targets at 0.9”, 1.35” and 1.8” (start, center,<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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and end of zone) were analyzed from the c-scan data. For the zone 4 transducer, targets were at<br />

3.15”, 3.6” (center and end of zone). In each case, there was some lateral banding of the noise<br />

pattern, so regions of noise in the highest and lowest bands were analyzed and are shown<br />

separately on the plots. Figures 5 and 6 show the target amplitudes and noise amplitudes <strong>for</strong><br />

zones 2 and 4 that the zone 4 transducer was not capable of per<strong>for</strong>ming inspection of the material<br />

in the calibration standard to a 1/64 inch FBH sensitivity. The noise level in the high noise band<br />

was marginally above the amplitude of the 0.4 mm (1/64 inch) target at the deep end of the zone.<br />

We consider that a 3dB margin is required between the noise and the target amplitude in order to<br />

achieve the inspection sensitivity. Review of the measured frequency per<strong>for</strong>mance, and the<br />

manufacturer’s reported measurements also showed that the transducer had frequency significantly<br />

lower than specified (measured at 6.02, 6.25, and 6.35 MHz, versus lower specification limit of 7.0<br />

MHz). The transducer was returned to the manufacturer.<br />

The zone 2-transducer appeared marginally capable of meeting the required sensitivity. It showed<br />

a difference of 2.8 dB between the noise and the lowest target signal, versus the 3dB requirement.<br />

There is a concern that the measured bandwidth was lower than specified (48% versus lower spec<br />

limit of 60%), and the manufacturers reported measurement of frequency was only 6.33 MHz.<br />

Based on the data of Figures 5 and 6, a decision was made to pursue development of transducers<br />

designed with the larger F/8 aperture. Note that the original plan was to purchase sets of<br />

transducers with both F/10 and F/8 aperture size. The smaller F/10 transducers reported above<br />

were purchased with the intent of making the final decision on aperture size based on the results of<br />

their evaluation.<br />

Figure 5. Noise and target amplitude responses, zone 2 transducer.<br />

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Figure 6. Noise and target amplitude responses, zone 4 transducer.<br />

Specified<br />

Reported by<br />

manufacturer<br />

Measured on #2FBH, 1.35”<br />

deep in Inconel 718<br />

<strong>Center</strong> freq (MHz) 7.5 ± 0.5 6.33 7.1<br />

Lower – 6 dB freq (MHz) 5.4<br />

Upper – 6 dB freq (MHz) 8.8<br />

Bandwidth (MHz) 3.4<br />

Bandwidth (%) ≥ 60 68 48<br />

Pulse duration (µS) 0.21<br />

Table 1. Frequency Measurements <strong>for</strong> Zone 2 Transducer.<br />

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Specified<br />

Reported by<br />

manufacturer<br />

Measured on<br />

2/64 inch<br />

FBH, 3.15”<br />

deep in<br />

Inconel 718<br />

Measured on<br />

2/64 inch<br />

FBH, 3.15”<br />

deep in Ti 64<br />

<strong>Center</strong> freq (MHz) 7.5 ± 0.5 6.02 6.35 6.25<br />

Lower – 6 dB freq (MHz) 4.9 4.7<br />

Upper – 6 dB freq (MHz) 7.8 7.8<br />

Bandwidth (MHz) 2.9 3.1<br />

Bandwidth (%) ≥ 60 72 46 50<br />

Pulse duration (µS) 0.25 0.31<br />

Table 2. Frequency Measurements <strong>for</strong> Zone 4 Transducer.<br />

Plans (April 1, 2002 – June 30, 2002):<br />

Detailed straw-man <strong>for</strong> an improved compensation procedure will be developed, and plans <strong>for</strong> a<br />

direct test of the new procedure will be <strong>for</strong>mulated.<br />

Continue with purchase of F/8 aperture transducers.<br />

Utilize phased array to simulate the per<strong>for</strong>mance of the F/8 aperture and verify that the beam<br />

properties produced will achieve the required sensitivity<br />

Milestones:<br />

Original<br />

Date<br />

Revised<br />

Date<br />

Description<br />

10” diameter fixed focus<br />

12 months 18 months Resolve model discrepancies and design<br />

transducers. (ISU)<br />

Status<br />

Model discrepancies resolved—<br />

design activity initiated. Delay will<br />

not affect remainder of program<br />

7 months 36 months Build transducers. (GE) Zones 2 and 4 transducers received.<br />

First two transducers took longer to<br />

build than anticipated causing<br />

milestone slip. Ready to order<br />

complete set.<br />

29 months 38 months Complete scans on 10” standards and RDB.<br />

Provide data to 3.1.1 <strong>for</strong> estimation of POD.<br />

(GE,PW)<br />

30 months 39 months Review results, determine whether #1FBH goal<br />

was achieved. (All)<br />

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Original<br />

Date<br />

Revised<br />

Date<br />

Description<br />

Status<br />

34 months Design and build two transducers <strong>for</strong> 14” diameter<br />

center zone. Evaluate per<strong>for</strong>mance on 14” chord<br />

block. (PW with support from GE)<br />

(30<br />

months)<br />

(33<br />

months)<br />

(39<br />

months)<br />

(42<br />

months)<br />

(48<br />

months)<br />

10” diameter phased array,(go/no go decision<br />

at 30 months)<br />

(Critical review with FAA, seek program redirection<br />

to develop phased arrays) (All)<br />

Complete preliminary phased array surveys. (PW)<br />

Evaluate up to three candidate phased array<br />

systems.<br />

Identify preferred configuration <strong>for</strong> factory<br />

evaluation system.<br />

Design and build improved phased array<br />

transducer assembly.<br />

Factory <strong>Evaluation</strong> / Demonstration<br />

36 months* 44 months Complete factory test of five heats. Conduct<br />

industry demonstration of #1FBH capability in 10”<br />

diameter. (GE, PW)<br />

38 months* 46 months Evaluate indication finds from factory test,<br />

document results. (GE, PW, ISU).<br />

40 months 48 months Report of laboratory and factory evaluations<br />

including sensitivity data <strong>for</strong> use by the Inspection<br />

Systems Capability Working Group and cost<br />

comparisons <strong>for</strong> the different inspection<br />

approaches. (All)<br />

Large diameter billet<br />

12 months Build chord calibration standard <strong>for</strong> 14” diameter,<br />

near-center region. (PW)<br />

18 months 20 months Evaluate capability on 13” and 14” diameter using<br />

conventional and zoned fixed focus, determine<br />

improvement over conventional. Provide data to<br />

3.1.1 <strong>for</strong> model validation and POD estimation <strong>for</strong><br />

large diameter billet. (GE, PW, ISU)<br />

20 months 24 months Laboratory assessment of sensitivity at diameters<br />

greater than 10" diameter using fixed focus<br />

transducers. (All)<br />

General issues<br />

28 months Complete attenuation compensation procedure in<br />

cooperation with 3.1.1. (ISU with support from PW<br />

and GE)<br />

30 months Procedures to account <strong>for</strong> attenuation effects that<br />

occur in titanium billet and thus improve the POD of<br />

billet inspection. (All)<br />

Original<br />

Date<br />

Revised<br />

Date<br />

Description<br />

Transducer order has been placed.<br />

Complete<br />

13” billet inspection complete at GE<br />

14” chord block inspection complete<br />

Complete at P&W<br />

Status<br />

60 months Provide revision of AMS 2628 titanium billet<br />

specification to SAE Committee K.<br />

60 months Calibration standards including 14" diameter chord<br />

block and transducers (fixed focus and phased<br />

array assemblies) as needed.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 32


Deliverables:<br />

Laboratory assessment of sensitivity at diameters greater than 10” diameter using fixed focus<br />

transducers.<br />

Procedures to account <strong>for</strong> attenuation effects that occur in titanium billet and thus improve the POD<br />

of billet inspection.<br />

Report of laboratory and factory evaluations including sensitivity data <strong>for</strong> use by the Inspection<br />

Systems Capability Working Group and cost comparisons <strong>for</strong> the different inspection approaches.<br />

Calibration standards including 14” diameter chord block and transducers (fixed focus and phased<br />

array assemblies) as needed.<br />

Revision to AMS 2628 titanium billet specification submitted to SAS Committee K.<br />

Metrics:<br />

Achievement of #1FBH in 10” diameter billet with no significant speed reduction from current<br />

multizone inspection.<br />

Major Accomplishments and Significant Interactions:<br />

Date<br />

June 16, 1999<br />

Description<br />

Technical Kick-off Meeting in West Palm Beach, FL<br />

Publications and Presentations:<br />

Date<br />

Description<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 33


Project 1:<br />

Task 1.3:<br />

Subtask 1.3.1:<br />

Production Inspection<br />

<strong>Titanium</strong> Forging Inspection<br />

Fundamental Property<br />

Measurements <strong>for</strong> <strong>Titanium</strong><br />

Forgings<br />

Team Members:<br />

HW: R. Bellows, Waled Hassan<br />

ISU: Bruce Thompson, Frank Margetan,<br />

Ron Roberts, Tim Gray<br />

GE: Ed Nieters, Mike Gigliotti, Lee<br />

Perocchi, Dave Copley, Wei Li, Jon Bartos,<br />

Bill Leach<br />

PW: Jeff Umbach, Bob Goodwin, Andrei<br />

Degtyar, Harpreet Wasan<br />

Students: A. Li<br />

Program initiation date: June 15, 1999<br />

Objectives:<br />

• To gain the fundamental understanding of the ultrasonic properties of titanium <strong>for</strong>gings that is<br />

needed to provide a foundation <strong>for</strong> the development of reliable inspection methods that provide<br />

uni<strong>for</strong>mly high sensitivity throughout the <strong>for</strong>ging envelope.<br />

• To acquire the data necessary to relate the detectability of defects in <strong>for</strong>gings to component<br />

properties (flow line characteristics, surface curvature) and defect properties (size, shape,<br />

composition, location, and orientation) thereby providing a foundation <strong>for</strong> the design of<br />

improved inspections and the evaluation of inspection capability.<br />

Approach:<br />

Sample Fabrication: A critical flaw list <strong>for</strong> titanium <strong>for</strong>gings will be generated in cooperation with<br />

RISC including description of typical morphologies <strong>for</strong> use in the model development ef<strong>for</strong>ts.<br />

This list will be used to define a limited set of <strong>for</strong>ging standards with embedded defects.<br />

Forging samples with varying flow line characteristics and surface curvatures, some of which will<br />

contain flat-bottomed holes or synthetic inclusions will be defined and manufactured.<br />

De<strong>for</strong>mation models will be used to predict variations in metal flow distributions and guide the<br />

sample development. Approximately 32 coupons from <strong>for</strong>gings with varying flow line directions,<br />

flow line densities, and geometrical curvatures (concave and convex) will be acquired. Samples<br />

available from the CBS and TRMD programs will be utilized to the extent possible.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Ultrasonic Property Measurement: UT and material anisotropy associated with the <strong>for</strong>ging process<br />

will be quantified by measurement of the sound speeds, attenuations, signal fluctuations and<br />

backscattered noise levels of the <strong>for</strong>ging coupons. The measurement methods developed in Phase<br />

I will generally be used. As in Phase I, cube specimens cut at various locations may be used <strong>for</strong><br />

initial surveys. In selected cases, novel coupon geometries will also be considered which permit<br />

beam propagation at various angles to the flow lines. Figure 2 displays one possible coupon<br />

design which allows measurements: (1) along flow lines; (2) perpendicular to flow lines; and (3) at<br />

oblique incidence. Such measurements will be used to establish the relationship of flow line<br />

direction to inspectability. The results of the experimental measurements will be used to develop<br />

and validate the noise models and ultimately allow consideration of the effect of <strong>for</strong>ging process on<br />

inspection capability as part of 3.1.2.<br />

Measurements will be made of the<br />

ultrasonic scattering from the embedded<br />

defects, including both the synthetic hard<br />

alpha inclusions and the samples available<br />

from the CBS and TRMD programs. This<br />

data will be provided <strong>for</strong> further model<br />

validation which will in turn be utilized in<br />

subtasks 3.1.2 <strong>for</strong> POD determination.<br />

Effects of Surface Curvature: The<br />

relationship between surface curvature and<br />

inspectability will be quantified in this<br />

subtask. The shape of the entry surface<br />

influences the focusing of the sonic beam<br />

within the <strong>for</strong>ging, and hence, affects both<br />

the amplitude of defect echoes and the level<br />

of competing grain noise. The team will<br />

measure the effects of surface curvature by<br />

using coupon designs such as that shown in<br />

Figure 3. Curvature corrections will be<br />

developed and transducer designs will be<br />

optimized in cooperation with 1.3.2. Models<br />

which predict the effects of surface<br />

curvature on backscattered flaw echoes,<br />

grain noise characteristics, and signal/noise<br />

ratios will be developed and validated in<br />

cooperation with 3.1.2. Measurements<br />

made using the surface-curvature<br />

specimens will be used to validate those<br />

models. The models will then be used to<br />

develop curvature corrections and optimized<br />

transducer designs <strong>for</strong> <strong>for</strong>ging inspections in support of 1.3.2.<br />

Measurements<br />

parallel to<br />

flow lines<br />

FLOW LINES<br />

Oblique angle<br />

measurements<br />

Measurements<br />

perpendicular<br />

to flow lines<br />

Figure 2. Potential coupon design <strong>for</strong> <strong>for</strong>ging samples.<br />

Octagonal shape provides entry and reflecting surfaces <strong>for</strong><br />

velocity and attenuation measurements at various<br />

orientations to the <strong>for</strong>ging flow lines.<br />

Initial Shape<br />

FBH’s<br />

A<br />

B<br />

C<br />

D<br />

E<br />

Surface<br />

Progression<br />

- 2”<br />

- 4”<br />

flat<br />

4”<br />

2”<br />

Figure 3. Potential design <strong>for</strong> surface curvature test<br />

specimens. Specimen contains flat-bottomed holes or<br />

other reflectors, and begins with a concave surface<br />

curvature which is progressively machined to arrive at<br />

convex entry surface. Design ensures that metal travel<br />

path and microstructure surrounding the reflectors remain<br />

unchanged in successive measurements.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Objective/Approach Amendments: Objective and approach remain as originally proposed in July<br />

1998.<br />

Progress (January 1, 2002 – March 31, 2002):<br />

Several consortium conference calls were conducted during the quarter to discuss the details of the<br />

subtask. A number of technical issues were discussed and decisions reached. The technical<br />

issues and discussions are summarized into three primary areas, (1) Property Measurements, (2)<br />

Noise Curvature Blocks, and (3) Synthetic Inclusion Disk and discussed separately below.<br />

Property Measurements<br />

One goal of the Fundamental Studies subtask is to document the manner in which ultrasonic<br />

properties vary within representative Ti 6-4 <strong>for</strong>gings, and to relate those properties to the <strong>for</strong>ging<br />

microstructure. The ultrasonic data will then be used by Subtask 1.3.2 to design new <strong>for</strong>ging<br />

inspections which improve defect detection sensitivity four-fold: from the current #1 FBH level to a<br />

#1/2 FBH level. Since backscattered grain noise is primarily responsible <strong>for</strong> determining defect<br />

detection limits, the emphasis has been on grain noise measurement and analysis.<br />

The overall plan calls <strong>for</strong> UT measurements on coupons cut from selected sites in three typical Ti 6-<br />

4 <strong>for</strong>gings supplied by the OEMs. Approximately 8-10 coupons have now been cut from each<br />

<strong>for</strong>ging, with coupon sites chosen to provide a range of local microstructures (based on<br />

backscattered noise C-scan, macroetch, and strain-map data). In previous quarters, grain noise<br />

studies were concluded on suites of coupons cut from <strong>for</strong>ged disks provided by GE and P&W.<br />

During the Jan-Mar 2002 quarter, similar measurements were conducted on the coupons from the<br />

Honeywell (HW) <strong>for</strong>ging. The noise measurement and FBH normalization procedures were<br />

identical to those reported in the Jan-Mar 2001 Quarterly Report. The noise measurement setup is<br />

shown in Figure 1, together with the coupon sites <strong>for</strong> the HW <strong>for</strong>ging.<br />

Backscattered grain noise amplitudes <strong>for</strong> one case are shown in Figure 2. The noise C-scans <strong>for</strong><br />

the HW coupons generally showed little variation with position in the hoop direction; however in<br />

some cases there was a strong variation with inspection direction or with radial/axial position. As<br />

was done earlier, each coupon was divided into quadrants of approximately uni<strong>for</strong>m noise<br />

amplitude, and noise statistics <strong>for</strong> each quadrant were computed <strong>for</strong> the two inspection directions in<br />

the radial-axial plane. Gated-peak noise amplitudes were measured relative to an available #1<br />

FBH reference, namely a 0.5”-deep hole in an IN100 step block. ISU models were then used to<br />

rescale the noise data relative to a hypothetical #1 FBH in Ti 6-4 at the same average depth as the<br />

noise measurements. Resulting average and peak noise levels <strong>for</strong> the HW coupons are shown in<br />

Figure 3.<br />

Measured average and maximum gated-peak noise levels are compared <strong>for</strong> the three OEMsupplied<br />

<strong>for</strong>gings in Table 1. When averaged over all coupons and inspection directions, results <strong>for</strong><br />

the three <strong>for</strong>gings were quite similar. The largest peak noise level seen in all of the cases studied<br />

was 6.9% of the #1 FBH reference. This occurred within Honeywell coupon #5 which was located<br />

in the OD portion of the <strong>for</strong>ging, about midway between the “<strong>for</strong>ward” and “aft” surfaces.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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When designing UT inspections of <strong>for</strong>gings, the high-noise regions are of chief interest since the<br />

elevated grain noise levels there can mask echoes from small or weakly reflecting defects. For this<br />

reason, additional UT measurements were planned <strong>for</strong> the highest-noise coupon from each <strong>for</strong>ging.<br />

These included determination of the attenuation and the backscattered noise capacity (FOM), both<br />

of which are frequency-dependent. Such measurements had been per<strong>for</strong>med earlier <strong>for</strong> the highnoise<br />

GE and P&W coupons. During the Jan-Mar quarter, similar measurements were completed<br />

<strong>for</strong> the highest-noise coupon from the HW <strong>for</strong>ging, and results are summarized in Figures 4 and 5.<br />

Because the microstructure typically varies with depth, FOM values were deduced <strong>for</strong> a series of<br />

depths by using time gates with different centers and durations. Power law fits to the FOM-versusfrequency<br />

data were then made <strong>for</strong> the depth zone having the highest noise capacity. Table 2<br />

summarizes the pertinent UT properties <strong>for</strong> the highest-noise zones of the high-noise coupons from<br />

the GE, P&W, and HW <strong>for</strong>gings. As expected from Table 1, the measured FOM value was largest<br />

<strong>for</strong> the Honeywell high-noise coupon.<br />

Note that the differences in FOM values in Table 2 are greater than the corresponding differences<br />

in peak noise values listed in Table 1. This is chiefly because, in the survey measurements leading<br />

to Table 1, only gated-peak noise amplitudes were measured, and the focal spot of the transducer<br />

was not necessarily located in the depth zone where the noise capacity was greatest. For Table 2,<br />

however, noise A-scan data was analyzed in a manner that identified the depth zone with the<br />

greatest noise capacity.<br />

The properties listed in Table 1 can be used as inputs to computer models that simulate ultrasonic<br />

inspections of <strong>for</strong>gings. Examples of such simulations <strong>for</strong> one proposed inspection scheme can be<br />

found in an article written <strong>for</strong> the 2001 QNDE conference held in Brunswick, Maine: “Survey of<br />

Ultrasonic Properties of Aircraft <strong>Engine</strong> <strong>Titanium</strong> Forgings”, by L. Yu, F. J. Margetan, R. B.<br />

Thomson, and A. Degtyar.<br />

During the quarter, we continued ef<strong>for</strong>ts to relate the observed noise variations in the Ti 6-4 <strong>for</strong>ging<br />

coupons to available microstructural data. The latter includes <strong>for</strong>ging strain map in<strong>for</strong>mation as<br />

calculated using DEFORM. One display of the strain data <strong>for</strong> the Honeywell <strong>for</strong>ging is shown in<br />

Figure 6. It shows the manner in which ellipsoidal elements in the billet are de<strong>for</strong>med by the multistep<br />

<strong>for</strong>ging process. The billet elements were chosen to have 5:1 aspects ratios, with the long<br />

dimension aligned with the billet axis, to approximately simulate billet macrograins. Ef<strong>for</strong>ts to<br />

correlate absolute noise levels with properties of the de<strong>for</strong>med ellipsoids seen in Figure 6 were not<br />

very successful. However, a clear correlation was seen between the local ellipsoid properties and<br />

the local noise anisotropy. The noise anisotropy (NA) is defined as the ratio of the average gatedpeak<br />

noise values <strong>for</strong> C-scans made from two orthogonal directions. For coupons that are not<br />

“tilted” with respect to the symmetry axis of the <strong>for</strong>ging, the NA equals the “axial” noise level divided<br />

by the “radial” noise level. If the shapes of macrograins in the <strong>for</strong>ging mimic the shapes of the<br />

ellipsoidal elements output by the DEFORM calculation, then the noise anisotropy is expected to<br />

correlate with the ellipsoid projection ratio defined in the right-hand panel of Figure 6. For the<br />

Honeywell <strong>for</strong>ging, a positive correlation is seen between the NA and projection ratio (Figure 7).<br />

However, the degree of correlation is not as high as seen earlier <strong>for</strong> the P&W <strong>for</strong>ging. A similar<br />

study comparing noise anisotropy and ellipsoid de<strong>for</strong>mation is planned <strong>for</strong> the GE <strong>for</strong>ging if suitable<br />

DEFORM calculations can be obtained.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 37


(a)<br />

Transducer is:<br />

15 MHz<br />

0.5”-Diameter<br />

F = 3.5 in.<br />

0.0<br />

0.2<br />

0.4<br />

0.6<br />

0.8<br />

1.0 1.0<br />

Coupons measure<br />

1.25” x 1.25” x 2.0”.<br />

Each of the four<br />

large surfaces was<br />

scanned.<br />

Gated region <strong>for</strong><br />

C-scan images of<br />

gated peak noise.<br />

Relative inspection<br />

sensitivity with depth<br />

within gate.<br />

(Via noise models.)<br />

Focused 1/4 way down<br />

(b)<br />

ID<br />

9<br />

1.75”<br />

7.63”<br />

AFT<br />

1.25” / 2<br />

1<br />

3<br />

2<br />

10<br />

4<br />

5<br />

6<br />

7 8<br />

Sonic shape.<br />

FWD<br />

HW Ti 6-4 Forging<br />

OD<br />

Figure 1. (a) Setup <strong>for</strong> backscattered noise measurements on <strong>for</strong>ging coupons. (b): Coupon<br />

locations <strong>for</strong> the Honeywell <strong>for</strong>ging.<br />

(a)<br />

Side 2<br />

(AFT)<br />

Side 1<br />

Side 3<br />

(OD)<br />

(hoop)<br />

(c)<br />

ID<br />

(side 4)<br />

H#<br />

AFT<br />

(side 2)<br />

5<br />

6<br />

4<br />

1<br />

3 2<br />

8 7<br />

FWD<br />

(side 5)<br />

engraved<br />

label<br />

OD<br />

(side 1)<br />

0% 100%<br />

(b)<br />

Thru OD<br />

Tic marks<br />

are 0.5”<br />

apart<br />

Cropped<br />

region used<br />

<strong>for</strong> noise<br />

statistics<br />

Specimen,<br />

inspection<br />

direction<br />

and<br />

absolute<br />

gain<br />

setting.<br />

Side 2 - AFT<br />

(Side 3 – hoop)<br />

H3 Side 1, 37dB<br />

Side 5 - FWD<br />

Avg.: 2.58% 2.13% 3.03%<br />

Peak: 10.4% 6.11% 10.4%<br />

Full<br />

image<br />

Left<br />

half<br />

Right<br />

half<br />

Inspection<br />

entry<br />

surface<br />

“Hoop” edge<br />

(Side 3) is<br />

always at the<br />

bottom of the<br />

image,<br />

allowing the<br />

other edges to<br />

be readily<br />

identified.<br />

“Edge effects”<br />

Table lists average<br />

and maximum<br />

gated-peak noise<br />

amplitude, as a<br />

percentage of the<br />

amplitude of the #1<br />

FBH in IN100 at<br />

the same water<br />

path and gain.<br />

Amplitudes are<br />

computed <strong>for</strong> the<br />

reduced-area<br />

region (illustrated<br />

above) with “edge<br />

effects” cropped.<br />

Figure 2. Details of backscattered grain noise measurements on the Honeywell <strong>for</strong>ging coupons.<br />

(a) Designation of inspection surfaces. (b) Noise C-scan and summary table <strong>for</strong> a typical case<br />

(inspection through OD face of coupon #3). (c) For a given coupon, results are tabulated <strong>for</strong> 8<br />

combinations of inspection direction and coupon quadrant.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Measured Noise Levels in Honeywell Ti 6-4 Forging Coupons<br />

Noise Level<br />

(100 = #1 FBH in Ti 6-4) .<br />

8.00<br />

7.00<br />

6.00<br />

5.00<br />

4.00<br />

3.00<br />

2.00<br />

1.00<br />

Red: Peak Noise<br />

Blue: Ave. Noise<br />

Honeywell Forging<br />

9<br />

AFT<br />

1<br />

10<br />

4<br />

6<br />

7 8<br />

FWD<br />

AFT<br />

(side 2)<br />

5<br />

6<br />

2<br />

5<br />

3<br />

OD<br />

0.00<br />

3 4 5 6 7 8<br />

12 3 4 5 6 7 8 12 3 4 5 6 7 8 1 2 3 4 5 6 7 8 1 2 3 4 5 6 7 8 1 2 3 4 5 6 7 8 1 2 3 4 5 6 7 8 1 2 3 4 5 6 7 8 1 2<br />

H1<br />

H2<br />

H3<br />

H4<br />

H6<br />

H8<br />

Coupon, and Quadrant<br />

Coupon, Inspection Direction, and Quadrant<br />

H5<br />

H7<br />

ID<br />

(side 4)<br />

4<br />

1<br />

3 2<br />

8 7<br />

FWD<br />

(side 5)<br />

OD<br />

(side 1)<br />

Figure 3. Comparison of peak (red) and average (blue) gated-peak noise levels in the Honeywellsupplied<br />

Ti 6-4 <strong>for</strong>ging coupons. Noise levels are relative to the amplitude of a (hypothetical) #1<br />

FBH located at the same depth in Ti 6-4 material. For each coupon eight values are shown,<br />

corresponding to different combinations of inspection directions and analysis quadrant.<br />

AFT<br />

Honeywell Coupon#5 Side 4 Attenuation<br />

9<br />

1<br />

2<br />

10<br />

4<br />

6<br />

5<br />

3<br />

OD<br />

Attenuation (Nepers/cm)<br />

0.05<br />

0.04<br />

0.03<br />

0.02<br />

0.01<br />

Full scan region<br />

Reduced scan region<br />

Power Law Fit<br />

fit is 0.00082 x freq 1.343<br />

7 8<br />

FWD<br />

0.00<br />

4 6 8 10 12 14 16 18<br />

Frequency (MHz)<br />

Figure 4. Measured average attenuation curve and associated power-law fit <strong>for</strong> the highest-noise<br />

coupon from the Honeywell Ti 6-4 <strong>for</strong>ging. The large arrow in the cross-sectional drawing of the<br />

<strong>for</strong>ging identifies the coupon and inspection direction. A 10-MHz, 0.25”-diameter planar probe was<br />

used. Average results are shown <strong>for</strong> the full scan region (central 1.5” x 0.75” of the entry surface)<br />

and <strong>for</strong> a reduced-area region (central 1.25” x 0.50”). Multiply attenuation values by 22.06 to<br />

change to dB/inch units.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 39


FOM (std. units)<br />

0.20<br />

0.18<br />

0.16<br />

0.14<br />

0.12<br />

0.10<br />

0.08<br />

0.06<br />

H5 Side 4 FOM (using meas. atten)<br />

Gate #1<br />

Gate#2<br />

Gate#3<br />

Gate#4<br />

Gate#5<br />

gate#6<br />

0.04<br />

0.02<br />

0.00<br />

5.0 10.0 15.0 20.0<br />

Frequency (MHz)<br />

RMS Noise (Volts)<br />

0.030<br />

0.025<br />

0.020<br />

0.015<br />

0.010<br />

0.005<br />

HW5 Side 4 RMS Noise<br />

Gate <strong>Center</strong> Duration<br />

G1 2.61 us (0.32”) 2.55 us<br />

G2 3.61 us (0.44”) 1.27 us<br />

G3 4.61 us (0.56”) 1.27 us<br />

G4 5.61 us (0.69”) 1.27 us<br />

G5 6.61 us (0.81”) 1.27 us<br />

G6 3.90 us (0.48”) 5.11 us<br />

G1<br />

G2<br />

G3<br />

G6<br />

G4<br />

G5<br />

0.000<br />

0 1 2 3 4 5 6 7 8 9 10<br />

Time after Front Wall Echo (usec)<br />

Figure 5. Measured grain-noise FOM values, as functions of frequency, <strong>for</strong> the Honeywell highnoise<br />

<strong>for</strong>ging coupon. The largest FOM values were seen <strong>for</strong> analysis Gate #3, centered about<br />

0.56” below the entry surface. The locations of the various gates used in the analysis of noise A-<br />

scans are shown in the rightmost panel which displays the measured rms noise level as a function<br />

of time. A 15-MHz, F7 focused transducer was used, and the peak in the rms noise curve<br />

corresponds to scattering by grains located in the focal zone.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Noise Anisotropy is<br />

defined as:<br />

9<br />

1<br />

10<br />

4<br />

6<br />

2<br />

5<br />

3<br />

Noise Inspected From Axial Direction<br />

Noise Inspected From Radial Direction<br />

We attempt to correlate NA with Y/X :<br />

Axial<br />

Radial<br />

7 8<br />

Elliptical<br />

Strain element<br />

X<br />

Figure 6. Left: DEFORM calculation showing how 5:1 elliptical elements in the billet are<br />

trans<strong>for</strong>med by the <strong>for</strong>ging process from the initial billet to the final <strong>for</strong>ged shape. (Only a portion of<br />

the billet is shown. Right: Definitions of the noise anisotropy and the ellipse projection ratio.<br />

Y<br />

NA (Axial Noise / Radial Noise) .<br />

Relationship between Noise Anisotropy and Forging<br />

De<strong>for</strong>mation (Starting from 5:1Ellipsoid)<br />

5.0<br />

sample#1<br />

sample#2<br />

sample#3<br />

sample#4<br />

sample#6<br />

sample#8<br />

4.0<br />

sample#5<br />

sample#7<br />

sample#9<br />

3.0<br />

2.0<br />

1.0<br />

Horizontal coordinate is the projection of<br />

the ellipse onto the axial inspection<br />

direction divided by the projection onto<br />

the radial inspection direction.<br />

0.0<br />

0 1 2 3 4 5 6<br />

Ellipse Projection Ratio<br />

Honeywell Forging Coupons<br />

Trendline<br />

NA (Axial Noise / Radial Noise) .<br />

2.5<br />

2.0<br />

1.5<br />

1.0<br />

0.5<br />

Relationship between Noise Anisotropy and Forging<br />

De<strong>for</strong>mation (Starting from 5:1Ellipsoid)<br />

P&W Forging Coupons<br />

Trendline<br />

sample#1<br />

sample#2<br />

sample#4<br />

sample#5<br />

sample#6<br />

sample#7<br />

sample#8<br />

0.0<br />

0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5<br />

Ellipse Projection Ratio<br />

Figure 7. Correlation between noise anisotropy and ellipse projection ratio <strong>for</strong> the Honeywell and<br />

P&W <strong>for</strong>gings. Each plotted point represents measurements within one quadrant of one <strong>for</strong>ging<br />

coupon.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 41


Peak> Range of Ave. Range of Peak<br />

GE: 0.81% 2.03% 0.2% - 1.9% 0.5% - 6.1%<br />

PW: 0.83% 2.31% 0.4% - 1.8% 0.7% - 5.5%<br />

HW: 0.88% 2.36% 0.4% - 2.5% 0.6% - 6.9%<br />

(#1 FBH in Ti 6-4 = 100%)<br />

Table 1. Comparison of average and maximum gated-peak noise voltages seen in the suites of<br />

coupons from the GE, P&W, and HW <strong>for</strong>gings. The first two columns list the average and<br />

maximum values <strong>for</strong> a given <strong>for</strong>ging, averaged over all coupons, inspection directions, and analysis<br />

quadrants. The last two columns list the ranges of measured values <strong>for</strong> average and peak noise in<br />

each <strong>for</strong>ging.<br />

Table 2. Comparison of UT properties <strong>for</strong> the high-noise coupons from the Pratt&Whitney, General<br />

Electric, and Honeywell Ti 6-4 <strong>for</strong>gings.<br />

Noise Curvature Blocks<br />

PW GE HW<br />

velocity (cm/usec): 0.622 0.618 0.621<br />

density (gm/cc): 4.43 4.43 4.43<br />

attenuation power law * : 6.83E-4*freq^1.79 4.31E-5*freq^2.26 8.20E-4*freq^1.34<br />

attenuation at 10 MHz: 0.93 dB/inch 0.17 dB/inch 0.40 dB/inch<br />

FOM power law * : 1.61E-3*freq^1.25 2.95E-3*freq^0.896 4.15E-3*freq^1.078<br />

Meas. FOM at 10 MHz: 0.027 0.021 0.047<br />

* For power laws, units are N/cm <strong>for</strong> attenuation, and<br />

cm^-0.5 <strong>for</strong> FOM, with the frequency input in MHz.<br />

Six “noise curvature blocks” were made to investigate the manner in which surface curvature<br />

influences inspection sensitivity in <strong>for</strong>gings. A principal use of the blocks will be to test models that<br />

predict the characteristics of backscattered grain seen during <strong>for</strong>ging inspections. The six blocks,<br />

each measuring approximately 1.6” x 5.9” x 2” (axial x radial x hoop) were fabricated by<br />

Pratt&Whitney from one of their Ti 6-4 <strong>for</strong>gings. The location of each block within the <strong>for</strong>ging<br />

cross-section is shown in Figure 8a. For five of the blocks, the upper surface in Figure 10a is<br />

curved, while the sixth block has a flat upper surface. Although each block was cut from the same<br />

position in the radial/axial plane of the <strong>for</strong>ging, the blocks, of necessity, had different angular<br />

positions, as shown in Figure 8b. Since microstructural variations in the hoop direction of a <strong>for</strong>ging<br />

are often minor, it was hoped that this construction method would produce six blocks with nearly<br />

identical microstructures.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 42


Preliminary measurements of backscattered noise levels through the (lower) flat surfaces of the<br />

blocks were carried out early in the quarter. Selected results are shown in Figure 9. Although the<br />

average noise levels were generally similar from block-to-block, the differences were deemed to be<br />

large enough to require further measurement and documentation. In addition, the preliminary<br />

measurements revealed that the flat block, which was cut from the <strong>for</strong>ging at a later date than the<br />

other five coupons, had been cut out “upside down” (i.e., with “TOP” and “BOT” faces reversed in<br />

Figure 8). This error, and the fact that the noise level in the ID portion of the <strong>for</strong>ging increases from<br />

“TOP” to “BOT” is responsible <strong>for</strong> the large difference seen in the right-hand portion of Figure 9<br />

between the noise level in the flat block and those of the other five coupons. Although un<strong>for</strong>tunate,<br />

this fabrication error was not deemed to be a major problem <strong>for</strong> testing the noise models. The<br />

principal noise measurements could be confined to the thicker zones of the blocks, and the flat<br />

block could simply be “flipped” when measurements were made.<br />

During the quarter, additional noise measurements were made through the flat surfaces of the<br />

blocks to: (1) carefully document the effect of microstructural differences between blocks; and (2) to<br />

test noise model predictions <strong>for</strong> inspections through flat surfaces. The measurements themselves,<br />

and subsequent analysis to calculate relevant noise statistics, were per<strong>for</strong>med at Pratt&Whitney.<br />

Additional analyses and model predictions were then carried out at ISU.<br />

This second round of measurements was made using a “characterized” 10-MHz transducer whose<br />

effective focal properties had been carefully determined (effective diameter = 0.344”; geometric<br />

focal length = 3.95”). Measurements through the flat surfaces of the blocks were made <strong>for</strong> two<br />

water paths: 2.4”, which put the actual focal spot just under the entry surface; and 1.0”, which put<br />

the focal spot approximately 0.5” deep in the metal. In each case the probe was scanned over a 3”<br />

x 0.5” (radial x hoop) region using a step size of 0.015” in each direction. The noise A-scans<br />

acquired at each site were stored <strong>for</strong> later processing. Each day that noise data was acquired, a<br />

reference echo from a #1 FBH in a calibration block was also measured. The reference echo was<br />

used to correct <strong>for</strong> minor differences in measurement system efficiency from one measurement trial<br />

to the next. In addition, the electronic noise level was measured so that it could be properly<br />

accounted <strong>for</strong> when noise model predictions were compared with experiment.<br />

The manner in which the measured noise level depends upon depth is shown in Figures 10 and 11<br />

<strong>for</strong> the 2.4” and 1.0” water paths, respectively. In the left-hand panels, the rms noise levels,<br />

averaged over the lateral scan positions, are shown <strong>for</strong> each block. Block-to-block differences in<br />

noise levels can be seen which presumably result from variations in the <strong>for</strong>ging microstructure with<br />

circumferential position. Also shown in Figures 10 and 11 are rms noise levels predicted using an<br />

ISU model. The model assumes a uni<strong>for</strong>m microstructure, and requires ultrasonic velocity,<br />

attenuation, and grain noise Figure-of-Merit (FOM) values as inputs. Initial guesses <strong>for</strong> the model<br />

inputs were obtained by averaging values measured in a suite of smaller coupons cut from one<br />

section of the same <strong>for</strong>ging (see Figure 8b). The estimated FOM value was then increased by 10%<br />

to bring the predicted rms noise level more into line with the average of the measurements on the<br />

six noise curvature blocks. In Figures 10-11, there is good agreement between the model<br />

prediction and the average experimental result in the central depth region, i.e., away from the<br />

influences of the front-wall and back-wall echoes. Also note that the location and width of the focal<br />

maximum in Figure 11 is well predicted by the theory.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 43


The average noise characteristics, as reflected by the rms-noise-versus-depth curves, are<br />

somewhat different <strong>for</strong> the different blocks. For each block the following procedure was used to<br />

determine a depth-dependent “microstructure difference factor”. (1) The measured rms-noiseversus<br />

depth curve was adjusted to remove the (minor) effect of electronic noise. (2)<br />

The six rms noise curves (one <strong>for</strong> each block) were averaged to determine the mean curve <strong>for</strong> the<br />

suite of coupons. This was done separately <strong>for</strong> each inspection water path. (3) The rms noise<br />

curve <strong>for</strong> a given coupon was divided by the mean curve to determine the fractional deviation from<br />

the mean at each metal depth. As shown in Figure 12, these difference factors were found to be<br />

nearly identical <strong>for</strong> the two inspections at different water paths, indicating that they do indeed arise<br />

from microstructural variations. (4) The difference factors measured <strong>for</strong> a given block using the 2.4”<br />

and 1.0” water paths were then averaged. In future analyses of grain noise measured through the<br />

curved surfaces of the blocks, these difference factors will be used (with the distance scale<br />

inverted) to “correct” noise quantities <strong>for</strong> microstructural differences. Remaining differences in<br />

noise properties will then presumable be due to surface curvature effects.<br />

From the stored grain noise A-scans, other noise statistics can be readily computed. For example,<br />

<strong>for</strong> one typical block, Figure 13 shows gated-peak noise C-scans reconstructed from the flatsurface<br />

A-scan data <strong>for</strong> four choices of the time gate. As the gate is widened, keeping its center at<br />

the same depth, the average noise is seen to increase, as expected. Similar C-scan images were<br />

generated <strong>for</strong> all six coupons, and the average and maximal noise amplitude in each image was<br />

tabulated. Results are shown in graphical <strong>for</strong>m in Figure 14-15, where they are compared to the<br />

predictions of the ISU noise model (rightmost portion of each plot). The model the does a good job<br />

of predicting the average gated peak noise amplitude <strong>for</strong> each of the four gates. However, the<br />

theory tends to underestimate the maximum noise amplitude seen in a given C-scan. The current<br />

noise model assumes a uni<strong>for</strong>m “average” microstructure. The actual microstructure of a typical<br />

block varies only modestly with axial depth, but varies quite significantly with radial position, as can<br />

be seen in Figure 13. In the future the model <strong>for</strong> gated-peak noise statistics will be modified to<br />

account <strong>for</strong> such microstructural variations. This should improve predictions of maximal gated-peak<br />

noise amplitudes.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 44


6.8”<br />

ID<br />

“Side 5” = “BOT”<br />

OD<br />

CURVED<br />

SURFACE<br />

1.64”<br />

0.49”<br />

0.75”<br />

0.49”<br />

1.5”<br />

#1 FBH<br />

“Side 2” = “TOP”<br />

0.1”<br />

(a)<br />

3.4”<br />

3.4”<br />

This side of the block<br />

will be rounded to ensure<br />

that the length of the block is 6.8”<br />

convex 4.0<br />

4<br />

The interior<br />

edges may be<br />

lopped to ensure<br />

that all 5 blocks<br />

fit within the<br />

<strong>for</strong>ging<br />

3<br />

convex 10.0<br />

5<br />

200 o<br />

(ref. gap)<br />

Material not available<br />

from this section<br />

Small coupons <strong>for</strong><br />

earlier property<br />

measurements<br />

260 o<br />

2”<br />

Flat block was<br />

later machined<br />

from one of the<br />

remaining<br />

wedges<br />

concave 8.0<br />

2<br />

1<br />

(b)<br />

concave 2.0<br />

concave 0.75<br />

(c)<br />

Figure 8. Positions of noise curvature blocks relative to the original P&W Ti 6-4 <strong>for</strong>ging. (a)-(b):<br />

Locations of the curved blocks in the radial-axial (a) and radial-hoop (b) planes. (c) The flat block<br />

was machined later from one of the remaining wedges, and is slightly shorter in the radial direction.<br />

Curved blocks have radii of curvature of 0.75” concave, 2” concave, 8” concave, 4” convex, and 10”<br />

convex, respectively.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 45


Noise C-scans through the “Flat Surfaces” of the Six Specimens<br />

10 MHz, 0.375”D, focal depth in water = 2.65”, Amp=7, Damping=1, Pulse Width = 20ns<br />

Waterpath = 1.0in, Focus ≈ 0.5” deep, Gain = 57.0dB, Gate delay = 0.3in, Gate Range = 0.4in<br />

OD<br />

Thicker region<br />

Thinner region<br />

ID<br />

22.4%<br />

10.0” Radius Convex Block<br />

28.4%<br />

18.8%<br />

4.0” Radius Convex Block<br />

27.2%<br />

17.1%<br />

Flat Reference Block<br />

14.1%<br />

22.9%<br />

0.75” Radius Concave Block<br />

32.8%<br />

23.3%<br />

2.0” Radius Concave Block<br />

32.3%<br />

19.9%<br />

8.0” Radius Concave Block<br />

30.5%<br />

Figure 9. Preliminary C-scans showing gated-peak grain noise levels measured through the flat<br />

surfaces of the six noise curvature blocks. Average noise levels as a percentage of full screen<br />

height are listed.<br />

Noise Measurements thru Flat Entry Surfaces<br />

2.4" water path; 57 dB<br />

Noise Measurements thru Flat Entry Surfaces<br />

2.4" water path; 57 dB<br />

RMS Grain Noise (% of FSH) .<br />

12<br />

Flat, FBHs in back<br />

Flat, FBHs in front<br />

0.75 cv 2.0 cv<br />

10<br />

8.0 cv 4.0 cx<br />

10.0 cx Theory<br />

8<br />

Model assumes: FOM = 1.1* (5.6E-4*freq^1.25)<br />

Atten = 5.7E-4*freq^1.8<br />

6<br />

4<br />

2<br />

Exp. values corrected <strong>for</strong> electronic<br />

noise and Ref signal differences<br />

0<br />

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6<br />

RMS Grain Noise (% of FSH) .<br />

12<br />

Theory<br />

Exp. Ave.<br />

10<br />

Model assumes: FOM = 1.1* (5.6E-4*freq^1.25)<br />

Atten = 5.7E-4*freq^1.8<br />

8<br />

6<br />

4<br />

2<br />

Exp. values corrected<strong>for</strong> electronic<br />

noise and Ref signal differences<br />

0<br />

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6<br />

Metal Depth (inches)<br />

Metal Depth (inches)<br />

Figure 10. Comparison of measured and predicted rms grain noise levels <strong>for</strong> inspections through<br />

the flat surfaces of the six noise curvature blocks using a 2.4” water path. Left-hand panel displays<br />

the measured noise levels <strong>for</strong> the six blocks individually, while the right-hand panel displays their<br />

average.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 46


Noise Measurements thru Flat Entry Surfaces<br />

1.0" water path; 57 dB<br />

Noise Measurements thru Flat Entry Surfaces<br />

1.0" water path; 57 dB<br />

RMS Grain Noise (% of FSH) .<br />

14<br />

12<br />

10<br />

Flat, FBHs in back<br />

Flat, FBHs in front<br />

0.75 cv 2.0 cv<br />

8.0 cv 4.0 cx<br />

10.0 cx Theory<br />

8<br />

6<br />

4<br />

2<br />

Exp. values corrected<br />

Model assumes: FOM = 1.1* (5.6E-4*freq^1.25)<br />

<strong>for</strong> electronic noise<br />

Atten = 5.7E-4*freq^1.8<br />

0<br />

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6<br />

Metal Depth (inches)<br />

RMS Grain Noise (% of FSH) .<br />

14<br />

Theory<br />

Exp. Ave.<br />

12<br />

Exp. values corrected<br />

<strong>for</strong> electronic noise<br />

10<br />

8<br />

6<br />

4<br />

2<br />

Model assumes: FOM = 1.1* (5.6E-4*freq^1.25)<br />

Atten = 5.7E-4*freq^1.8<br />

0<br />

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6<br />

Metal Depth (inches)<br />

Figure 11. Comparison of measured and predicted rms grain noise levels <strong>for</strong> inspections through<br />

the flat surfaces of the six noise curvature blocks using a 1.0” water path. Left-hand panel displays<br />

the measured noise levels <strong>for</strong> the six blocks individually, while the right-hand panel displays their<br />

average.<br />

Coupon Noise / Average<br />

(a)<br />

Coupon Noise / Average .<br />

1.80<br />

1.60<br />

1.40<br />

1.20<br />

1.00<br />

RMS grain noise in Ti noise curvature blocks<br />

measured from flat side, water path = 2.4"<br />

Normalized by average over six coupons.<br />

flat with FBHs in back<br />

0.75 cv<br />

2.0 cv<br />

8.0 cv<br />

4.0 cx<br />

10.0 cx<br />

0.80<br />

(5 and 0.62 dB corrections to "flat")<br />

0.60<br />

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6<br />

1.4<br />

1.3<br />

1.2<br />

1.1<br />

Depth (inches)<br />

RMS grain noise in Ti noise curvature blocks measured from<br />

flat side, normalized by average over six coupons.<br />

4.0 cx- 1.0"<br />

4.0 cx - 2.4"<br />

4.0 cx - ave.<br />

1.0<br />

0.9<br />

0.8<br />

4.0” – Convex Specimen<br />

0.7<br />

(c)<br />

0.6<br />

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6<br />

Depth (inches)<br />

Coupon Noise / Average<br />

Coupon Noise / Average .<br />

1.80<br />

1.60<br />

1.40<br />

1.20<br />

1.00<br />

0.80<br />

(b)<br />

(d)<br />

RMS grain noise in Ti noise curvature blocks<br />

measured from flat side, water path = 1"<br />

Normalized by average over six coupons.<br />

flat with FBHs in back<br />

0.75 cv<br />

2.0 cv<br />

8.0 cv<br />

4.0 cx<br />

10.0 cx<br />

0.60<br />

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6<br />

1.4<br />

1.3<br />

1.2<br />

1.1<br />

1.0<br />

0.9<br />

0.8<br />

0.7<br />

Depth (inches)<br />

RMS grain noise in Ti noise curvature blocks measured from<br />

flat side, normalized by average over six coupons.<br />

0.75” – Concave Specimen<br />

0.6<br />

0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6<br />

Depth (inches)<br />

0.75 cv - 1.0"<br />

0.75 cv - 2.4"<br />

0.75 cv - ave.<br />

Figure 12. (a)-(b): Microstructure difference factors, as functions of depth, measured using water<br />

paths of 2.4” and 1.0”, respectively. (c)-(d): More detailed views of the microstructure correction<br />

factors <strong>for</strong> two of the blocks.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 47


4.0” Convex Block; Flat Side Inspection; 1.0” Water Path<br />

Depth Zone<br />

Gate 1<br />

0.8”-1.0”<br />

Gate 2<br />

0.7”-1.1”<br />

Gate 3<br />

0.6”-1.2”<br />

Gate 4<br />

0.5”-1.3”<br />

OD<br />

ID<br />

Figure 13. Gated peak noise C-scan images <strong>for</strong> four choices of the time gate (or depth zone).<br />

Results are shown <strong>for</strong> one of the noise curvature blocks inspected at a 1” water path.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 48


% FSH<br />

25<br />

20<br />

15<br />

10<br />

Noise Measurements from flat side, water path = 1"<br />

Average Gated Peak Noise, Gain = 57 dB, I3 probe<br />

Gate1<br />

Gate 2<br />

Gate 3<br />

Gate 4<br />

5<br />

0<br />

Flat with<br />

FBH in<br />

back<br />

Flat with<br />

FBH in<br />

front<br />

0.75"<br />

concave<br />

2.0"<br />

concave<br />

8.0"<br />

concave<br />

4.0"<br />

convex<br />

10.0"<br />

convex<br />

THEORY<br />

% FSH<br />

25<br />

20<br />

15<br />

10<br />

5<br />

Noise Measurements from flat side,water path=2.4"<br />

Average Gated Peak Noise, Gain = 57 dB, I3 probe<br />

Gate1<br />

Gate 2<br />

Gate 3<br />

Gate 4<br />

0<br />

Flat with<br />

FBH in<br />

back<br />

Flat with<br />

FBH in<br />

front<br />

0.75"<br />

concave<br />

2.0"<br />

concave<br />

8.0"<br />

concave<br />

4.0" convex 10.0"<br />

convex<br />

THEORY<br />

Figure 14. Measured and predicted average amplitudes in gated-peak noise C-scan images.<br />

Results are shown <strong>for</strong> the four choices of the time gate (or depth zone) <strong>for</strong> each inspection water<br />

path.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

print date/time: 6/6/2002 - 8:39 AM – Page 49


% FSH<br />

Noise Measurements from flat side, water path = 1"<br />

Maximum Gated Peak Noise, Gain = 57 dB, I3 probe<br />

80<br />

60<br />

40<br />

Gate1<br />

Gate 2<br />

Gate 3<br />

Gate 4<br />

20<br />

0<br />

Flat with<br />

FBH in<br />

back<br />

Flat with<br />

FBH in<br />

front<br />

0.75"<br />

concave<br />

2.0"<br />

concave<br />

8.0"<br />

concave<br />

4.0"<br />

convex<br />

10.0"<br />

convex<br />

THEORY<br />

% FSH<br />

80<br />

60<br />

40<br />

20<br />

Noise Measurements from flat side,water path=2.4"<br />

Maximum Gated Peak Noise, Gain = 57 dB, I3 probe<br />

Gate1<br />

Gate 2<br />

Gate 3<br />

Gate 4<br />

0<br />

Flat with<br />

FBH in<br />

back<br />

Flat with<br />

FBH in<br />

front<br />

0.75"<br />

concave<br />

2.0"<br />

concave<br />

8.0"<br />

concave<br />

4.0" convex 10.0"<br />

convex<br />

THEORY<br />

Figure 15. Measured and predicted maximum amplitudes in gated-peak noise C-scan images.<br />

Results are shown <strong>for</strong> the four choices of the time gate (or depth zone) <strong>for</strong> each inspection water<br />

path.<br />

Synthetic Inclusion Disk<br />

Machining of the <strong>for</strong>ging continued following the initial evaluation of the as-<strong>for</strong>ged piece described<br />

in the previous quarterly report. Mike Gigliotti (GE-CRD) requested that the machined <strong>for</strong>ging be<br />

delivered to him with an excess material envelope of 0.25” on the outer diameter and 0.1” on the<br />

<strong>for</strong>ward and aft faces, outside the planned final dimensions. The machining and ultrasonic<br />

inspection were planned in two stages. Initially the outside diameter (face UG) and four flat faces<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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(UO, US, UM, UH) were machined, and were inspected ultrasonically (see figure 16 <strong>for</strong><br />

identification of faces). Then the remaining faces were machined, with the exception of the bore<br />

UZ, since the piece will be delivered with a solid bore.<br />

Figure 16. Configuration and face identification of the synthetic inclusion <strong>for</strong>ging.<br />

Plans (April 1, 2002 – June 30, 2002):<br />

Property Measurements Continue ef<strong>for</strong>ts to relate grain noise variations within <strong>for</strong>gings to <strong>for</strong>ging<br />

strain variations as predicted using DEFORM.<br />

Noise Curvature Blocks: Per<strong>for</strong>m grain noise measurements through the curved surfaces of the<br />

blocks. Compare RMS and gated-peak noise statistics, corrected <strong>for</strong> microstructural differences to<br />

the predictions of the ISU model.<br />

Synthetic Inclusion Disk: The remaining faces of the machined <strong>for</strong>ging will be inspected<br />

ultrasonically. The data will be analyzed to verify that the noise levels and noise distributions make<br />

it a suitable piece <strong>for</strong> the synthetic inclusion <strong>for</strong>ging. It will then be delivered to GE CR&D <strong>for</strong><br />

continued machining into its final <strong>for</strong>m.<br />

Milestones:<br />

Original<br />

Date<br />

Revised<br />

Date<br />

Description<br />

Status<br />

Flaw and sample definition<br />

3 months Generate critical flaw list <strong>for</strong> titanium <strong>for</strong>gings in<br />

cooperation with RISC and provide to 3.1.2. (All)<br />

4 months Utilize de<strong>for</strong>mation model predictions to guide<br />

sample development. (PW with support from ISU)<br />

6 months 11 months Provide list of samples and sample geometry to be<br />

developed <strong>for</strong> <strong>for</strong>ging property measurements.<br />

(ISU with support from GE, PW)<br />

Complete<br />

Complete<br />

Complete<br />

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Original<br />

Revised<br />

Description<br />

Status<br />

Date<br />

Date<br />

Sample fabrication<br />

12-30<br />

months<br />

Acquire/fabricate the necessary samples. (GE with<br />

support from PW, AS)<br />

Complete<br />

Fundamental property measurements<br />

12 - 36<br />

months<br />

Acquire velocity, attenuation, backscattered noise,<br />

and defect-echo data necessary to assess the<br />

effects of microstructural anisotropy and surface,<br />

curvature, etc., on <strong>for</strong>ging inspections. (ISU with<br />

support from GE, PW, AS)<br />

18 months 24 months Provide velocity data <strong>for</strong> incorporation into the<br />

noise model. (ISU with support from GE, PW, AS)<br />

Complete techniques <strong>for</strong> curvature correction<br />

approaches. (All)<br />

24 months Provide surface curvature data <strong>for</strong> development of<br />

curvature correction factors. Provide data to 1.3.2<br />

<strong>for</strong> transducer design optimization. (ISU with<br />

support from GE, PW, AS)<br />

24 - 39<br />

months<br />

Validate noise models in cooperation with 3.1.2.<br />

(All)<br />

45 months Report of the effects of anisotropy and surface<br />

curvature on inspection sensitivity <strong>for</strong> typical<br />

titanium <strong>for</strong>gings used in aircraft engines.<br />

45 months Initiate final report. (All)<br />

45 months Techniques used to correct <strong>for</strong> geometry effects<br />

including curvature correction factors.<br />

54 months Complete final report. (All)<br />

60 months Representative sample blocks of <strong>for</strong>ging material or<br />

fundamental property measurements.<br />

Primary measurements required to<br />

assess effects of microstructural<br />

anisotropy completed using<br />

property/flow line blocks). For<br />

surface curvature effects see below<br />

Complete<br />

Complete<br />

Work initiated using “Noise<br />

Curvature Blocks” to assess<br />

combined effects of surface<br />

curvature and microstructure on<br />

inspections, and to validate noise<br />

models.<br />

Deliverables:<br />

Techniques to correct <strong>for</strong> geometry effects including curvature correction factors.<br />

Report of effect of anisotropy and surface curvature on inspection sensitivity <strong>for</strong> typical titanium<br />

<strong>for</strong>gings used in aircraft engines.<br />

Representative sample blocks of <strong>for</strong>ging material or fundamental property measurements.<br />

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Metrics:<br />

Assessments of the effects of microstructural anisotropy and surface curvature on inspection<br />

sensitivity <strong>for</strong> typical titanium <strong>for</strong>gings, supporting the needs of inspection development, POD<br />

estimation, and life management tasks.<br />

Comparisons of inspections using standard and optimized transducer designs, quantifying the<br />

improvement in detection sensitivity.<br />

Major Accomplishments and Significant Interactions:<br />

Date<br />

June 16, 1999<br />

Description<br />

Technical Kick-off Meeting in West Palm Beach, FL<br />

Publications and Presentations:<br />

Date<br />

2002<br />

Description<br />

L. Yu, F.J. Margetan, R.B. Thompson and A. Degtyar, “Survey of Ultrasonic Properties of Aircraft<br />

<strong>Engine</strong> <strong>Titanium</strong> Forgings”, Rev. of Prog. in QNDE, Vol.21, eds. D.O. Thompson and D.E.<br />

Chimenti, (AIP, Melville NY, in press)<br />

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Project 1:<br />

Task 1.3:<br />

Subtask 1.3.2:<br />

Production Inspection<br />

<strong>Titanium</strong> Forging Inspection<br />

Inspection Development <strong>for</strong><br />

<strong>Titanium</strong> Forgings<br />

Team Members:<br />

HW: Andy Kinney, Tim Duffy, Waled<br />

Hassan<br />

ISU: Tim Gray, Bruce Thompson, Frank<br />

Margetan, Ron Roberts<br />

GE: Dave Copley, Ed Nieters, Wei Li, Bob<br />

Gilmore, , Jon Bartos, , Richard Klaassen,<br />

Mike Keller, John Halase<br />

PW: Jeff Umbach, Bob Goodwin, Andrei<br />

Degtyar, Harpreet Wasan, Dave Raulerson<br />

Students: none<br />

Program initiation date: June 15, 1999<br />

Objectives:<br />

• To develop a high sensitivity ultrasonic inspection of titanium <strong>for</strong>gings utilizing a 1/128” (#½)<br />

FBH calibration target, digital C-scan image acquisition, and signal-to-noise rejection criteria<br />

target without significant cost increase.<br />

• To demonstrate the new technique in a production environment over an extended period to<br />

determine its feasibility (both cost and readiness) as a production inspection.<br />

Approach:<br />

Forging Selection and Preparation: Select one representative <strong>for</strong>ging design from each of the<br />

OEMs <strong>for</strong> use throughout the duration of this subtask (both inspection development and<br />

demonstration). Selection criteria will include:<br />

• <strong>for</strong>ging shapes that address generic concerns such as effects of curvature, surface condition,<br />

and part thickness<br />

• <strong>for</strong>ging material and microstructure<br />

• <strong>for</strong>ging cost<br />

• production volume and schedule<br />

Sensitivity and coverage maps will be developed <strong>for</strong> the selected <strong>for</strong>gings using model-based tools.<br />

CAD files will be provided to ISU by each of the OEMs <strong>for</strong> the selected <strong>for</strong>ging geometries.<br />

Particular attention will be given to the effect of curved surfaces on inspection sensitivity relative to<br />

flat surface sensitivity. Calibration standards will be designed to cover the range of metal travel and<br />

curvatures found on the selected <strong>for</strong>gings. Plans include two sets of standards in order to support<br />

multiple member involvement.<br />

Transducer Design Models: Fixed focus and phased array transducer design models will be<br />

reevaluated in detail to determine reasons <strong>for</strong> discrepancies between predicted and measured<br />

subsurface focused transducer behavior observed during Phase I work. This reevaluation will focus<br />

initially on assessing how well the input parameters used <strong>for</strong> the models represent the physical<br />

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ehavior of the transducers. This ef<strong>for</strong>t will begin as part of Task 1.1 and 1.2 which will concentrate<br />

on fixed focus transducers. Two blocks (one <strong>for</strong> fixed-focus and one <strong>for</strong> phased array) suitable <strong>for</strong><br />

the evaluation of subsurface focused transducers will be manufactured to provide experimental<br />

data with consideration given to samples available in 1.3.1. Based on this exercise, modifications<br />

will be made to model input parameters or to the model code to improve the prediction accuracy.<br />

Attention will also be paid to selection of transducer materials with consistent and measurable<br />

properties, <strong>for</strong> example the machining of lenses from solid material rather than using cast-in-place<br />

epoxy. Coordination with transducer and system vendors is expected with the objective of ensuring<br />

that results of this ef<strong>for</strong>t impact the per<strong>for</strong>mance characteristics of future products used in jet engine<br />

inspection.<br />

Surface Finish Effects: The effect of surface finish on inspectability will be determined. Surface<br />

finish requirements are anticipated to be more stringent at the higher sensitivity inspections<br />

necessary <strong>for</strong> <strong>for</strong>gings (compared to billet) and will be a focus of study in this subtask. Empirical<br />

and theoretical approaches will be used to assess the relationship between surface finish and<br />

inspectability. Empirical studies will be limited to 100 machining passes spread across five 13”<br />

diameter by 2” thick pancake samples. Results will be implemented in the UT modeling tools.<br />

Transducer Design and Selection: The ultrasonic beam properties (frequency, depth-of-field,<br />

diameter, bandwidth, mode, etc.) required to produce an acceptable 1/128” FBH calibration (FBH<br />

@ 80%, Ti grain noise < 50%) will be defined. Fixed focus transducers <strong>for</strong> flat entry surfaces will be<br />

designed, manufactured, and evaluated using appropriate ETC test specimens as necessary. An<br />

assessment of the transducers (producing the above determined ultrasonic beam properties)<br />

necessary to inspect the three OEM <strong>for</strong>gings will be made. Any additional required transducers will<br />

be designed and manufactured. A commercial source <strong>for</strong> such transducers will be established.<br />

Productivity Improvement: It was shown in Phase I that inspection sensitivity improvements will, in<br />

general, increase the time required <strong>for</strong> the inspection. Fixed-focus transducer inspection<br />

approaches have the advantage of being expandable (in an economical fashion) to include the<br />

collection of data from multiple transducers simultaneously. This approach has the potential to<br />

offset the productivity losses which will likely occur from the increased inspection sensitivity<br />

required by this task. In order to meet the inspection time goals <strong>for</strong> this task, a study will be made<br />

of the OEM <strong>for</strong>gings to determine potential areas of productivity improvement. A maximum<br />

productivity approach will be defined and developed <strong>for</strong> evaluation in the laboratory demonstration.<br />

Fixed Focus Laboratory Testbed: Laboratory testbed <strong>for</strong> the development and evaluation of the<br />

fixed-focus inspection approach <strong>for</strong> a 1/128” FBH calibration <strong>for</strong>ging inspection with digital C-scan<br />

data acquisition and SNR based rejection criterion will be established. Additional transducers<br />

necessary to inspect the OEM <strong>for</strong>gings will be designed, manufactured and tested. Scan plans <strong>for</strong><br />

the selected OEM <strong>for</strong>gings will be developed with model-based support. A limited number (1-2) of<br />

each of the selected <strong>for</strong>gings will be inspected per the scan plan. Per<strong>for</strong>mance of the fixed focus<br />

inspection approach <strong>for</strong> <strong>for</strong>ging inspection will be documented. Alternative inspection technologies<br />

will be identified using the experience base of the four partners, as well as NTIAC.<br />

Phased Array Inspection: An evaluation will be made of available phased array technology to<br />

determine which are potentially production-ready and capable. At this time, the digital focused<br />

array transducer system DFATS annular phased array and the R/D Tech 2D array are known as<br />

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possible candidates. Development work on these approaches will be limited to building one sensor<br />

assembly <strong>for</strong> each approach if suitable sensors are not already available at the OEMs. <strong>Evaluation</strong><br />

will be per<strong>for</strong>med on appropriate ETC test specimens with both flat and curved sound entry<br />

surfaces. It is expected that phased array approaches will be necessary to arrive at the necessary<br />

sensitivity through curved surfaces. Arrangements will be made to accommodate full team<br />

participation <strong>for</strong> all of these evaluations. The results will be reviewed to identify a preferred<br />

alternative inspection technology. The review will consider inspection per<strong>for</strong>mance, equipment cost<br />

and complexity, operating speed, potential <strong>for</strong> productivity improvements, and other implementation<br />

factors.<br />

Phased Array Laboratory Testbed: A laboratory testbed <strong>for</strong> the development and evaluation of the<br />

alternative inspection approach <strong>for</strong> a 1/128” FBH calibration <strong>for</strong>ging inspection with digital C-scan<br />

data acquisition and SNR based rejection criterion will be established. Additional transducers<br />

necessary to inspect the OEM <strong>for</strong>gings will be designed, manufactured and tested. Scan plans <strong>for</strong><br />

the selected OEM <strong>for</strong>gings will be developed. A limited number (1-2) of each of the selected<br />

<strong>for</strong>gings will be inspected per the scan plan. The full description of the testbed is not known at this<br />

time because of its dependence on the initial assessment. An amendment and appropriate request<br />

<strong>for</strong> funding will be prepared in consultation with the FAA when the details are completed.<br />

Factory Testbed, <strong>Evaluation</strong> and Demonstration: The laboratory results from the fixed-focus and<br />

alternative inspection method will be reviewed to identify a preferred configuration <strong>for</strong> factory<br />

demonstration and potential implementation. The review will consider inspection per<strong>for</strong>mance,<br />

equipment cost and complexity, operating speed, and other implementation factors. A hybrid<br />

system using fixed focus and an alternative inspection technology will be considered as part of this<br />

evaluation. The chosen configuration will be used to per<strong>for</strong>m factory evaluation of 30 <strong>for</strong>gings at a<br />

production inspection facility. A production testbed with digital C-scan data acquisition will be<br />

established <strong>for</strong> the evaluation of the 1/128” FBH calibration <strong>for</strong>ging inspection technique. (This may<br />

include the purchase of additional capital equipment if none is present at production inspection<br />

facility or available <strong>for</strong> loan from a consortium member.) Scan plans <strong>for</strong> the selected OEM <strong>for</strong>gings<br />

will be written by the respective OEM with ISU providing support using the inspectability model<br />

tools. Attention will be given to maximize productivity (to minimize any cycle time impact caused by<br />

the higher sensitivity) <strong>for</strong> the inspection during the production testbed design and scan plan<br />

development. Any additional transducers required to implement the scan plans will be designed<br />

using the transducer design models and built using commercial sources. A total of 30 <strong>for</strong>gings (10<br />

from each OEM) will be inspected over the course of 10 months. Noise levels with respect to the<br />

calibration target, and actual inspection time in hours will be documented <strong>for</strong> each <strong>for</strong>ging and<br />

provided to task 3.1.2. Any detections will be first reported to the responsible OEM. Up to six<br />

indications (from up to three separate <strong>for</strong>gings) which fail the proposed acceptance limits will be<br />

destructively evaluated to determine their cause. Funds to purchase these <strong>for</strong>gings are not<br />

included in the current proposal but will require an amendment at the time. The actual hours <strong>for</strong> the<br />

conventional production inspection of these <strong>for</strong>gings will be gathered and compared to the time of<br />

the 1/128” FBH inspection to establish a per part cost difference. Additional cost components will<br />

include items such as system cost, longevity of equipment, recurring equipment costs, and costs<br />

associated with false calls. An industry demonstration will be held to provide the results to the other<br />

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OEMs and the <strong>for</strong>ging industry. A final report summarizing the results of the technical ef<strong>for</strong>t and the<br />

final factory demonstration will be written in the required FAA <strong>for</strong>mat.<br />

Objective/Approach Amendments: Objective and approach remain as originally proposed in July<br />

1998.<br />

Progress (January 1, 2002 – March 31, 2002):<br />

Significant progress was made towards the goal of achieving #1/2 FBH sensitivity in Ti-6-4 <strong>for</strong>gings.<br />

Progress was made in both defining the inspection parameters and the supporting tasks of creating<br />

calibration standards and defining surface condition requirements with additional details provided<br />

below.<br />

Calibration Standards<br />

The team agreed on a final design <strong>for</strong> the standards that will make them more generic rather than<br />

useful <strong>for</strong> a single inspection scenario. Initially, the standards were to reflect the requirements of<br />

the three OEM <strong>for</strong>gings to be used in this program. The zones that were initially defined were from<br />

the inspection of these three <strong>for</strong>gings and are dependent on the noise in the coupons made from<br />

sample <strong>for</strong>gings. The team agreed it would be a mistake to create the calibration standards just <strong>for</strong><br />

zones defined <strong>for</strong> those samples. Instead, the standards will have FBHs placed at fairly fine<br />

increments, 0.05”, so that zones can be defined and setups made <strong>for</strong> a variety of zone depths <strong>for</strong> a<br />

range of <strong>for</strong>ging geometries.<br />

Four blocks will be required to accomplish 0.05” steps to a depth of 4.0”. The first depth, however,<br />

will be at 0.06” to meet current near surface setup requirements. The second hole depth is at 0.10”<br />

and all subsequent hole depths are at incremental depths of 0.05”. The design of the first block is<br />

shown in Figure 1. GE has had all 4 blocks machined with the steps and plans are in place to have<br />

the FBHs drilled. The completion of the standards is expected to be within the revised milestone<br />

date of month 36.<br />

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Forging Calibration Standard #1<br />

1.75"<br />

.300"<br />

7.0"<br />

0.216<br />

.300"<br />

1.156"<br />

holes drilled .156" deep<br />

02/13/2002<br />

Figure 1. One of the four blocks comprising the set of calibration standards <strong>for</strong> zoned <strong>for</strong>ging<br />

inspections.<br />

Analysis of supplier capability to create FBHs was tested with the sample of 2” cube material made<br />

from powder Ti-6-4. Several attempts at analyzing the condition of the holes was presented in<br />

earlier reports that included replication and laser profilometry analysis. During this reporting period,<br />

GE has carried out metallographic analysis of the holes to complete the evaluation. The analysis<br />

was completed in 2 steps. First, the block was ground to a thickness that is 5 to 10 mils above the<br />

bottom of the hole. This view allowed measurement of the roundness of the hole including focus to<br />

the bottom of the hole. The second step consisted of transverse polishing to evaluate flatness of<br />

the bottom of the hole. Figure 2 shows a representative example of the analysis that was<br />

per<strong>for</strong>med on several holes that were produced by 2 suppliers. The result of this analysis is that<br />

the 2 suppliers that made FBHs <strong>for</strong> this study are equally capable of providing the features that<br />

were requested. One of the suppliers is able to provide smaller holes with their equipment.<br />

Historically, only one of the suppliers was used <strong>for</strong> calibration standards and this study shows that a<br />

second supplier is also capable.<br />

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#1 FBH<br />

2A Top<br />

2A Side<br />

1A 1B 1C<br />

2A 2B 2C<br />

3A 3B 3C<br />

2A Bottom<br />

Figure 2. Sample of metallographic evaluation of FBHs.<br />

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Surface Finish Studies<br />

The plans <strong>for</strong> the surface finish study have been refined during this reporting period with<br />

significant input by the three OEMs. GE has primary responsibility <strong>for</strong> this activity and will<br />

initiate the execution of the plan. While the plan is not quite finalized, the sequence of events<br />

is as follows –<br />

(1) GE has FBHs placed in the pancake, per<strong>for</strong>ms UT characterizing of the holes, applies the<br />

1 st set of machining passes, acquires profiles of the machining grooves, and per<strong>for</strong>ms UT<br />

with specified transducers,<br />

(2) P&W per<strong>for</strong>ms UT inspection of the 1 st machined surface, applies the 2 nd set of machining<br />

passes, and per<strong>for</strong>ms UT inspection of the 2 nd machined surface,<br />

(3) GE acquires profiles of the 2 nd machined surface, and per<strong>for</strong>ms UT inspection of the 2 nd<br />

machined surface,<br />

(4) Honeywell per<strong>for</strong>ms UT inspection of the 2 nd surface, applies the 3 rd set of machining<br />

grooves, and per<strong>for</strong>ms UT inspection of the 3 rd surface,<br />

(5) GE per<strong>for</strong>ms UT inspection of the 3 rd surface finish, and acquires profiles of the 3 rd<br />

machined surface,<br />

(6) Data is analyzed by the team to relate surface finish conditions to near surface resolution<br />

and to signal to noise ratio. Hopefully, a relationship can also be established between<br />

feedrate and front surface signal ringdown.<br />

Some of the details that are yet to be worked out include identification of the transducers to be<br />

used, which feedrates to use, what is the minimum UT data that should be collected at each<br />

site, and how should the machinists requirements be controlled/recorded.<br />

Beam Properties<br />

A goal of subtask 1.3.2 is to design an inspection scheme that achieves #1/2 FBH sensitivity in Ti<br />

<strong>for</strong>gings. When designing a zoning scheme and choosing transducers, one of the key steps is to<br />

define the requirements of the ultrasonic pulse volume. It has been shown theoretically and verified<br />

experimentally that the signal-to-noise (S/N) ratio is approximately inversely proportional to the<br />

square root of the pulse volume. Thus, to meet the subtask goal, one needs to define the<br />

restrictions on the pulse volume that provide acceptable S/N ratios <strong>for</strong> a #1/2 FBH inspection.<br />

During the previous and current quarters such data was acquired at GE-QTC. Signal-to-peak-noise<br />

ratios were measured using several transducers with different focal characteristics to achieve a<br />

wide range of pulse-volume values. The measurements were per<strong>for</strong>med on the highest noise<br />

“property” coupons from each OEM’s Ti 6-4 <strong>for</strong>ging. Two of the three coupons had arrays of #1<br />

FBH drilled into them, and one of the holes in the PW coupon served as a reference against which<br />

peak noise values were measured. The data acquired using an F6 transducer with the beam<br />

focused on the FBHs is shown at Figure 3. The gain was selected such that the response from<br />

#1/2 FBH would be at 80% Full Screen Height (FSH). The peak noise was measured <strong>for</strong> each of<br />

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the high-noise coupons shown in the figure, resulting in 30.6%, 43.0% and 36% <strong>for</strong> the PW, HW<br />

and GE coupons respectively.<br />

In addition to the S/N measurements, sonic pulse volumes were also measured. First, the –6dB<br />

beam diameter at the FBH depth was determined from a fine increment C-scan of the reference<br />

hole in the PW coupon. Figure 4 illustrates the beam diameter determination <strong>for</strong> the same<br />

example, leading to a value of 39.4 mils. Secondly, as illustrated in Figure 5, the pulse duration<br />

was measured by finding the –6 dB points <strong>for</strong> the envelope function of the rectified FBH echo, and<br />

this duration was translated to a pulse length in metal. For the case shown, the pulse length was<br />

36.7 mils, leading to a measured pulse volume of (π/4)(39.4 mils) 2 (36.7mils) = 44,600 cubic mils.<br />

Peak noise vs. pulse volume <strong>for</strong> all measurements is summarized in Figure 6.<br />

PW8<br />

Max. noise<br />

30.6%<br />

HW5<br />

Max noise<br />

43%<br />

GE6<br />

Max. noise<br />

36%<br />

#1/2 FBH ~ 80%<br />

Figure 3. Example of S/N measurements in high-noise <strong>for</strong>ging coupons. Here the FBH holes are<br />

located at the focus of an F6 transducer.<br />

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Figure 4. Beam diameter determination <strong>for</strong> the case of an F6 transducer focused on the FBHs. All<br />

pixels with amplitudes within 6 dB of the maximum are located, and their joint area is measured.<br />

125<br />

F6 - Reference Wave<strong>for</strong>m at Focus<br />

100<br />

F6-0dB-Rect<br />

F6-0dB-Env<br />

Amplitude<br />

75<br />

50<br />

25<br />

0<br />

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7<br />

Microseconds<br />

Figure 5. Pulse duration determination <strong>for</strong> the case of an F6 transducer focused at the FBH depth.<br />

The full width of the envelope at the –6 dB level (50% of maximum) is 0.150 microseconds.<br />

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Peak-Noise-to-Signal (% FSH)<br />

80.0<br />

70.0<br />

60.0<br />

50.0<br />

40.0<br />

30.0<br />

20.0<br />

10.0<br />

0.0<br />

Peak Noise Levels <strong>for</strong><br />

Ti 6-4 High Noise Coupons<br />

#1 FBH at 12 dB above 80%<br />

or at 318.5% on this scale<br />

56.6% (3 dB below 80%)<br />

For each specimen,<br />

Rule-of-Thumb would<br />

predict a straight line<br />

passing thru origin.<br />

Slope dependent on FOM<br />

PW8<br />

HW5<br />

GE6<br />

F5 @ 0dB<br />

F5 @ -3dB<br />

F6 @ 0dB<br />

F6 @ -3dB<br />

F8 @ 0dB<br />

1.6 usec time gate<br />

0 100 200 300<br />

Sqrt (Pulse Volume in cubic mils)<br />

#1/2 FBH<br />

approx at 80%<br />

on this scale.<br />

Figure 6. Peak noise vs. pulse volume measurements per<strong>for</strong>med at GE-QTC. PW8, HW5, and<br />

GE6 denote the highest noise coupons cut from three Ti 6-4 <strong>for</strong>gings.<br />

From Figure 6 one can conclude that choosing the square root of pulse volume to be 240 mils 3/2 or<br />

smaller likely ensures that the peak noise is at least 3 dB below the response from a #1/2 FBH <strong>for</strong><br />

the “noisiest” PW and GE coupons. For this choice, the peak noise in the noisiest HW coupon<br />

would be near to but slightly above the 3dB level. If we assume that the typical pulse duration is<br />

equal to 37 mils (average of measured values) the limitation on the beam diameter would be about<br />

( π × ) ⎤<br />

1/2<br />

240 ⎡⎣4 / 37 ⎦ or about 45 mils. Thus, we estimate that a <strong>for</strong>ging inspection which achieves<br />

#1/2 FBH sensitivity, requires a beam diameter that does not exceed 45 mils at any depth within the<br />

region of interest.<br />

Our next objective was to design an inspection that covered 3.2” of material depth using the<br />

minimum number of zones and ensuring that the beam diameter did not exceed 0.045” at any<br />

depth. We note that 3.2” is the maximum depth required to inspect <strong>for</strong>gings selected <strong>for</strong> this task<br />

from all OEMs. An optimization procedure was employed to determine the maximum zone size and<br />

to design a transducer <strong>for</strong> each zone. First the water path was fixed at 3” with the transducer<br />

diameter and focal length treated as unknown “fitting” parameters. Since the entry surface is flat <strong>for</strong><br />

this exercise, one needs to consider spherically focused probes only.<br />

The beam diameter <strong>for</strong> a given transducer at a given depth was calculated using the Gaussian-<br />

Hermite beam model developed by Iowa State University. It was determined that a 7/16”-wide zone<br />

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size was adequate to support a 0.045” maximal beam diameter. Eight such zones are needed to<br />

cover 3.2” of material and nine zones would cover almost 4”. If the water path were fixed such an<br />

inspection would require nine different transducers. We determined that by varying the water path<br />

one transducer could be used to inspect three zones. Thus, <strong>for</strong> nine zones, three transducers are<br />

required. The parameters of these three probes are listed in Table 1. These are the transducers<br />

originally designed <strong>for</strong> zones 2, 5 and 8 <strong>for</strong> the original inspection scheme that used a fixed 3” water<br />

path. For example, the zone 2 transducer (transducer #1 in Table 1) can also inspect zones 1 and 3<br />

with 4.8” and 1.2” water paths respectively. The final inspection scheme that utilizes three<br />

transducers is presented in Table 2. For this scheme, the on-axis profile (of pressured squared) is<br />

shown in Figure 7. The amplitude of an echo from a small defect is approximately proportional to<br />

pressure squared, so Figure 7 displays the manner in which defect signal amplitude depends on<br />

depth when the proposed scheme is used without a DAC.<br />

On-axis profile <strong>for</strong> 3-transducer 7/16" zone design<br />

Ammplitude<br />

8E-04<br />

7E-04<br />

6E-04<br />

5E-04<br />

4E-04<br />

3E-04<br />

2E-04<br />

1E-04<br />

Zone1<br />

Zone2<br />

Zone3<br />

Zone4<br />

Zone5<br />

Zone6<br />

Zone7<br />

Zone8<br />

Zone9<br />

0E+00<br />

0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0<br />

Depth, in<br />

Figure 7. Predicted on-axis, pressure-squared, beam profile <strong>for</strong> each zone using the 3-transducer<br />

7/16” zone inspection scheme.<br />

The designed optimal transducers have diameters that are not exactly multiples of 1”. However, by<br />

slightly varying the water paths, we believe the inspection can be per<strong>for</strong>med by three F6<br />

transducers with diameters of 1”, 2” and 3”. The 1” diameter F6 transducer is already available,<br />

and the 2” diameter transducer has been ordered. The intent is to test the proposed inspection <strong>for</strong><br />

the first 6 zones during the next quarter. Based on those results the decision will be made on how<br />

to proceed. The use of a DAC to produce a uni<strong>for</strong>m amplitude <strong>for</strong> #1/2 FBHs throughout a zone will<br />

also be investigated in the upcoming quarter.<br />

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Probe<br />

Diameter,<br />

in<br />

Probe<br />

Diameter, cm<br />

Probe Radius<br />

of Curvature, in<br />

Probe Radius<br />

of Curvature,<br />

cm<br />

Transducer #1 0.92 2.34 5.77 14.66<br />

Transducer #2 1.88 4.78 11.22 28.50<br />

Transducer #3 2.80 7.11 16.70 42.42<br />

Table 1. Designed transducer parameters.<br />

7/16" Zone Size, 3-transducer inspection, 4" coverage<br />

Zone From To Transducer # Water path, in Water path, cm<br />

in in<br />

Maximum beam<br />

diameter within<br />

the zone, in<br />

1 0.0000 0.4375 1 4.8 12.19 0.046<br />

2 0.4375 0.8750 1 3.0 7.62 0.045<br />

3 0.8750 1.3125 1 1.2 3.05 0.045<br />

4 1.3125 1.7500 2 4.8 12.19 0.045<br />

5 1.7500 2.1875 2 3.0 7.62 0.044<br />

6 2.1875 2.6250 2 1.2 3.05 0.044<br />

7 2.6250 3.0625 3 4.8 12.19 0.045<br />

8 3.0625 3.5000 3 3.0 7.62 0.044<br />

9 3.5000 3.9375 3 1.2 3.05 0.044<br />

Table 2. Designed inspection scheme to achieve #1/2 FBH sensitivity throughout 4” of Ti 6-4<br />

<strong>for</strong>ging material. The scheme uses three transducers and has nine zones, each 7/16” wide.. Each<br />

transducer covers three zones using three different water paths.<br />

Phased Array Inspection Development<br />

Significant progress was made on the design of the phased array transducer that will be used to<br />

make a test of #1/2 FBH inspection sensitivity with currently available technology. In addition to<br />

discussion at the monthly conference call, a separate conference call was held with a subteam to<br />

discuss the transducer design that is being per<strong>for</strong>med at ISU. The design has progressed to a<br />

state allowing discussion with transducer manufacturers <strong>for</strong> placement of an order by P&W.<br />

Figure 8 shows the most recent design <strong>for</strong> the F6 transducer that will allow focussing to a depth of<br />

3.2 inches as required by the selection of the OEM <strong>for</strong>gings <strong>for</strong> inspection demonstration in this<br />

sub-task. Several modifications of the design have occurred and these were due primarily to<br />

compromises that had to be made from the ideal design to allow <strong>for</strong> the limitations of existing<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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phased array instruments. The design modifications were made after extensive discussions by ISU<br />

with the primary equipment manufacturer.<br />

Figure 8. Schematic drawing of 128 element transducer <strong>for</strong> <strong>for</strong>ging inspection.<br />

P&W has begun the purchase of the transducer with discussions with two manufacturers and will<br />

contact the third know manufacturer of phased array transducers at the start of the next quarter.<br />

Plans (April 1, 2002 – June 30, 2002):<br />

Complete calibration standards.<br />

Order 2” and 3” diameter transducers <strong>for</strong> complete 9 zone inspection.<br />

Continue inspection development with DAC tests <strong>for</strong> individual zones.<br />

Select supplier and place order <strong>for</strong> phased array transducer.<br />

First machining and sonic measurements will be per<strong>for</strong>med <strong>for</strong> the surface finish study samples<br />

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Milestones:<br />

Original<br />

Date<br />

Revised<br />

Date<br />

Description<br />

General Issues<br />

3 months 7 months Finalize selection of OEM <strong>for</strong>ging samples <strong>for</strong><br />

study. CAD files will be provided to ISU <strong>for</strong><br />

generation of sensitivity and coverage maps. (HW,<br />

GE, PW)<br />

3 months Complete design of transducer design model<br />

sample blocks. (GE with support of HW, ISU, PW)<br />

15 months 18 months Complete manufacture of transducer design model<br />

sample blocks. (GE)<br />

24 months Finalize and transition transducer design models to<br />

OEMs. (ISU)<br />

24 months -30 Review fundamental property data from 1.3.1 <strong>for</strong><br />

transducer design optimization. (ISU)<br />

29 months ? Complete model assessment of inspection<br />

sensitivity <strong>for</strong> OEM <strong>for</strong>gings including POD<br />

considerations in cooperation with 3.1.2. (ISU with<br />

support from HW, GE, PW)<br />

Fabrication of calibration standards<br />

15 months Complete calibration standard design. (All)<br />

24 months 36 Complete manufacture of calibration standards.<br />

(GE)<br />

Surface finish studies<br />

36 months<br />

Generation of samples and collection of empirical<br />

data <strong>for</strong> surface finish studies (GE)<br />

39 months<br />

Determine surface finish requirements <strong>for</strong> 1/128”<br />

FBH <strong>for</strong>ging inspection. (All)<br />

42 months<br />

Implementation of empirical results from surface<br />

finish results in UT model tools. (ISU)<br />

42 months<br />

Review curvature correction approaches from 1.3.1<br />

(All)<br />

<strong>Titanium</strong> <strong>for</strong>ging fixed-focus inspection<br />

development<br />

24 months 30 Complete definition of transducer beam properties<br />

required <strong>for</strong> a 1/128” FBH calibration in Ti-6Al-4V.<br />

(ISU, GE, PW and HW)<br />

33 months<br />

Complete any needed new transducers. Establish<br />

commercial sources <strong>for</strong> transducers. (GE)<br />

-------------------------------------------------------------------<br />

44<br />

Complete definition of maximum productivity fixed<br />

focus inspection approach. (GE with support from<br />

PW, AS, ISU)<br />

Status<br />

complete<br />

complete<br />

Task cancelled – results not needed<br />

to resolve transducer model<br />

problems<br />

complete<br />

An additional sample may be<br />

required<br />

Alignment with 3.1.2 will follow<br />

restart of that task<br />

complete<br />

Raw material delivered<br />

Final definition depends on<br />

completion of noise analysis<br />

The second half was moved to 44<br />

months.<br />

39 months Establish fixed focus laboratory testbed. (GE)<br />

40 months Finalize scan plans <strong>for</strong> OEM <strong>for</strong>gings. (All)<br />

42 months Conduct laboratory inspection of high sensitivity<br />

zoned inspection on six OEM <strong>for</strong>gings. Provide<br />

data to 3.1.2 <strong>for</strong> model validation and POD<br />

prediction. (All)<br />

43 months Laboratory demonstration of fixed focus high<br />

iti it f i i ti f fl t f<br />

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Original<br />

Date<br />

Revised<br />

Date<br />

Description<br />

sensitivity <strong>for</strong>ging inspection <strong>for</strong> flat surfaces.<br />

44 months Complete definition of maximum productivity fixed<br />

focus inspection approach (GE with support from<br />

PW, HW, ISU)<br />

<strong>Titanium</strong> <strong>for</strong>ging phased array inspection<br />

development<br />

36 months Complete evaluation of up to 3 candidate phased<br />

inspection techniques. (All)<br />

37 months Review results and select phased array inspection<br />

technique to pursue. (All)<br />

39 months Establish phased array inspection technique and<br />

laboratory testbed. (TBD)<br />

40 months Complete modified phased array inspection scan<br />

plans <strong>for</strong> OEM <strong>for</strong>gings. (All)<br />

42 months Conduct laboratory inspection of six OEM <strong>for</strong>gings<br />

using phased array approach as required. Provide<br />

data to 3.1.2 <strong>for</strong> model validation and POD<br />

prediction. (All)<br />

43 months Laboratory demonstration of high sensitivity <strong>for</strong>ging<br />

inspection utilizing an alternative technique <strong>for</strong><br />

curved entry surface inspection.<br />

Factory <strong>Evaluation</strong> / Demonstration<br />

43 months Review results of laboratory inspections per<strong>for</strong>med<br />

with fixed focus and the alternative technique.<br />

Define high sensitivity <strong>for</strong>ging inspection <strong>for</strong> factory<br />

demonstration. (All)<br />

49 months Establish production testbed <strong>for</strong> high sensitivity<br />

<strong>for</strong>ging inspection. (GE with support from PW and<br />

AS)<br />

49 months Finalize scan plans <strong>for</strong> OEM <strong>for</strong>gings. (All)<br />

57 months Complete production inspection <strong>for</strong> 30 <strong>for</strong>gings (10<br />

from each OEM). Provide data to 3.1.2 <strong>for</strong> model<br />

validation and POD prediction. (All)<br />

57 months Factory demonstration of high sensitivity <strong>for</strong>ging<br />

inspection including digital C-scan data acquisition<br />

per<strong>for</strong>med on 30 separate <strong>for</strong>gings.<br />

59 months Evaluate indication finds from production test,<br />

document results. Provide data to 3.1.2 <strong>for</strong> model<br />

validation and POD prediction. (All)<br />

60 months Report of laboratory and factory evaluations<br />

including sensitivity data <strong>for</strong> use by the Inspection<br />

System Capability Working Group and cost<br />

comparisons <strong>for</strong> the different inspection<br />

approaches.<br />

Status<br />

This milestone was separated from a<br />

33 month milestone with multiple<br />

tasks.<br />

Deliverables:<br />

Transducer design models (both fixed-focus and phased array) transitioned to the OEMs.<br />

Calibration standards and transducers as needed.<br />

Laboratory demonstration of fixed focus high sensitivity <strong>for</strong>ging inspection <strong>for</strong> flat surfaces.<br />

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Laboratory demonstration of high sensitivity <strong>for</strong>ging inspection utilizing an alternative technique <strong>for</strong><br />

curved entry surface inspection.<br />

Factory demonstration of high sensitivity <strong>for</strong>ging inspection including digital C-scan data acquisition<br />

per<strong>for</strong>med on 30 separate <strong>for</strong>gings.<br />

Report of laboratory and factory evaluations including sensitivity data <strong>for</strong> use by the Inspection<br />

Systems Capability Working Group and cost comparisons <strong>for</strong> the different inspection approaches.<br />

Metrics:<br />

Demonstration of 1/128” (#½) FBH sensitivity inspection with digital C-scan data acquisition and<br />

SNR-based reject criterion <strong>for</strong> representative titanium <strong>for</strong>gings using zoned inspection approach<br />

with inspection speed comparable to current inspections.<br />

Major Accomplishments and Significant Interactions:<br />

Date<br />

June 16, 1999<br />

Description<br />

Technical Kick-off Meeting in West Palm Beach, FL<br />

Publications and Presentations:<br />

Date<br />

Description<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Task 2:<br />

Task 2.1:<br />

Subtask 2.1.1:<br />

Inservice Inspection<br />

Inspection Development <strong>for</strong><br />

Rotating Components<br />

Development of UT Capability<br />

<strong>for</strong> Inservice Inspection<br />

Team Members:<br />

HW: Prasanna Karpur, Andy Kinney<br />

ISU: Tim Gray, Bruce Thompson<br />

GE: Tony Mellors<br />

PW: John Lively, Dave Raulerson, Rob<br />

Stephan, Jeff Umbach, Dave Bryson, Anne<br />

D’Orvilliers<br />

Program status: June 15, 1999. The FAA contracting office suspended new work on this subtask,<br />

effective March 16, 2000. All milestones were significantly effected. Deliverables originally<br />

proposed will not be provided unless/until FAA direction to resume ef<strong>for</strong>t on this task.<br />

Task 2:<br />

Task 2.1:<br />

Subtask 2.1.2:<br />

Inservice Inspection<br />

Inspection Development <strong>for</strong><br />

Rotating Components<br />

Eddy Current Probe <strong>Evaluation</strong><br />

and Implementation<br />

Team Members:<br />

HW: A. Kinney, T. Duffy<br />

GE: W. Bantz, J. Collins, D. Copley, B.<br />

McKnight, T. Mellors, S. Nath<br />

ISU: L. Brasche, N. Nakagawa<br />

PW: D. Raulerson, J. Lively, R. Stephan<br />

Program status: June 15, 1999. The FAA contracting office suspended new work on this subtask,<br />

effective March 16, 2000. All milestones were significantly effected. Deliverables originally<br />

proposed will not be provided unless/until FAA direction to resume ef<strong>for</strong>t on this task.<br />

Task 2:<br />

Task 2.2:<br />

Subtask 2.2.1:<br />

Inservice Inspection<br />

Inspection Development<br />

Transitions to Airline<br />

Maintenance<br />

Application of ETC Tools in<br />

Overhaul Shops - EC Scanning<br />

Team Members:<br />

HW: Jim Hawkins, Jim Ohm, Tim Duffy,<br />

Andy Kinney<br />

ISU: L. Brasche, N. Nakagawa<br />

GE: Julia Collins, Tony Mellors, Shridhar<br />

Nath<br />

PW: Kevin Smith, Dave Bryson, Anne<br />

D’Orvilliers, Rob Stephan, Dave Raulerson,<br />

John Lively<br />

Program status: June 15, 1999. The FAA contracting office suspended new work on this subtask,<br />

effective March 16, 2000. All milestones were significantly effected. Deliverables originally<br />

proposed will not be provided unless/until FAA direction to resume ef<strong>for</strong>t on this task.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Task 2:<br />

Task 2.2<br />

Subtask 2.2.2:<br />

Inservice Inspection<br />

Inspection Development<br />

Transitions to Airline<br />

Maintenance<br />

High Speed Bolthole Eddy<br />

Current Scanning<br />

Team Members:<br />

HW: Tim Duffy, Jim Ohm, Waled Hassan<br />

ISU: Lisa Brasche<br />

GE: Tony Mellors, Shridhar Nath, Jon<br />

Bartos<br />

PW: Kevin Smith, Dave Bryson, Rob<br />

Stephan<br />

Students: None<br />

Program initiation date: June 15, 1999<br />

Objectives:<br />

To develop common fixtures to reduce inspection variables and arrive at a standardized inspection<br />

technique.<br />

To measure the process capability.<br />

To utilize this in<strong>for</strong>mation to develop an industry best practice document.<br />

Approach:<br />

<strong>Evaluation</strong> of Existing Processes: Ef<strong>for</strong>ts will concentrate on process improvements <strong>for</strong> and<br />

standardization of high speed bolt hole scanning. A detailed evaluation of existing OEM inspection<br />

processes and needs will be conducted. Current equipment and tooling will be analyzed to provide<br />

a baseline of existing inspection processes and their limitations. The data will be analyzed <strong>for</strong><br />

potential process improvements and identification of common tooling approaches. A survey of<br />

available commercial tooling will be included as part of the assessment and included in the baseline<br />

as possible.<br />

Development of Common Tooling: The ef<strong>for</strong>ts will then be focused on the detailed design and<br />

fabrication of common tooling with an emphasis placed on variability reduction and defect<br />

detectability improvements. An inspection demonstration will be conducted on a sample set of<br />

hardware from each of the industrial members <strong>for</strong> validation of process development. A<br />

comparison to the baseline data will be made. Working with task 3.1.3 an evaluation of the process<br />

POD will be conducted on existing bolt hole reliability specimens.<br />

Development of Common Process: A common inspection technique and best practices document<br />

will be developed. Currently AS4787, Eddy Current Inspection of Circular Holes in Nonferrous<br />

Metallic Aircraft <strong>Engine</strong> Hardware, serves as a standard <strong>for</strong> hole inspection. This document will be<br />

revised to reflect the results of the ETC ef<strong>for</strong>t. Recommendations <strong>for</strong> equipment improvements will<br />

be supplied to vendors and implications <strong>for</strong> further study will be provided to the FAA.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Objective/Approach Amendments: Objective and approach remain as originally proposed in July<br />

1998.<br />

Progress (January 1, 2002 – March 31, 2002):<br />

The subtask was realigned during this quarter. A revised plan was generated and is reflected in the<br />

“Milestones” section below. The technical team supporting this subtask held several conference<br />

calls leading to significant technical progress . The following represents a summary of the<br />

accomplishments:<br />

Bolt hole Simulator Design: The design of the bolt hole simulator is complete. This piece will be<br />

used to precisely fixture round bolt hole specimens (see Figure 1) in a circular layout as they would<br />

be <strong>for</strong> a typical rotating engine component. This piece will be able to hold twenty-five 1.875”<br />

diameter specimens having a 0.250-inch thickness. The bolt hole diameter within these circular<br />

specimens will be 0.460 inches. The layout aligns the specimens in a precise circular pattern with<br />

the bolt holes within 0.002 inches of geometric center. When specimens are aligned, they can be<br />

locked into position to prevent rotation and lift-out during scanning.<br />

Probe Translation Device: A preliminary design is complete. This device is required to precisely<br />

position and translate a rotating eddy current probe through boltholes of various diameters in critical<br />

engine rotating hardware. These probes will be mounted to off-the-shelf high-speed eddy current<br />

bolt hole rotating drivers and are used <strong>for</strong> detecting cracks along the length of the bolt holes. There<br />

are various probe-rotating drivers available and the device is designed to be able<br />

Figure 1. FML100146 Eddy Current Bolt hole Crack Specimen Design.<br />

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to firmly fixture and work with a number of these rotating drivers. Schematics or actual rotating<br />

drivers were made available <strong>for</strong> this design. The probe translation device will be adaptable to<br />

different engine part numbers. Figure 2 shows a schematic of the preliminary design of the probe<br />

translation device. The following requirements were imposed during the design process:<br />

1. Fixtured alignment to control wobble of probe while translating through a part<br />

2. Fine X-Y plane adjustment to center probe within bolt hole diameter<br />

3. Machine control of probe travel through bolt holes by means of selectable fixed transverse<br />

speeds of zero, 0.100, and 0.200 inches/second in a helical scan pattern<br />

4. Rapid adjustable automatic translation retraction to a start next scan position<br />

5. Scan limit switch to prevent excess travel of probe<br />

6. Minimum of three inches of probe translation travel<br />

7. Slip clutch to prevent burn-out of translation motor<br />

8. Use of exchangeable bolt-on adapter plates <strong>for</strong> fit to specific parts/bolt hole patterns<br />

9. Adaptability to Uniwest probe rotating driver, Roman Elotest, Foerster, Zetec, etc as provided.<br />

10. There can be no electrical interference caused the probe translation device on the eddy current<br />

inspection process including data acquisition.<br />

11. Manufacturing cost less than $10,000<br />

Part Adapter Plate: In order to adapt the proposed bolt hole scanning system design to various<br />

parts and <strong>for</strong> the inspection of each hole, the ability to manually lift the instrument and secure it <strong>for</strong><br />

the next bolt hole must be present. This will be accomplished through an exchangeable adapter<br />

plate designed <strong>for</strong> that purpose. These adapter plates shall bolt to the bottom of the translation<br />

device. To precisely adjust the eddy-current probe within a bolt hole, a fine X-Y adjustment that can<br />

also lock the probe into the correct position within the hole is provided. Figure 3 shows an example<br />

of an adapter plate that is currently in use in production. Our plan includes the design and<br />

manufacturing of two such adapter plates <strong>for</strong> pre-selected industry applications. The selection of<br />

these applications in underway and once finalized the design of these adapter plates will be<br />

completed.<br />

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Figure 2. A preliminary design of the probe translation device.<br />

Figure 3. An example of an adapter plate that is currently in use.<br />

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Plans (April 1, 2002 – June 30, 2002):<br />

• Finalize the design of the probe translation device and complete manufacture.<br />

• Identify two industry bolt hole configurations <strong>for</strong> the inspection assessment study and design<br />

and manufacture the needed adapter plates.<br />

• Manufacture the part simulator fixture<br />

• Obtain a documented and larger population POD specimen set <strong>for</strong> use in tooling assessment<br />

Milestones:<br />

Original<br />

Revised<br />

Description<br />

Status<br />

Date<br />

Date<br />

0 –12<br />

months<br />

Evaluate existing OEM techniques. (All)<br />

Complete<br />

12 –30<br />

months<br />

12-32<br />

months<br />

Develop common tooling. (Honeywell with support<br />

from GE, PW)<br />

In progress<br />

• Define common tooling requirements<br />

• Design and build prototype tooling<br />

• Design tests <strong>for</strong> tooling assessment<br />

Per<strong>for</strong>m tooling assessment<br />

30-36<br />

months<br />

32-38<br />

months<br />

Develop common inspection technique. (Honeywell<br />

with support from GE, PW)<br />

•Per<strong>for</strong>m demonstration on sample hardware<br />

36 –48<br />

months<br />

38-48<br />

months<br />

Determine improved process capability (Honeywell<br />

with support from GE, PW)<br />

• Evaluate process PODs<br />

• Revise AS4787<br />

Deliverables:<br />

Common fixture <strong>for</strong> reduced inspection variability.<br />

Common high speed bolt hole eddy current inspection technique through revision of AS4787.<br />

Report of process capability and reliability.<br />

Metric:<br />

Common practices and tooling required to achieve a demonstrated 30 mil crack detectability and<br />

4:1 signal-to-noise in a common bolt hole geometry<br />

Major Accomplishments and Significant Interactions:<br />

Date<br />

June 17, 1999<br />

March 22, 2000<br />

Description<br />

Technical Kick-off Meeting at West Palm Beach, FL<br />

TOGAA review at Honeywell in Phoenix, AZ<br />

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Publications and Presentations:<br />

Date<br />

Description<br />

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Project 2:<br />

Task 2.2:<br />

Subtask 2.2.3:<br />

Inservice Inspection<br />

Inspection Development<br />

Transitions to Airline<br />

Maintenance<br />

<strong>Engine</strong>ering Studies of Cleaning<br />

and Drying Process in<br />

Preparation <strong>for</strong> FPI<br />

Team Members:<br />

HW: Andy Kinney, James Hawkins, Tim<br />

Duffy<br />

ISU: Brian Larson, Rick Lopez, Lisa<br />

Brasche<br />

GE: Terry Kessler, Charlie Loux, Jon<br />

Bartos<br />

PW: Anne D'Orvilliers, Brian MacCracken,<br />

Kevin Smith, Jeff Stevens, John Lively<br />

Students: S. Gorman, L. Rohrhey, and Y. Wang<br />

Program initiation date: February 7, 2000<br />

Objectives:<br />

• To establish a quantifiable measure of cleanliness including the minimum condition to allow<br />

effective inspection processing.<br />

• To establish the effect of local etching on detectability and provide guidance on best practices<br />

<strong>for</strong> removal of local surface damage from FOD and other surface anomalies.<br />

• To determine the effect of chemical cleaning, mechanical cleaning, and drying processes on the<br />

detectability of LCF cracks in titanium and nickel alloys that would be typical in field run<br />

hardware.<br />

• To update existing specifications to reflect the improved processes and provide best practices<br />

documents <strong>for</strong> use by the OEMs and airlines.<br />

Approach:<br />

The overall approach to the FPI studies is shown in the following flowchart with details provided in<br />

the text that follows.<br />

Literature and Industry Survey: The effects of cleanliness, cleaning method, and drying method on<br />

penetrant inspectability will be evaluated. As a first step, a review of the literature related to FPI<br />

processes and cleaning and drying methods will be conducted. Literature related to cleaning<br />

processes as well as NDE processes will be reviewed. Existing CASR literature review data will<br />

serve as a starting point.<br />

A survey of current practices used by the OEMs, airlines, and third party maintenance shops will be<br />

conducted to determine the existing “state of the practice”. Potential partners will be identified <strong>for</strong><br />

participation in the follow on studies on fielded hardware. A team meeting will be held to identify<br />

the cleaning methods and drying methods to be studied and the contaminants of concern. Other<br />

organizations not participating in ETC will be invited to attend the meeting and coordination with<br />

other relevant programs will be maintained. A design of experiments approach will be considered<br />

in order to optimize the use of the results. A set of 40 specimens, 20 titanium and 20 nickel will be<br />

generated by CASR staff.<br />

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Survey of common<br />

practices (industry)<br />

Survey of existing data<br />

(literature)<br />

Identify drying<br />

methods <strong>for</strong> study<br />

Identify cleaning<br />

methods <strong>for</strong> study<br />

Identify typical<br />

contaminants of<br />

concern<br />

Define and acquire<br />

crack samples <strong>for</strong><br />

baseline studies<br />

Identify engine run<br />

hardware <strong>for</strong> use<br />

in cleanability<br />

studies<br />

Study to detemine<br />

"how clean is<br />

clean"; "how clean<br />

is needed"<br />

Use metrics<br />

established<br />

by<br />

MacCracken/<br />

Kessler<br />

Assess methods<br />

at airline shops;<br />

compare against<br />

baseline sample<br />

Matrix of cleaning<br />

process effectivity<br />

vs contaminant<br />

<strong>Engine</strong>ering study<br />

to determine effect<br />

of drying method<br />

on detectability<br />

(t and T) <strong>for</strong><br />

oven drying<br />

flash drying and air<br />

drying<br />

Utilize lcf samples<br />

to extent possible;<br />

study on<br />

components<br />

required to<br />

address thermal<br />

mass issues<br />

<strong>Engine</strong>ering study<br />

to determine effect<br />

of cleaning on<br />

detectability<br />

Potential variables:<br />

aqueous degreasers<br />

ultrasonic cleaners<br />

plastic media blast<br />

water jet blast<br />

solvent cleaners<br />

etching processes (local only)<br />

chemical cleaners<br />

vapor degreasers<br />

Utilize lcf crack samples to<br />

assess detectability; effect of<br />

cleaner on background, wetting<br />

characteristics, residual stress,<br />

etc.<br />

Matrix of drying<br />

process vs<br />

detectability<br />

Matrix of cleaning<br />

process vs<br />

detectability<br />

Develop best<br />

practices<br />

document and<br />

necessary spec<br />

changes<br />

Figure 1. Program Plan <strong>for</strong> “<strong>Engine</strong>ering Studies of Cleaning and Drying Process in Preparation <strong>for</strong><br />

FPI”.<br />

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Assessment of Cleanliness on Inspectability: A major concern <strong>for</strong> the inspector is the cleanliness of<br />

the part to be inspected and the impact that surface condition will have on detectability, with the<br />

question often being asked, “How clean is clean?” Some ef<strong>for</strong>t has been undertaken to provide<br />

guidance in this area in the most recent version of SAS 2647. An engineering study will be<br />

per<strong>for</strong>med to assess the utility of these metrics through on-site evaluation at airline shops using<br />

field run hardware. LCF blocks will be used to establish a baseline and <strong>for</strong> comparison across test<br />

sites. A matrix will be generated that establishes the effectiveness of various cleaning methods in<br />

removing general classes of typical contaminants. It is expected that various operational<br />

conditions, types of cleaner equipment/systems, cleaner type, cleaner concentration, process<br />

parameters, and alloy types will be considered. Appropriate data will be gathered on the field<br />

systems used in the study such as chemical concentration of the cleaning solutions, temperature,<br />

etc to allow comparison between systems and to approved process parameters. Guidance on the<br />

effect of cleanliness on penetrant inspectability will be provided in the <strong>for</strong>m of a cleanliness matrix<br />

that summarizes cleaning process effectivity <strong>for</strong> various contaminants.<br />

Assessment of the Effect of Cleaning Method on Inspectability: Given a definition of the required<br />

cleanliness from the ef<strong>for</strong>t above, an engineering study to arrive at the effect of cleaning methods<br />

on detectability will be per<strong>for</strong>med using LCF blocks. Potential cleaning methods to be considered<br />

include<br />

♦ aqueous degreasers<br />

♦ ultrasonic cleaners<br />

♦ plastic media blast<br />

♦ water jet blast<br />

♦ solvent cleaners<br />

♦ etching processes (local only)<br />

♦ chemical cleaners <strong>for</strong> both Ti and Ni<br />

♦ vapor degreasers<br />

Local etching of FOD and other local anomalies to remove smeared metal and improve crack<br />

detectability is a common practice. An evaluation to define optimal local etching practices will be<br />

per<strong>for</strong>med. Parameters within the global cleaning process which may need to be considered<br />

consist of degree of agitation, time spent in tanks, degree of concentration and post-clean,<br />

particulate size and content, pressure, etc. The effect of cleaning methods on background, wetting<br />

characteristics, residual stress, and crack detectability will be assessed. A matrix will be generated<br />

which establishes the detectability as a function of the selected cleaning processes and provided as<br />

a final product of the study.<br />

Assessment of the Drying Method on Inspectability: Once the part is appropriately cleaned, it is<br />

essential that all fluids be removed from any rejectable defects such that penetrant solution can<br />

easily enter the flaw. Definition and adherence to appropriate drying times and temperatures is<br />

critical to the overall effectiveness of the FPI process. An engineering study will be per<strong>for</strong>med to<br />

establish the optimal drying process parameters. Potential drying methods to be considered<br />

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include air drying, oven drying, and flash drying. Initial studies will utilize lcf blocks with final<br />

recommendations to be based on actual engine hardware. A matrix that defines the effect of drying<br />

parameters on detectability will be generated.<br />

Development of Best Practices Document: The final stage of the work will be generation of a best<br />

practices document that provides guidance to the OEMs and airlines and will allow <strong>for</strong> any<br />

necessary specification changes. An assessment will be made of the need <strong>for</strong> further work such as<br />

a <strong>for</strong>mal POD study and recommendations provided.<br />

Objective/Approach Amendments: Objective and approach were discussed and details were<br />

added to the approach in the February 2000 kick-off meeting.<br />

Progress (January 1, 2002 – March 31, 2002):<br />

The third and final testing session <strong>for</strong> this study was held at Delta February 4-7. Honeywell<br />

completed the “baked on” contamination process which lead to oxidation/scale, soot, and<br />

coke/varnish as specified by the team. All planned cleaning methods of the baked on<br />

contamination was completed at the Delta Airlines engine shop and at Northwest Airlines (wet-glass<br />

beading) both in Atlanta.<br />

Additionally, follow-up studies identified from results of the first cleaning run which occurred in<br />

October at Delta were made. These include additional samples with penetrating oil contamination.<br />

Some specimens were involved in various other cleaning trials including the use of vapor<br />

degreasing, acidic scale conditioner, acetone and permanganate.<br />

Part two of the cleaning studies at Delta included evaluation of the cleaning methods listed below<br />

<strong>for</strong> each of the contaminate types. In cases where unsatisfactory cleaning results were found <strong>for</strong> a<br />

particular contaminate/cleaning method combination, as determined by photometer brightness<br />

numbers, the sample was then cleaned by another method.<br />

• Oxidation of nickel specimens<br />

C3 – Alkaline De-rust Solution A<br />

C7a – Ultrasonic w/Alkaline De-rust Solution B<br />

B2 – Wet Glass Bead<br />

B5 – Aluminum Oxide 500 grit<br />

• Oxidation and scale of titanium specimens<br />

C2a – Alkaline De-rust Solution A<br />

C2b – Alkaline De-rust Solution B<br />

B2 – Wet Glass Bead<br />

B5 – Aluminum Oxide 500 grit<br />

• Soot on titanium<br />

C1 – Aqueous degreaser<br />

C2a – Alkaline De-rust Solution A<br />

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C2b – Alkaline De-rust Solution B<br />

C5 – Alkaline Gel Cleaner<br />

B1– Plastic media blast (at 80 and 40 psi) <strong>for</strong> 30 sec<br />

• Soot on nickel-based specimens<br />

C3 – Alkaline De-rust Solution A<br />

C7a – Ultrasonic w/Alkaline De-rust Solution B<br />

B1– Plastic media blast (at 80 and 40 psi) <strong>for</strong> 30 sec<br />

• Varnish/Coke on nickel-based specimens<br />

C3 – Alkaline De-rust Solution A<br />

C5 – Alkaline Gel Cleaner<br />

C7a – Ultrasonic w/Alkaline De-rust Solution B<br />

B1– Plastic media blast (40 psi) <strong>for</strong> 30 sec<br />

Visually, almost all of the specimens were evaluated as having a surface that appeared to be clean<br />

following the initial cleaning attempt. At the very least, two out of the three specimens <strong>for</strong> a<br />

particular contaminate/cleaning method combination were assessed as visually clean. However,<br />

crack crevice cleaning as evaluated by brightness was a different story. Many of the specimens<br />

showed reduced brightness with respect to baseline brightness and in some cases no indication<br />

could be discerned either by photometer or by a more sensitive though qualitative visual black light<br />

examination.<br />

The C4 four-step alkaline process <strong>for</strong> nickel-based materials (alkaline rust remover, acidic scale<br />

conditioner, alkaline permanganate, alkaline rust remover) proved successful <strong>for</strong> removing all three<br />

contaminants from the cracks and restoring much of the baseline fluorescent brightness. It was<br />

somewhat less effective on nickel oxidation. However, no cleaning process <strong>for</strong> titanium proved as<br />

effective as the four-step <strong>for</strong> nickel-based materials.<br />

For removal of oxidation on titanium, the cleaning difficulty was partly due to the higher degree of<br />

oxidation with to the nickel-based material. Oxidation on the titanium was estimated to be<br />

equivalent to 5,000 hours of engine run. It represents a heavy amount of oxidation that is now<br />

being seen on some of the hotter running titanium components.<br />

In addition, the method <strong>for</strong> producing soot by suspending specimens, crack opening down, over hot<br />

oil produced a blackened surface having somewhat of a sheen rather than a matte black finish.<br />

This condition would more likely be found on turbine engine hot section parts, but probably not on<br />

titanium cold section parts. The contaminant condition proved more resistant to some of the<br />

cleaning methods than typical soot.<br />

There were sometimes apparent inconsistent results <strong>for</strong> a particular contaminant/cleaning method<br />

that may be related to three different crack sizes being used. That is, perhaps a chemical cleaning<br />

method is more effective at removal of soot on a large, open crack than on a small, tight crack or<br />

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aluminum oxide blasting is concealing the tighter cracks more so than the open cracks. There<strong>for</strong>e<br />

the crack morphology is being considered in interpretation of the results.<br />

Some of the preliminary observations or conclusions include:<br />

• Vapor degreasing and aqueous cleaning both appear to be effective <strong>for</strong> removing oil.<br />

• Alkaline derust is not effective on oxidation/scale, or soot on Ti-6-4. Short soak, high or low<br />

concentrations do not effectively remove penetrating oil in Ti-6-4. Alkaline residue may reduce<br />

fluorescent penetrant brightness.<br />

• Alkaline gel was not an effective cleaning on either Ti-6-4 or INCO 718.<br />

• Wet glass-beading lead to loss of 4 of 6 cracks and significant brightness reductions in the<br />

other two cracks.<br />

• Aluminum oxide 500 mesh grit may be more suitable <strong>for</strong> critical rotating parts. Surface damage<br />

appears to occur <strong>for</strong> 240 and 320 mesh grit sizes.<br />

UVA<br />

Oct<br />

BL<br />

00-067<br />

UVA<br />

Oxidat.<br />

& scale<br />

An example of the data summaries that are being generated is shown above <strong>for</strong> sample 01-037.<br />

The in<strong>for</strong>mation includes the original optical micrograph <strong>for</strong> the sample, three UVA indications taken<br />

at different times and under different conditions at Delta and the optical micrograph after<br />

processing. This particular sample underwent walnut shell media blast which has been coded as<br />

the “B6” method. The BT values are brightness readings. Note that <strong>for</strong> this sample the brightness<br />

decreased from the baseline run after use of the walnut shell blast. However, subsequent<br />

processing through ultrasonic agitation in an acetone bath returned the brightness to levels near the<br />

original baseline. This indicates that some media may have remained in the crack immediately<br />

after blasting which was removed by the subsequent “fluid processing”. Consideration is being<br />

given to recommending that a water wash step be added after all mechanical blasting operations<br />

used to clean parts.<br />

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The etch study was repeated during this visit at Delta <strong>for</strong> both Ti-6-4 and INCO 718. There were<br />

difficulties in blending the Ti-6-4 and the INCO 178 etch specimens to acceptable conditions <strong>for</strong><br />

processing through the etchant procedures. It may be somewhat reassuring to note that the cracks<br />

were difficult to smear. It was also difficult to determine visually if smearing was sufficient to close<br />

the cracks as FPI revealed. The etching of Ti-6-4 had a better effect than etching of INCO718,<br />

however crack detectability was significantly lower than the baseline <strong>for</strong> all samples. The report<br />

summarizing this study is being prepared.<br />

A considerable volume of data has been generated on this program with analysis underway. A<br />

meeting to review the data and conclusions is planned <strong>for</strong> early April. Final report sections were<br />

assigned and drafts have been or are being completed.<br />

Plans (April 1, 2002 – June 30, 2002):<br />

Complete accounting of all results including crack length measurements from the UV photos,<br />

organizing UV images, verification of brightness results and crack lengths and spreadsheet results<br />

by cleaning method.<br />

A two-day wrap up meeting is scheduled <strong>for</strong> April 7-8 in Phoenix. This will provide an opportunity to<br />

evaluate all cleaning results and document conclusions and recommendations <strong>for</strong> follow-on work.<br />

Further evaluation of some selected specimens with diminished/no brightness will include scanning<br />

electron microscopy, a hot water rinse study, and additional fatigue of several specimens to break<br />

open closed or smeared cracks followed by penetrant testing.<br />

Report preparation is underway with a draft to be provided in the next quarter.<br />

Milestones:<br />

Original<br />

Date<br />

Revised<br />

Date<br />

Description<br />

4/00 Complete literature survey. Complete industry<br />

survey of common practices used in cleaning and<br />

drying. (All)<br />

5/00 Identify cleaning and drying methods and typical<br />

contaminants of concern <strong>for</strong> study in the problem.<br />

6/00 Establish experimental parameters <strong>for</strong> engineering<br />

studies.<br />

6/00 Define necessary crack samples and determine<br />

need <strong>for</strong> fabrication<br />

6/00 Establish partnerships with airlines to per<strong>for</strong>m onsite<br />

evaluation of cleaning methods.<br />

8/00 Initiate study to define optimal local etching<br />

practices.<br />

9/00 Present status update at ATA September NDT<br />

meeting in San Francisco. (This along with<br />

telephone survey replaces proposal milestone <strong>for</strong><br />

month 3. Industry workshop to identify cleaning<br />

and drying methods and typical contaminants of<br />

concern <strong>for</strong> study in the program.)<br />

12/00 Initiate combined Effects of Cleanliness Study and<br />

Cleanability & Drying Studies.<br />

12/00 Complete local etching practices study and<br />

generate guidance document.<br />

Status<br />

Completed 4/28/00<br />

Completed 5/8/00<br />

Completed 5/10/00<br />

Completed 6/28/00<br />

Completed 6/28/00<br />

Etch study initiated with OEM etch<br />

solution comparison 8/16/00<br />

Complete 9/28/00 at 44 th Annual<br />

ATA NDT Forum<br />

Specimen completion 2/01; Delta<br />

overhaul study 6/01<br />

Etching study completed 2/02; report<br />

to be completed 7/02<br />

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Original<br />

Date<br />

Revised<br />

Date<br />

Description<br />

12/01 Complete combine Effects of Cleanliness Study<br />

and Cleanability & Drying Studies and generate<br />

matrix.<br />

Status<br />

Drying studies completed 6/01;<br />

cleaning study complete 2/02<br />

12/01 Initiate best practices document. Final report in progress. Draft to<br />

FAA 7/02.<br />

2/02 Complete best practices document and provide<br />

recommendations <strong>for</strong> further study.<br />

Final report to FAA in 7/02.<br />

Milestone change summary from the Phase II Technical Proposal – Volume I, Task 2.2.3 dated July<br />

10, 1998.<br />

1.) The industry workshop, month 3 (May 2000) milestone was changed in the February 8 kick-off<br />

meeting to a status update to the ATA September 12 meeting in San Francisco. It was felt that<br />

a month 3 milestone could not provide any input that the OEM experts were not already aware<br />

of and also that the subtask had nothing to communicate to the engine overhaul shops at the<br />

time.<br />

2.) The experimental design, month 3 (May 2000) milestone was set back one month to June to<br />

review contaminates, determine cleaning methods and decide what cleaning methods would be<br />

per<strong>for</strong>med on which contaminate type. Until this was determined, the necessary crack samples<br />

could not be determined and so this also was set back one month.<br />

3.) The team decided that since the “Effect of Cleanliness Study” was very similar to the<br />

Cleanability and Drying Studies, and would at least require crack samples called <strong>for</strong> in this<br />

second study, that the studies be combined. The determination of how clean is clean must<br />

include not just surface cleaning, but crack cleanliness also.<br />

4.) Etching practices study will now be completed at the same time as the cleanability and drying<br />

studies since the sample rendered unusable in the cleanliness study can be and will be used <strong>for</strong><br />

the etching practice study.<br />

Deliverables:<br />

Guidance on an optimal process <strong>for</strong> local etching practices.<br />

Specimen sets as required.<br />

Matrices which define the cleaning effectivity vs. typical engine run hardware contaminants,<br />

detectability <strong>for</strong> various cleaning methods, and detectability <strong>for</strong> various drying methods.<br />

Best Practices Document that provides guidance to the OEMs and airlines and will allow <strong>for</strong> any<br />

necessary specification changes.<br />

Recommendations <strong>for</strong> further work such as a <strong>for</strong>mal POD study.<br />

Metrics:<br />

Improved cleaning and drying processes clearly defined <strong>for</strong> implementation by the industry as part<br />

of FPI used in inspection of critical rotating hardware.<br />

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Major Accomplishments and Significant Interactions:<br />

Date<br />

Feb. 7-8, 2000<br />

April 2000<br />

May 2000<br />

June 2000<br />

July 2000<br />

August 2000<br />

September<br />

2000<br />

December<br />

2000<br />

February 2001<br />

June 2001<br />

October 2001<br />

December<br />

2001<br />

February 2002<br />

April 2002<br />

Description<br />

Technical Kick-off meeting.<br />

Completion of literature search and industry survey.<br />

Cleaning and drying methods, and typical contaminants of concern <strong>for</strong> study were identified and<br />

listed.<br />

Experimental parameters were established <strong>for</strong> engineering studies. The matrix of these<br />

parameters are being finalized by the sub-team. Necessary crack samples and need <strong>for</strong><br />

fabrication were defined. A list of these samples are being generated. Established partnerships<br />

with airlines to per<strong>for</strong>m onsite evaluation of cleaning.<br />

Definitions <strong>for</strong> typical titanium and nickel based engine hardware contaminates.<br />

OEM etch solutions compared.<br />

Experimental parameter write-up completed.<br />

Detailed procedure <strong>for</strong> etch study completed.<br />

Sample fabrication complete.<br />

Drying study per<strong>for</strong>med at airline overhaul facility.<br />

Initial cleaning study per<strong>for</strong>med at airline overhaul facility.<br />

“Baked on” contamination of samples completed.<br />

Cleaning study per<strong>for</strong>med at airline overhaul facility. Completed cleaning study data generation.<br />

Team meeting to analyze results and arrive at preliminary conclusions.<br />

Publications and Presentations:<br />

Date<br />

Sept. 28, 2000<br />

Description<br />

Status Update to 44 th Annual Air Transport Association NDT Forum<br />

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Project 3:<br />

Task 3.1:<br />

Subtask 3.1.1:<br />

Inspection Systems Capability<br />

Assessment and Validation<br />

POD Methodology Applications<br />

POD of Ultrasonic Inspection of<br />

Billets<br />

Team Members:<br />

HW: Tim Duffy, Andy Kinney, Waled<br />

Hassan<br />

ISU: Thomas Chiou, Bill Meeker, Bruce<br />

Thompson, Frank Margetan, Tim Gray, Ron<br />

Roberts, Lisa Brasche<br />

GE: Dick Burkel, Bob Gilmore, Jon Bartos,<br />

Mike Keller, Dave Copley, Ed Nieters, Walt<br />

Bantz<br />

PW: Jeff Umbach, Kevin Smith, Taher<br />

Aljundi, Andrei Degtyar<br />

Students: V. Chan<br />

Program initiation date: June 15, 1999; All ef<strong>for</strong>t unrelated to the RDB was stopped on March 17,<br />

2000. On March 14, 2001, guidance was received regarding resumption of the technical work on<br />

subtask 3.1.1 with the initial activity being the revision of program schedules and technical path to<br />

account <strong>for</strong> the RDB results.<br />

Objectives:<br />

• To enhance the ability to estimate the POD of naturally-occurring defects, such as hard-alpha<br />

inclusions in titanium billet, under a variety of inspection scenarios, through identification of a<br />

standard recommended approach <strong>for</strong> adjusting the parameters of the flaw response model to<br />

match the properties of natural-flaw populations.<br />

• To verify that the new POD methodology improves on the accuracy of existent techniques,<br />

provides more in<strong>for</strong>mation such as PFA, and can be reliably applied to circumstances other<br />

than those of the actual experimental measurements as influenced by changing individual<br />

inspection parameters such scan index, transducer properties, etc.<br />

• To verify that the new POD methodology provides sensible predictions using more limited data<br />

than is possible with existent techniques.<br />

• To provide the OEM’s with tools to allow implementation of the new methodology in internal<br />

damage tolerance analyses by increasing the user-friendliness of methodology software and<br />

associated flaw and noise response models.<br />

• To provide the best available estimates of titanium billet POD by means of periodical updates to<br />

existing estimates based on new in<strong>for</strong>mation such as new flaw data and extension of the POD<br />

estimates to a wider range of typical billet diameters.<br />

• To provide to the aircraft engine industry the first estimates and a capability <strong>for</strong> further<br />

estimating POD <strong>for</strong> ultrasonic inspection of nickel billet that is comparable to that provided by<br />

the new SNR-based POD methodology <strong>for</strong> titanium billet.<br />

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• To provide the aircraft engine industry with meaningful assessments of the improvements in<br />

flaw detectability af<strong>for</strong>ded by the ETC inspection developments.<br />

Approach:<br />

The proposed program consists of six major elements, which have been selected in response to the<br />

issues identified above.<br />

Method to Tune Flaw Response Model to the Behavior of Naturally Occurring Flaws: A standard<br />

approach <strong>for</strong> readjusting parameters of the ultrasonic response model to incorporate in<strong>for</strong>mation<br />

about distributions of properties of naturally-occurring flaws will be developed. The advanced flaw<br />

response models that have been developed as a part of ETC-Phase I treat the case of flaws large<br />

with respect to the ultrasonic beam which may not be centered on the beam axis. Procedures to<br />

“tune” the model are now needed, in a fashion analogous to that employed in the R e technique, but<br />

taking advantage of the much greater capabilities of the ISU flaw response models to treat realistic<br />

flaw geometries. During the first four months of the program, team members will jointly develop a<br />

recommended approach to this end. One candidate approach will be to modify the R e method by<br />

replacing the assumed FBH reflector with a cylindrical reflector viewed from the side. The response<br />

of such reflectors is readily treated by the new ISU models and it more closely mimics the overall<br />

shape of naturally occurring hard-alpha inclusions.<br />

Assessment of Success of the new POD/PFA Methodology: The capability of the new<br />

methodology, incorporating ISU flaw response models <strong>for</strong> generating POD and PFA estimates, and<br />

<strong>for</strong> predicting the effects on POD and PFA of many individual inspection parameters, has already<br />

been established qualitatively and quantitatively, using synthetic flaws in test blocks of simple<br />

shape. The Random Defect Block (RDB) will provide a similar test. It was designed to ensure an<br />

adequate distribution of SHA properties to provide meaningful tests of the capability of both<br />

conventional and Multizone inspection systems, while allowing <strong>for</strong> sufficient randomization of the<br />

final choice of SHA parameters (such as length, diameter, percentage nitrogen, skew relative to the<br />

billet axis, and depth below the inspection surface) to avoid an inspector discerning any pattern to<br />

the design. Inspection results (e.g., amplitude, SNR) will be compared with response ranges<br />

predicted from the ISU model to validate the adequacy of the flaw and noise response models to<br />

predict actual experimental data and hence, drive the methodology. A final stage in the validation<br />

process will be a test of the ability of the ISU model to predict the ultrasonic response from the<br />

complex-shaped natural flaws found during the CBS. The results will be analyzed by the team as a<br />

final validation of the Phase I methodology and any necessary modifications will be made. Ef<strong>for</strong>ts<br />

to assess the success of the new methodology will continue through its direct application in other<br />

Phase II work elements.<br />

Improvements and Transfer to the OEMs of the POD/PFA Methodology and Software: For the new<br />

methodology to have full impact on damage tolerant design and management of rotating<br />

components, it is necessary that the tools, i.e., software be in a <strong>for</strong>m readily usable by the OEMs.<br />

These tools will be provided in Phase II. The methodology will be revised as needed based on<br />

results obtained in its application and software will be delivered to the OEMs incorporating those<br />

modifications. As dictated by the results of the RDB and CBS studies, any necessary refinements<br />

will be made in the flaw and noise response models. Included will be the development of numerical<br />

approximations to the predictions of the ultrasonic response models suitable <strong>for</strong> incorporation into<br />

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the methodology. These may be thought of as approximations to the response surfaces which<br />

avoid executing the full flaw response calculation each time the methodology needs to examine a<br />

new case, thereby greatly speeding up the POD calculation process so that it will proceed at a rate<br />

which will be convenient <strong>for</strong> a user operating in an interactive mode. Selected improvements will<br />

also be made in the flaw and noise response models, supported by data generated in Fundamental<br />

Studies ef<strong>for</strong>t and that has the potential to significantly effect POD. Included will be the effects of<br />

microstructure on the ultrasonic beam profile, and hence, on the distributions of flaw responses;<br />

and the effects of tightly focusing the beam on the distribution of noise. In this latter case, it has<br />

been shown that, when the focal spot size approaches the dimensions of the macrostructure, the<br />

noise distribution is significantly modified. Models were developed in Phase I which described<br />

microstructural effects on noise, but a good means of determining the parameters that are inputs to<br />

the models, i.e., of characterizing the material, have yet to be developed. These procedures will be<br />

developed in Phase II. The laws governing the combinations of signal and noise distributions will<br />

be developed. Once known, these promise to greatly reduce the need <strong>for</strong> experimental<br />

measurements of flaw response to exercise the methodology and hence, should significantly<br />

increase its portability. Finally, the effects of variations in calibration response and uncertainties in<br />

the determination of flaw size on the accuracy of POD determination will be investigated, and the<br />

methodology will be modified as needed to accept these results. Results of all of these software<br />

and procedural advances will be integrated and provided to the OEMs <strong>for</strong> their internal use.<br />

POD <strong>for</strong> <strong>Titanium</strong> Billet - Existent/New Data Analysis, and Use of the CBS: Additional in<strong>for</strong>mation<br />

about the properties of flaws in titanium alloys will be collected and reviewed as it becomes<br />

available. Here, particular attention will be placed on the results <strong>for</strong> large diameter billets. This<br />

in<strong>for</strong>mation will be reviewed and used to update POD estimates <strong>for</strong> ultrasonic inspection of titanium<br />

billet and to extend the POD estimates to cover billets up to 14″ diameter. Included will be a review<br />

of the revised inspection approaches <strong>for</strong> larger diameter billets, the development of any model<br />

modifications required to predict the flaw response <strong>for</strong> those approaches, validation of those models<br />

using calibration standards and chord blocks, and prediction of POD. These predictions will be<br />

compared to those of existent methodologies where the data is sufficient to allow existent<br />

methodologies to be used.<br />

In<strong>for</strong>mation from the responses of the CBS defects will be used with the new methodology to<br />

update POD estimates and provide them to RISC and TRMD. New flaw detection data will be<br />

incorporated into revised estimates of titanium billet POD as they occur, and will provide a basis <strong>for</strong><br />

revising the “default” POD estimates that have been supplied to the AIA Rotor Integrity<br />

Subcommittee (RISC).<br />

In<strong>for</strong>mation from the responses of the CBS defects will be used in three ways. Ten of these defects<br />

will have undergone careful metallographic analysis in Phase I. As noted previously, this<br />

in<strong>for</strong>mation will be a part of the detailed validation of the flaw response models. It will provide input<br />

to tuning the model <strong>for</strong> the response of naturally occurring flaws. Finally, methods will be sought<br />

and implemented to utilize the in<strong>for</strong>mation in the remaining 50 flaws which were not the subject of<br />

destructive metallographic characterization. Here, the approach will be to seek a correlation<br />

between the C-scan image size (available <strong>for</strong> all 60 flaws) and actual defect size available <strong>for</strong> the<br />

ten which have been sectioned. If such a correlation is successful on these 10 defects, it will be<br />

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used to estimate the size of all defects found in the contaminated heat. From this size estimate and<br />

the measured response, an enhanced data base <strong>for</strong> fine tuning the model <strong>for</strong> the response of<br />

naturally occurring flaws will be available. In addition, in<strong>for</strong>mation about billet flaws gained from the<br />

related <strong>for</strong>ging studies (i.e., from TRMD); and from direct comparison of multizone and conventional<br />

ultrasonic inspection system per<strong>for</strong>mance, will be considered. Based on this in<strong>for</strong>mation, integrated<br />

in the context of the new methodology, updated POD estimates will be made and provided to RISC<br />

and TRMD.<br />

POD <strong>for</strong> Nickel Billet: The new methodology will be implemented on ultrasonic inspection of nickel<br />

billet analogous to that used <strong>for</strong> titanium alloys in Phase I. This will draw heavily on the modeling<br />

work of Phase I, and on results of fundamental studies and model developments planned <strong>for</strong> Phase<br />

II. Based on those fundamental studies, flaw response models will be developed <strong>for</strong> white spots<br />

and other defects from the critical flaw list. Flaw response data and noise data will be gathered,<br />

including any pertinent results from the pilot lot inspection in Subtask 1.1.2 as well as<br />

measurements on synthetic white spots in Subtask 1.1.1. These data will be used as the basis <strong>for</strong><br />

initial estimates of nickel billet POD analogous to that employed <strong>for</strong> Ti-billet in Phase I, extended<br />

where possible by subsequent improvements in the methodology, as developed in Phase II.<br />

Measurements of calibration standards and chord blocks will be used <strong>for</strong> validation as appropriate.<br />

A study will be conducted of the effects of calibration response variability and determination of flaw<br />

size on the accuracy of POD predictions.<br />

Comparison of Inspection Systems - Use of the Random Defect Block: This section will be updated<br />

in the next quarter to reflect all changes currently being made.<br />

Objective/Approach Amendments:<br />

The objective and general approach remain as originally proposed in July 1998 with the exception<br />

of work related to the Random Defect Block. A proposal <strong>for</strong> new work was submitted to the FAA in<br />

February 2000. Per FAA technical redirection, on March 17, 2000, all ef<strong>for</strong>t other than that related<br />

to the RDB was suspended. The RDB recovery program was initiated in May 2000. On March<br />

14, 2001, guidance was received regarding resumption of the technical work on subtask 3.1.1 with<br />

the initial activity being the revision of program schedules and technical path to account <strong>for</strong> the RDB<br />

results.<br />

Progress (January 1, 2002 – March 31, 2002):<br />

In this period, our CBS reconstruction work was focused on defect B1AW2-B (POD 9). Because<br />

this defect is very close to the surface of the billet, side 1 of the cube block retained the original<br />

billet surface to prevent the defect from being accidentally cut-off. The curved surface geometry,<br />

however, had caused some degree of accessibility problem in carrying out ultrasonic scans from<br />

neighboring sides 2, 4, 5 and 6 (Fig. 1). The footprint of the 5 MHz insonifying transducer beam<br />

might be partially off the edges of one or more of these sides, resulting in signal loss. Furthermore,<br />

other than vertical edges of the cube block, there were no fiducial marks available in the<br />

micrographs to help align the successive cross-sections of the defect. This has made the<br />

micrograph re-alignment in the vertical direction quite difficult and uncertain. Nevertheless, both<br />

geometric and ultrasonic models of this defect have been completed to the best our capacity. The<br />

geometric model consists of one flat void part with four branches, and was built using 6 geometric<br />

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model parts across 17 micrograph planes (including 4 patches) with 30 boundary traces. The<br />

physical dimension of the minimal “bounding box” in the original orientation of micrographs (also<br />

shown in Figure 1) is 135 (X) x 31 (Y) x 64 (Z) mils. Figs. 2-4 depict the three-dimensional<br />

geometric surface model of the defect. Based on the geometric model results, the corresponding<br />

UT model was utilized to produce the simulated C-scan images as shown in Fig. 5. The overall<br />

agreement between the experiment and model predictions is not as good as <strong>for</strong> previous cases. As<br />

viewed through sides 5 and 6, the model predictions are low by 5.8 dB and 6.1 dB respectively,<br />

Through side 2, the predictions are high by 8.1 dB. For the CBS, our target agreement is 6 dB,<br />

although we have often obtained agreements on the order of 3 dB. We believe that the differences<br />

observed <strong>for</strong> this defect are on the high side of the target agreement because of the<br />

a<strong>for</strong>ementioned absence of fiducial marks which made the construction of the solid model less<br />

accurate. As viewed through side 4, the model predictions are high by an unacceptable 15.2 dB.<br />

We believe that this is caused by the a<strong>for</strong>ementioned possibility that part of the beam was “cut-off”<br />

by the curved exterior surface of the sample. Examination of Figure 1 shows that this would have<br />

been most likely to occur <strong>for</strong> side 4.<br />

Flaw (inside)<br />

Side 1 (top)<br />

Side 2 (back)<br />

Side 5 (right)<br />

Side 6 (left)<br />

Side 4 (front)<br />

Z<br />

Side 3<br />

X<br />

Side 6<br />

Side 2 Side 5<br />

Y<br />

Side 1<br />

Figure 1<br />

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Z<br />

Y<br />

X<br />

Figure 2. Angle View of Void Model <strong>for</strong> B1AW2-B (I)<br />

Z<br />

Y<br />

X<br />

Figure 3. Angle View of Void Model <strong>for</strong> B1AW2-B (II)<br />

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Z<br />

Y<br />

X<br />

Figure 4. Angle View of Void Model <strong>for</strong> B1AW2-B (III)<br />

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5 MHz C-scan Image Comparisons: B1AW2-B<br />

Side 2<br />

Model Experiment Model<br />

Side 4<br />

Experiment<br />

31(H) x 31(V) @10 mils, 2dB<br />

peak amplitude @2dB=573 mv<br />

deviation=155% or 8.1 dB<br />

60(H) x 30(V) @10 mils, 2dB<br />

peak amplitude @2dB=225 mv<br />

51(H) x 31(V) @10 mils, 0dB<br />

peak amplitude @0dB=901 mv<br />

deviation=474% or 15.2 dB<br />

60(H) x 30(V) @10 mils, 0dB<br />

peak amplitude @0dB=157 mv<br />

Model<br />

Side 5<br />

Experiment<br />

Model<br />

Side 6<br />

Experiment<br />

31(H) x 31(V) @10 mils, 2dB<br />

peak amplitude @2dB=111 mv<br />

deviation=-49% or -5.8 dB<br />

60(H) x 30(V) @10 mils, 2dB<br />

peak amplitude @2dB=217 mv<br />

31(H) x 31(V) @10 mils, 0dB<br />

peak amplitude @0dB=192 mv<br />

deviation=-51% or -6.1 dB<br />

60(H) x 30(V) @10 mils, 0dB<br />

peak amplitude @0dB=384 mv<br />

Multizone Color Code<br />

0 128 255<br />

Experiment 255 = 500mv <strong>for</strong> sides 2, 5 and 6<br />

= 250mv <strong>for</strong> side 4<br />

Plans (April 1, 2002 – June 30, 2002):<br />

Figure 5. 5 MHz C-scan Image Comparisons: B1AW2-B<br />

Primary plans <strong>for</strong> this period are to complete the analysis of the CBS data. Assuming approval of<br />

the restart technical plan by the FAA, technical work will resume as directed by the agency.<br />

Milestones:<br />

Revised dates of TBD are shown <strong>for</strong> most of the tasks, given that work has been stopped while the<br />

problems with the random defect block are being addressed. Revised dates to be provided in next<br />

report.<br />

Original<br />

Revised<br />

Description<br />

Status<br />

Date<br />

Date<br />

Approach to tune flaw response model to the<br />

behavior of naturally occurring flaws<br />

4 months TBD Provide a written description of the recommended<br />

method (GE, ISU)<br />

6 months TBD A report defining a method <strong>for</strong> relating properties of<br />

naturally-occurring flaws to the parameters of the<br />

ISU model.<br />

12 month deliverable of 3.1.2 is<br />

serving as a common basis <strong>for</strong> 3.1.1,<br />

3.1.2. General procedure <strong>for</strong> tuning<br />

flaw response model is included in<br />

the 3.1.2 white-paper.<br />

Completion of full report delayed by<br />

redirection of work.<br />

Improvements and assessment of POD/PFA<br />

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Original<br />

Date<br />

Revised<br />

Date<br />

Description<br />

Status<br />

methodology<br />

12 months TBD Report results from applying RDB and CBS data to<br />

validate the ISU models developed in Phase I.<br />

(ISU, with support from AE, GE, PW)<br />

12 months TBD A report assessing success of the Phase I<br />

development of a new POD methodology.<br />

Ongoing<br />

Modify the modeling software if and when<br />

necessitated by experimental data. (ISU)<br />

30 months Review and report on effects on POD of calibration<br />

response variability, and uncertainty in determining<br />

flaw size, conducted on Nickel only. (GE, with<br />

support from ISU) Provide OEMs with integrated<br />

software containing flaw response and noise<br />

models. (ISU)<br />

30 months Report documenting the software and material<br />

characterization procedures with which the OEMs<br />

can implement the new methodology.<br />

48 months Complete development and validation of models <strong>for</strong><br />

the effects of microstructure on beam profiles and<br />

apparent attenuation. (ISU, PW with support from<br />

GE, AE)<br />

60 months<br />

TBD<br />

Provide OEMs with final software and procedure<br />

packages. (ISU)<br />

Completion of full report delayed by<br />

redirection of work.<br />

Completion of full report delayed by<br />

redirection of work.<br />

POD <strong>for</strong> titanium billet – existent/new data analysis,<br />

and use of the CBS<br />

12 months TBD Complete report of analysis of CBS data. (ISU,<br />

with support from AE, GE, PW)<br />

Ongoing<br />

Updated POD estimates <strong>for</strong> naturally occurring<br />

flaws in titanium alloys as new field-find data<br />

become available. (GE, ISU, with support from AE,<br />

ISU)<br />

42 months<br />

Initiate POD assessment of revised inspection<br />

approaches <strong>for</strong> large diameter billet (10″ to 14″).<br />

(PW with support from ISU, GE) Characterize<br />

transducers to be used in inspection of large<br />

diameter billets. (Utilize results from 1.2.1)<br />

42 months Report documenting the revised estimates of POD<br />

<strong>for</strong> larger diameter titanium billet<br />

51 months Predict response <strong>for</strong> large diameter billets. Use<br />

calibration standards, RDB, and chord blocks <strong>for</strong><br />

validation as appropriate. (ISU with support from<br />

PW, GE)<br />

Provide POD estimate <strong>for</strong> larger diameter billet.<br />

(ISU, with support from AE, GE, PW) Compare<br />

results with those from alternative POD<br />

methodologies. (GE, with support from ISU)<br />

51 months Report documenting the estimates of POD and<br />

PFA <strong>for</strong> titanium billet based on use of the random<br />

defect block, CBS data, and data reported to<br />

JETQC, including comparison with POD results<br />

from existent methodologies.<br />

Completion of full report delayed by<br />

redirection of work.<br />

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Original<br />

Revised<br />

Description<br />

Status<br />

Date<br />

Date<br />

POD <strong>for</strong> nickel billet<br />

24 months Initiate nickel billet POD program utilizing results<br />

from Production Inspection Task. (ISU, with<br />

support from AE, GE, PW)<br />

30 months Characterize transducers to be used in inspection<br />

of nickel billets. (Utilize results from 1.1.2)<br />

58 months Predict response <strong>for</strong> nickel billets. Use calibration<br />

standards and chord blocks <strong>for</strong> validation as<br />

appropriate. (ISU with support from AE, GE, PW)<br />

60 months Provide report of POD estimates <strong>for</strong> nickel billet.<br />

(ISU with support from AE, GE, PW)<br />

Compare results with those from alternative POD<br />

methodologies. (GE, with support from ISU)<br />

60 months Report documenting the POD and PFA estimates<br />

<strong>for</strong> nickel billet, including comparison with POD<br />

results from existent methodologies.<br />

(8/97 -<br />

Phase I<br />

(12/97 -<br />

Phase I)<br />

(4/98 -<br />

Phase I)<br />

(8/98 -<br />

Phase I)<br />

Program<br />

start<br />

6/15/99<br />

Comparison of inspection systems - Use of the<br />

Random Defect Block<br />

Random defect block fabrication completed.<br />

ISU predictions of accuracy of model completed.<br />

Initiate ETC measurements using zoned and<br />

conventional inspection (on commercial systems.<br />

Complete measurements on RDB. (GE)<br />

Begin data analysis of ETC measurements on<br />

random defect block. (All)<br />

5/8/00<br />

1/8/01<br />

Begin random defect block recovery program.<br />

Complete random defect block recovery program.<br />

6 months TBD Incorporate interim results into provision of<br />

improved default POD curves to RISC and TRMD.<br />

(GE, PW, with support of AE)<br />

38 months Provide report comparing conventional and zoned<br />

inspection systems in use by billet suppliers, based<br />

on data from the Random Defect Block. (All)<br />

40 months A report documenting the relative effectiveness of<br />

conventional and Multizone systems <strong>for</strong> the<br />

ultrasonic inspection of billet.<br />

Completed. Ef<strong>for</strong>t initiated at<br />

program start in June 1999<br />

Completed<br />

Expect delay resulting from RDB<br />

issues.<br />

Deliverables:<br />

A report defining a method <strong>for</strong> relating properties of naturally-occurring flaws to the parameters of<br />

the ISU model.<br />

A report assessing success of the Phase I development of a new POD methodology.<br />

Software and material characterization procedures with which the OEMs can implement the new<br />

methodology.<br />

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A report documenting the relative effectiveness of conventional and Multizone systems <strong>for</strong> the<br />

ultrasonic inspection of billet.<br />

Revised estimates of POD <strong>for</strong> larger diameter titanium billet (10″ to 14″).<br />

POD and PFA estimates <strong>for</strong> nickel billet, including comparison with POD results from existent<br />

methodologies.<br />

Estimates of POD and PFA <strong>for</strong> titanium billet based on use of the random defect block, CBS data,<br />

and data reported to JETQC, including comparison with POD results from existent methodologies.<br />

Metrics:<br />

A procedure <strong>for</strong> incorporating the properties of naturally-occurring defects into a model-based POD<br />

methodology will have been defined in a <strong>for</strong>mal report which becomes the basis <strong>for</strong> industrial<br />

practice, providing a consistent basis <strong>for</strong> future implementation of the POD methodology.<br />

The success of the new POD methodology developed in Phase I will be critically reviewed in terms<br />

of attainment of the original goals, using the following criteria:<br />

• POD results are more accurate than those of existing methodologies. They should be close<br />

(e.g., flaw size <strong>for</strong> a given probability within ±40%) to those from existing (R e and â-versus-a)<br />

methods when the requirements of those methods are satisfied and provide sensible<br />

predictions in cases in which the existing methods cannot produce answers.<br />

• PFA results are estimated as a function of threshold and these estimates are validated by<br />

independent experiments.<br />

• The method provides a means to predict the effect on POD and PFA of changing (as a<br />

minimum) transducer beam properties (diameter, focal length, water path, beam orientation);<br />

transducer frequency; scan index; flaw properties (location, dimensions, acoustic impedance,<br />

orientation relative to the sound beam); material properties (acoustic impedance,<br />

grain-boundary noise), with experimental validation that the response agrees with that predicted<br />

by the model, as a result of changing any one of these parameters, within accuracies typical of<br />

ultrasonic measurement, i.e., about ±3 dB (or ±40%).<br />

Modifications will be developed that will enhance the speed, simplicity of use, and range of<br />

applicability of the POD software developed in Phase I; the ease of operation will be demonstrated<br />

by successful transfer of the software to one or more OEMs.<br />

Estimates of the POD of hard-alpha defects in titanium billets will be extended to cover billet<br />

diameters up to 14″. Success of this enhanced capability <strong>for</strong> assessing the quality of one of the<br />

materials used in manufacture of aircraft engines will be indicated by incorporation of these<br />

estimates in life management calculations by the FAA, members of ETC and the Rotor Integrity<br />

Subcommittee of AIA.<br />

Estimates of the POD of hard-alpha defects in titanium billets, and of white spots in nickel billets,<br />

will be updated periodically. Success will be indicated by incorporation of these estimates in life<br />

management calculations by the FAA, members of ETC, and the Rotor Integrity Subcommittee of<br />

AIA.<br />

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Improvements in detectability attainable through use of zoned ultrasonic inspection will be<br />

quantified and documented, permitting subsequent assessments by the OEMs of the effectiveness<br />

of such systems in improving the quality of titanium billet used <strong>for</strong> aircraft engine applications.<br />

Major Accomplishments and Significant Interactions:<br />

Date<br />

June 14-15, 1999<br />

September 15,<br />

1999<br />

June 8-12, 2000<br />

August 15, 2000<br />

October 6, 2000<br />

November 15,<br />

2000<br />

February 8, 2001<br />

February 22, 2001<br />

May 7-8, 2001<br />

August 14, 2001<br />

Description<br />

Technical Kick-off Meeting in West Palm Beach, FL<br />

Workshop in Ames to discuss the random defect block and other 3.1.1 planning issues.<br />

Inspection of the Random Defect Block by RMI in Niles, OH be<strong>for</strong>e and after modification of<br />

the surface condition, as observed by entire team.<br />

Presentation of preliminary results of the RDB recovery program to the FAA at the Semi-<br />

Annual Review Meeting in Evendale, OH..<br />

Team discussion, with FAA, of RDB recovery program.<br />

Presentation of status of RDB recovery program at AACE Annual Symposium in Seattle, WA.<br />

Presentation of status of the RDB recovery program at the ETC Semi-Annual Review in<br />

Atlantic City, NJ.<br />

Presentation of results of the RDB recovery program and proposed future plans at ANE,<br />

Burlington, MA.<br />

Team meeting to lay out plan <strong>for</strong> restart of subtask<br />

Presentation of current status at the FAA R E&D Technical Review in Atlantic City<br />

Publications and Presentations:<br />

Date<br />

December 8, 1999<br />

March 28, 2000<br />

July 19, 2000<br />

July 19, 2000<br />

Description<br />

“Probability of Detection Determination <strong>for</strong> Internal Inclusions in Gas Turbine <strong>Engine</strong> Rotating<br />

Components”, presented by Bruce Thompson at the 4 th Annual FAA/Air Force Workshop on<br />

the Application of Probabilistic Methods to Gas Turbine <strong>Engine</strong>s, Jacksonville, Florida.<br />

“Overview of S/N Based POD Methodologies”, presented by Bruce Thompson at the ASNT<br />

Spring Conference and 9 th Annual Research Symposium, Birmingham, Alabama<br />

“A Methodology <strong>for</strong> Predicting the Probability of Detection <strong>for</strong> Ultrasonic Testing”, presented<br />

by W. Q. Meeker at the Review of Progress in Quantitative <strong>Nondestructive</strong> <strong>Evaluation</strong>, Ames,<br />

Iowa.<br />

“Ultrasonic and Statistical Analyses of Hard-Alpha Defects in <strong>Titanium</strong> Alloys”, presented by<br />

C.-P. Chiou at the Review of Progress in Quantitative <strong>Nondestructive</strong> <strong>Evaluation</strong>, Ames, Iowa.<br />

October 16, 2000 “The Use of Physical Models of the Inspection in the Determination of POD”, presented by R.<br />

B. Thompson at the workshop, “POD Methodologies: New Horizons,” organized by The<br />

Technological Cooperation Program (TTCP), an international collaboration of the defense<br />

departments of English-speaking countries, in Patuxent River, Maryland.<br />

March 28, 2001<br />

July, 2001<br />

“Use of Physical Models of the Inspection Process in the Determination of Probability of<br />

Detection,” presented by R. B. Thompson at the ASNT Spring Conference and 10 th Annual<br />

Research Symposium, Denver, Colorado.<br />

“Use of Physical Models of the Inspection Process in the Determination of Probability of<br />

Detection,” R. B. Thompson, published in Materials <strong>Evaluation</strong>, Volume 59, Number 7,<br />

pp.861-865 (2001)<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Project 3:<br />

Task 3.1:<br />

Subtask 3.1.2:<br />

Inspection Systems Capability<br />

Assessment and Validation<br />

POD Methodology Applications<br />

POD of Ultrasonic Inspection of<br />

<strong>Titanium</strong> Forgings<br />

Team Members:<br />

HW: Tim Duffy, Andy Kinney, Waled<br />

Hassan<br />

GE: Dick Burkel, Bob Gilmore, Jon Bartos,<br />

Dave Copley, Walt Bantz, Ed Nieters<br />

ISU: Thomas Chiou, Bill Meeker, Bruce<br />

Thompson, Lisa Brasche<br />

PW: Jeff Umbach, Kevin Smith, Taher<br />

Aljundi<br />

Students: none<br />

Program initiation date: June 15, 1999. All ef<strong>for</strong>t was stopped on March 17, 2000; On March 14,<br />

2001, guidance was received regarding resumption of the technical work on subtask 3.1.2 with the<br />

initial activity being the revision of program schedules and technical path to account <strong>for</strong> the RDB<br />

results.<br />

Objectives:<br />

• To extend the SNR-based methodology developed in Phase I to predict the POD of naturally<br />

occurring defects in titanium, sonic-shaped <strong>for</strong>gings <strong>for</strong> commonly used ultrasonic procedures<br />

and geometries.<br />

• To further extend the POD methodology to <strong>for</strong>gings of final shape, including the prediction of<br />

POD as a function of position within the part.<br />

• To provide the OEM’s with a set of tools which they can use to implement the new methodology<br />

in internal analysis of POD of <strong>for</strong>gings by increasing the user-friendliness of the methodology<br />

software and flaw and noise response models <strong>for</strong> <strong>for</strong>ging conditions. Included are<br />

improvements in speed, accuracy, range of cases treated and reduction in the amount of<br />

experimental data required.<br />

• To improve the reliability of experimental methods <strong>for</strong> detecting flaws in sonic-shaped <strong>for</strong>gings<br />

and final-shaped, machined parts by developing and validating tools which allow evaluation of<br />

the likely effect on POD of proposed changes in inspections systems and procedures such as<br />

scan plans, transducer properties, gate widths, etc.<br />

• To verify that the new methodology produces POD results which are comparable with results<br />

from existent methodologies in cases when sufficient data is available that the existent<br />

methodologies can be successfully applied and which are consistent with reasonable<br />

expectations when such data is not available.<br />

• To provide the best available estimates of titanium <strong>for</strong>ging POD to the aircraft engine industry,<br />

by means of periodically updating existing estimates based on new in<strong>for</strong>mation, as it becomes<br />

available. This will include incorporating new flaw data, and extending the POD estimates to a<br />

wider range of typical <strong>for</strong>gings geometries through use of the ISU physical models.<br />

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• To use this methodology to assess the improvements in POD af<strong>for</strong>ded by the Production<br />

Inspection Task 1.3.2.<br />

Approach:<br />

This task will extend and apply the approach used in Phase I <strong>for</strong> billets to develop a method <strong>for</strong><br />

estimating POD of naturally occurring flaws in <strong>for</strong>gings. The methodology developed in Phase I is<br />

based on detection theory concepts involving distributions of noise and of flaw response in the<br />

presence of noise. In this subtask, that methodology will be applied to the case of <strong>for</strong>gings, with a<br />

major extension being related to predicting the POD as a function of position within the <strong>for</strong>ging.<br />

The proposed program consists of four major elements, which have been selected in response to<br />

the issues identified above.<br />

Application of the Methodology to Sonic-Shaped Forgings: Initial work in Phase II will use designed<br />

experiments to specify distributions of noise and signal response in existing blocks of <strong>for</strong>ged<br />

material containing FBHs and/or SHAs. The initial focus will be on the effect of material anisotropy<br />

that results from flow lines created by the <strong>for</strong>ging process on POD. The first step will be<br />

determination of the magnitude of anisotropy, which will be determined in subtask 1.3.1,<br />

Fundamental Studies. Given that in<strong>for</strong>mation, the flaw response and noise models will be modified<br />

to take into account this anisotropy. Appropriate statistical distributions will then be developed,<br />

based on a combination of these models and experimental data to describe the distributions of<br />

signal and noise response <strong>for</strong> a simple <strong>for</strong>ging geometry. Any further modifications to the<br />

methodology needed to take into account anisotropy will be made.<br />

When samples become available from Task 1.3.2, similar, but more extensive, experimental studies<br />

will be conducted on sonic-shaped <strong>for</strong>gings. These experiments will be conducted with samples<br />

containing flat bottom holes placed at some number n (to be determined later) positions in the<br />

sample. The positions will be chosen to provide a range of inspection geometries, surface<br />

curvatures, flaw depths, etc. Because of the symmetry of sonic-shaped samples, it will be possible<br />

to replicate these synthetic flaws systematically around the sample unit to allow a study of the<br />

variability of the responses of nominally identical flaws (providing important in<strong>for</strong>mation needed to<br />

quantify sources of variability in signal response). Initial scanning, analysis, and modeling will be<br />

done on a representative sample of n/2 of the seeded flaw positions. The experimental data will be<br />

important <strong>for</strong> developing a methodology that will account <strong>for</strong> the strong effect that flaw location will<br />

have on POD with complicated geometries. The data will be analyzed to check and tune the<br />

deterministic signal-response model and to develop appropriate statistical models <strong>for</strong> the variability<br />

in the signal response measurements, the important components of the POD prediction model.<br />

The resulting POD prediction methodology will then be used to predict POD at the other n/2<br />

positions, to validate the results. The data generated during these scans will also be used to<br />

provide a database which will be used in the development of noise distributions, as influenced by<br />

surface curvature.<br />

Because a significant amount of the data will be generated in the above study, it should be possible<br />

to compare POD predictions from the new methodology with predictions of existing methods such<br />

as the ahat vs. a and the R e methods. Such comparisons will be made to provide an important<br />

check on the different aspects of the methodology over the required wide range of inspection<br />

conditions encountered in <strong>for</strong>gings. Ef<strong>for</strong>ts will be initiated to take into account the morphology of<br />

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naturally occurring flaws in <strong>for</strong>gings. It is recognized that this morphology will be somewhat<br />

different from that in billets due to the de<strong>for</strong>mations that occur in the <strong>for</strong>ging process. Close<br />

contacts will be maintained with the TRMD program to obtain the necessary morphology<br />

in<strong>for</strong>mation.<br />

Development of the Capability to Make Predictions of the Local POD in Final Forging Shapes:<br />

Because of the complexity of the geometry of final part shape and of the effects of anisotropy<br />

associated with flow lines, the POD will depend strongly on position in final <strong>for</strong>ging shapes. The<br />

new methodology is designed to take these effects into account, and this capability will be<br />

developed and applied. The essential steps that are required will be determinating, on a<br />

point-by-point basis, the following:<br />

• Effect of <strong>for</strong>ged material on the flaw response and noise distributions, building on the results of<br />

the sonic-shaped studies<br />

• Effect of surface curvature and other geometrical parameters on the beam shape and there by<br />

on the flaw response and noise distributions<br />

In parallel, an implementation plan <strong>for</strong> including these point-by-point variations in the methodology<br />

will be developed, so that the result can be efficiently integrated with the life prediction code,<br />

DARWIN.<br />

Experimental validation will then be undertaken. The ultrasonic response model will be used to<br />

predict the signal response from flaws which are insonified through representative surface<br />

geometries using the samples being developed in Task 1.3.1. Samples will be designed in<br />

cooperation with 1.3.1 to evaluate the full range of surface curvatures typical in final and sonic<br />

shape <strong>for</strong>gings. Consideration will also be given to evaluation beyond typical curvatures to<br />

determine the limits of the model applicability. The flaw response model will be verified by scanning<br />

these specimens and comparing these observations to the model predictions. Checks on the<br />

resulting POD predictions will be made <strong>for</strong> certain testing situations <strong>for</strong> which POD curves have<br />

been estimated by other means (e.g., the ahat vs. a and the R e methods). Upon completion of<br />

these tests, an updated version of the methodology will be prepared.<br />

Improvements/Transfer of the POD/PFA Methodology Software to OEMs: For the new<br />

methodology to have full impact on damage tolerant design and management of rotating<br />

components of aircraft engines, it is necessary that the tools, i.e., software <strong>for</strong> implementing the<br />

methodology, the associated modules <strong>for</strong> predicting flaw and noise response as influenced by<br />

anisotropy and geometry, and materials characterization procedures to efficiently use them, be in a<br />

<strong>for</strong>m that can be readily used by the OEMs. These tools will be developed, incorporating the results<br />

of the previously described major work elements. Included will be the methodology software, flaw<br />

and noise response modeling modules (as influenced by anisotropy and part geometry), and<br />

characterization procedures to provide the necessary inputs. As in 3.1.1, numerical approximations<br />

to the predictions of the ultrasonic response models will be developed which are suitable <strong>for</strong> being<br />

called by the methodology to speed the calculation process to a rate which will be convenient <strong>for</strong> a<br />

user operating in an interactive mode. Also building on the experiences gained in the Task 3.1.1,<br />

the flaw response models and noise models will be designed to incorporate the effects of<br />

microstructure on beam profile, and hence, on the distribution of flaw response, the effects of tight<br />

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focusing with respect to the scale of the microstructure on the <strong>for</strong>m of the signal and noise<br />

distributions, and the rules required to determine the distribution of signal-in-the-presence-of-noise<br />

from the noise distribution and the flaw free noise response. All of these will be considered as<br />

influenced by the presence of anisotropy and beam modification by the part geometry. Results of<br />

these software and procedural advances will be integrated and provided to the OEMs <strong>for</strong> their<br />

internal use. These uses are anticipated to include life management calculations, such as<br />

consideration of the likely effects on POD of proposed changes in inspection systems and<br />

procedures such as scan plans, transducer properties, gate widths, etc.<br />

POD <strong>for</strong> <strong>Titanium</strong> Forgings: Ef<strong>for</strong>ts to acquire naturally occurring hard alpha inclusion data will be<br />

continuously made. Possible sources include field and manufacturing finds, the utility of which will<br />

depend on the degree to which appropriate procedures are utilized to fully characterize the 3-D<br />

shapes of these finds. In<strong>for</strong>mation gained during the <strong>for</strong>ging studies of the TRMD program will also<br />

be used. This in<strong>for</strong>mation will be used, as appropriate, to provide POD estimates. The<br />

methodology will be used to evaluate the improvements in POD af<strong>for</strong>ded by developments of the<br />

Production Inspection Task 1.3.2.<br />

Objective/Approach Amendments: Objective and approach remain as originally proposed in July<br />

1998.<br />

Progress (January 1, 2002 – March 31, 2002):<br />

On March 16, 2000 the FAA issued instructions to end all expenditures on Task 3, other than those<br />

associated with the RDB technical plan, with a restart to be considered once the sources of the<br />

discrepancy had been resolved. Hence the vast majority of the work on this task was terminated.<br />

A low level of ef<strong>for</strong>t has continued with the objective of coordinating with the Production tasks the<br />

work that is needed to support the POD ef<strong>for</strong>t. This had the objectives of ensuring that the<br />

fundamental studies measurements would produce the in<strong>for</strong>mation needed by the POD group and<br />

that <strong>for</strong>ging samples being produced would support the POD methodology. To these ends, the<br />

progress of the fundamental studies and <strong>for</strong>gings tasks have been monitored in terms of findings<br />

such as the degree of anisotropy and inhomogeneity of noise that has been observed in billet and<br />

<strong>for</strong>ging materials and plans to prepare samples that will provide in<strong>for</strong>mation to be used in POD<br />

assessment. In the latter context, particular attention has been paid to the fabrication of a <strong>for</strong>ging<br />

containing synthetic hard-alpha inclusions and flat bottom holes. On March 14, 2001, the FAA<br />

indicated that work is to be resumed on sub-tasks 3.1.1 and 3.1.2, and planning <strong>for</strong> that restart<br />

initiated.<br />

Plans (April 1, 2002 – June 30, 2002):<br />

Planning of the restart of subtask 3.1.2 will take place after the completion of the planning <strong>for</strong><br />

restart of subtask 3.1.1. In the meantime, continued interactions with the Fundamental Studies and<br />

Production Tasks will occur, with the initial ef<strong>for</strong>t focused on the design of the <strong>for</strong>ging POD sample.<br />

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Milestones:<br />

Revised dates of TBD are shown <strong>for</strong> most of the tasks, given that work has been stopped while the<br />

problems with the random defect block are being addressed.<br />

Original<br />

Date<br />

Revised<br />

Date<br />

Description<br />

Status<br />

Application of the Methodology to Sonic-Shaped<br />

Forgings:<br />

12 months TBD White-paper defining a method <strong>for</strong> predicting POD<br />

<strong>for</strong> sonic-shaped <strong>for</strong>ged parts.<br />

18 months Complete scanning and analysis of blocks of <strong>for</strong>ged<br />

material with FBH and SHA flaws. (ISU with<br />

support of AS)<br />

22 months Investigate the application of Phase I methodology<br />

to the scan data on <strong>for</strong>ged material with FBH and<br />

SHA flaws. (ISU)<br />

24 months Initiate generalization of the POD methodology to<br />

apply to sonic-shaped <strong>for</strong>gings. (ISU with support<br />

from GE)<br />

27 months Define experimental plan <strong>for</strong> use of FBH and SHA<br />

sonic-shaped <strong>for</strong>ged samples available from TRMD<br />

and Phase II Production Inspection Task. (All)<br />

27 months Report documenting a method <strong>for</strong> predicting POD<br />

<strong>for</strong> sonic-shaped <strong>for</strong>ged parts.<br />

30 months Acquire data from available FBH and SHA<br />

sonic-shaped <strong>for</strong>ged samples to generate<br />

noise and signal plus noise distributions.<br />

(PW, AS, GE)<br />

32 months Complete necessary modeling and supply<br />

model predictions corresponding to data<br />

available from sonic-shaped <strong>for</strong>ged samples.<br />

(ISU with support from AS)<br />

Utilize sonic-shaped <strong>for</strong>ging scan data to<br />

define noise distribution. (GE, PW with<br />

support from ISU)<br />

32 months Report documenting the revisions to the noise<br />

and flaw modeling developed in this subtask<br />

and supply the modified model predictions.<br />

36 months Utilize sonic-shaped <strong>for</strong>ging scan data to<br />

estimate the flaw-signal distribution and to<br />

compare with model prediction to define the<br />

deviation distribution. Apply the generalized<br />

methodology to estimate POD of synthetic<br />

hard alpha inclusions. (ISU with support from<br />

GE, PW)<br />

Compare with ahat vs. a and the R e methods.<br />

(GE with support from PW)<br />

36 months Report assessing the adequacy of POD predictions<br />

of the physical/statistical model-based methodology<br />

developed in this program, based on comparison<br />

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Original<br />

Date<br />

Revised<br />

Date<br />

Description<br />

Status<br />

with the ahat vs. a and the Re methods, and<br />

describing and illustrating the advantages of the<br />

new methodology.<br />

Development of the Capability to Make Predictions<br />

of the Local POD in a Final Forging Geometry<br />

24 months Analyze results (anisotropy, geometry effects) of<br />

Production and Inservice Inspection Tasks <strong>for</strong><br />

implications to POD as a function of position in<br />

typical <strong>for</strong>ging geometries. (ISU with support from<br />

AS, PW)<br />

27 months Define implementation plan <strong>for</strong> POD as function of<br />

position. (GE with support from ISU, PW, and AS)<br />

30 months Report providing default POD curves <strong>for</strong> titanium<br />

<strong>for</strong>gings, <strong>for</strong> both production and in-service<br />

inspections, <strong>for</strong> use by the OEMs and FAA in life<br />

management/risk assessment studies.<br />

30 months Initial estimates of POD and PFA <strong>for</strong> sonic-shaped<br />

titanium <strong>for</strong>gings based on use of the FBH, SHA,<br />

CBS data, and field finds.<br />

36 months Complete modeling tools <strong>for</strong> the effects of<br />

geometry on flaw response and noise distributions.<br />

(ISU with support from PW)<br />

36 months Revised estimates of POD as a function of <strong>for</strong>ging<br />

geometry, including effects of anisotropy,<br />

curvature, and position within the <strong>for</strong>ging.<br />

38 months Complete experimental validation of modeling<br />

tools. (PW with support from GE, AS) Complete<br />

the development of the methodology needed to<br />

account <strong>for</strong> positional effects on POD. (ISU with<br />

support from GE, PW, and AS)<br />

40 months Compare with ahat vs. a and the R e methods. (GE<br />

with support from ISU and PW)<br />

42 months Provide updated methodology with POD as<br />

function of position as an output. (ISU)<br />

ongoing<br />

Improvements/Transfer of the POD/PFA<br />

Methodology Software to OEMs<br />

Modify the modeling software if and when<br />

necessitated by experimental data. (ISU)<br />

40 months Provide OEMs with integrated software containing<br />

flaw response and noise models as influenced by<br />

anisotropy and geometry. (ISU)<br />

48 months Review results <strong>for</strong> effects of introducing numerical<br />

approximation methods to the flaw response<br />

surface to speed the operation of the new<br />

methodology. (ISU, with support of AS, GE, PW)<br />

52 months Complete development and integrate validated<br />

methods to add noise to flaw response in c-scan<br />

images in the presence of anisotropy. (ISU with<br />

support from PW)<br />

60 months Provide OEMs with final software and procedure<br />

packages. (ISU)<br />

60 months Report describing the technical details of the POD<br />

prediction methodology <strong>for</strong> sonic-shaped and final<br />

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Original<br />

Date<br />

Revised<br />

Date<br />

Description<br />

Status<br />

geometry <strong>for</strong>gings.<br />

POD <strong>for</strong> <strong>Titanium</strong> Forgings<br />

48 months Apply the generalized methodology to estimate<br />

improvements in POD af<strong>for</strong>ded by developments of<br />

Task 1.3. (ISU with support from GE)<br />

ongoing<br />

Deliverables:<br />

Update POD estimates <strong>for</strong> naturally occurring flaws<br />

in Ti alloys as field find data become available.<br />

(ISU with support of GE, PW, and HW)<br />

White-paper defining a method <strong>for</strong> predicting POD <strong>for</strong> sonic-shaped <strong>for</strong>ged parts.<br />

Initial estimates of POD and PFA <strong>for</strong> sonic-shaped titanium <strong>for</strong>gings based on use of the FBH,<br />

SHA, CBS data, and field finds.<br />

Revised estimates of POD as a function of <strong>for</strong>ging geometry, including effects of anisotropy,<br />

curvature, and position within the <strong>for</strong>ging.<br />

Report providing default POD curves <strong>for</strong> titanium <strong>for</strong>gings, <strong>for</strong> both production and inservice<br />

inspections, <strong>for</strong> use by the OEMs and FAA in life management/risk assessment studies.<br />

Report assessing the adequacy of POD predictions of the physical/statistical model-based<br />

methodology developed in this program, based on comparison with the ahat vs. a and the R e<br />

methods, and describing and illustrating the advantages of the new methodology.<br />

Report describing the technical details of the POD prediction methodology <strong>for</strong> sonic-shaped and<br />

final geometry <strong>for</strong>gings.<br />

Prototype software implementing the methodology and associated flaw and noise response models<br />

<strong>for</strong> POD prediction as a function of inspection parameters, position in <strong>for</strong>ging, and flaw<br />

characteristics.<br />

Metrics:<br />

Procedures will be developed <strong>for</strong> estimating the POD of sonic shaped <strong>for</strong>gings and of final <strong>for</strong>ging<br />

geometries as a function of position. Success will be indicated by the incorporation of these<br />

procedures by the OEMs in their life management programs.<br />

The ability of response models to predict flaw signals will be measured against the goal of having<br />

the predicted ultrasonic flaw response be within 3dB of experimental values at least 95% of the time<br />

when considered over typical inspection modalities.<br />

The ability to predict noise distributions will be measured against the goal of having predicted<br />

ultrasonic noise response within 3dB of experimental values at least 95% of the time when<br />

considered over typical inspection modalities.<br />

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The development and transfer of the software <strong>for</strong> POD/PFA curve generation will be considered<br />

successful if it is utilized by the members of ETC and the Rotor Integrity Subcommittee of AIA in life<br />

management decisions.<br />

Estimates of the POD of hard-alpha defects in sonic-shaped and final <strong>for</strong>ging geometries will be<br />

provided to the FAA and members of the ETC and Rotor Integrity Subcommittee. These estimates<br />

will be judged adequate if they compare favorably with predictions of existing POD methodologies<br />

<strong>for</strong> inspection situations in which such POD values can be obtained and if they provide sensible<br />

predictions in cases in which the existing methodologies cannot do so.<br />

Major Accomplishments and Significant Interactions:<br />

Date<br />

June 14-15,<br />

1999<br />

September 16,<br />

1999<br />

Description<br />

Technical Kick-off Meeting in West Palm Beach, FL<br />

Workshop to detail the approach <strong>for</strong> POD <strong>for</strong> Forgings. Included review of first draft of white paper<br />

and assignment <strong>for</strong> preparation of chapters of the document.<br />

Publications and Presentations:<br />

Date<br />

Description<br />

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Project 3:<br />

Task 3.1:<br />

Subtask 3.1.3:<br />

Inspection Systems Capability<br />

Assessment and Validation<br />

POD Methodology Applications<br />

POD of Eddy Current<br />

Inspections in the Field<br />

Team Members:<br />

HW:<br />

GE: Dick Burkel, Jon Bartos, Shridhar<br />

Nath, Walt Bantz<br />

ISU: Bill Meeker, Norio Nakagawa, Bruce<br />

Thompson<br />

PW: Kevin Smith, Dave Raulerson, Taher<br />

Aljundi<br />

Students: none<br />

Program initiation date: June 15, 1999. All ef<strong>for</strong>t was stopped on March 17, 2000.<br />

Objectives:<br />

• To develop a new methodology <strong>for</strong> estimating the POD and PFA of eddy current (ET)<br />

inspections in the field which facilitates prediction of POD and PFA <strong>for</strong> specific changes in test<br />

parameters, surface conditions, material noise characteristics and feature geometries in a rapid<br />

fashion without the need to construct extensive specimen sets.<br />

• To validate that methodology by comparing its POD results to corresponding predictions of<br />

existing methodologies, such as the a-hat versus a model, when sufficient data exists to<br />

support that comparison.<br />

• To apply the methodology to the estimation of POD/PFA of inservice inspections of flat plates and<br />

slots.<br />

• To transfer the resulting software and procedures to the OEM’s <strong>for</strong> their use in life management<br />

calculations.<br />

Approach:<br />

As in the previous work on UT, the methodology will be based on the determination of the<br />

distributions of signal and of noise, with physical models of the measurement process being used to<br />

allow the maximum in<strong>for</strong>mation to be obtained from limited experimental data. Special emphasis<br />

will be placed on the needs imposed by the development of field durability issues.<br />

The incorporation of physical models of the inspection adds flexibility and extensibility to the<br />

methodology, while reducing the cost. In general, physical models make parametric studies<br />

inexpensive, by repeated computations of output signals <strong>for</strong> a wide range of inspection parameters.<br />

The specific benefits of the models used in POD/PFA analyses are twofold:<br />

• The model-assisted POD/PFA estimation significantly reduces the specimen preparation,<br />

compared to a purely experiment-based POD estimate. The economic benefit is substantial <strong>for</strong><br />

flat-surface geometry since only a handful of crack specimens are sufficient to provide<br />

normalization and model predictions can then cover a wide range of parameters. The benefit is<br />

even more substantial when complex geometries are considered because, without models, one<br />

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must prepare a large number of specimens of varying defect sizes and conditions to per<strong>for</strong>m<br />

POD analyses <strong>for</strong> each new inspection geometry. The expense of this approach often leads to<br />

a best ef<strong>for</strong>t approach rather than a rigorous statistical study of the required number of<br />

samples.<br />

• Models make POD/PFA results transferable. For instance, suppose that the distributions have<br />

been determined <strong>for</strong> a given probe and the POD/PFA estimated. The model can then be used<br />

to transfer this POD/PFA result to another probe, with appropriate correction factors, because<br />

of the model’s ability to reliably predict relative signal strengths between one probe and<br />

another. Also, the model allows results to be transferred from one geometry [e.g., straight<br />

edges] to another geometry [e.g., slot edges]. Collectively, the use of models can reduce the<br />

cost and time requirements of POD/PFA analyses to more manageable levels in an<br />

environment where both inspection demands and opportunities are increasing. This results not<br />

only in cost savings, but more importantly, increases the likelihood that <strong>for</strong>mal POD/PFA<br />

estimates will be made with enhancement to safety and quantification of the benefits now<br />

possible.<br />

Figures 4 and 5 present flow diagrams of the work plan that has been developed to accomplish<br />

these goals, as is discussed in detail in the following text.<br />

a<br />

Notch<br />

& crack<br />

specimens<br />

h<br />

ET measurement<br />

b<br />

1D line/<br />

2D raster<br />

scan data<br />

g<br />

Physical probe<br />

response<br />

model<br />

(flaw & geometry)<br />

c<br />

Data<br />

analysis<br />

Validation<br />

Noise<br />

component<br />

Flaw<br />

signal<br />

Geometry<br />

signal<br />

d<br />

e<br />

Monte Carlo<br />

(Scan index,etc)<br />

f<br />

i<br />

Stat. model of<br />

noise<br />

distribution<br />

j<br />

Stat. model of<br />

signal<br />

distribution<br />

l<br />

Crack<br />

morphology<br />

database<br />

k<br />

POD, PFA,<br />

ROC<br />

Figure 4. Detailed experimental and validation plan <strong>for</strong> EC methodology.<br />

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7a-7l<br />

6<br />

8<br />

9<br />

10<br />

Key<br />

additional<br />

ingredients<br />

Bolt hole<br />

or<br />

slot demonstr.<br />

Second<br />

generation<br />

methodology<br />

Validation<br />

Third<br />

generation<br />

methodology<br />

2<br />

Workshop<br />

&<br />

Implementation plan<br />

3a-3l 4 5<br />

First<br />

Flat plate<br />

generation<br />

demonstration<br />

Validation<br />

methodology<br />

Figure 5. Overall framework <strong>for</strong> development and validation of the EC methodology.<br />

Workshop and Implementation Plan: A kickoff meeting will be held to finalize a number of aspects<br />

of the program.<br />

Development of Key Additional Ingredients <strong>for</strong> POD Modeling: The basic tools <strong>for</strong> the flaw<br />

response models are already in place and <strong>for</strong>med the basis <strong>for</strong> feasibility demonstrations. In this<br />

element a number of required extensions will be made. The primary model software is the<br />

BEM-based code, the development of which was initiated in the ETC Phase I, novel probe design<br />

program. The code has progressed recently to the point that it can deal with complex part<br />

geometries as well as general probe geometries and constructions. Of particular importance <strong>for</strong><br />

this proposed ef<strong>for</strong>t is its capability to deal with two types of probes of high current interest, i.e.,<br />

differential reflection and wide-field probes, and with complex geometries such as the edges of a<br />

slot. The code has been validated against experimental data from edge crack inspections with<br />

air-core coil probes. It is there<strong>for</strong>e a crucial component of the project to validate the BEM code<br />

experimentally against data from the project-specific inspection conditions, namely cracks in flat<br />

plate and slot geometries, with differential-reflection and wide-field probes. Such experimental<br />

validations will be per<strong>for</strong>med, as discussed below. In this work element, the theoretical<br />

comparisons will be made and model modifications made as needed. FEM-based models will also<br />

be used as a tool <strong>for</strong> cross-checking on the accuracy and validity of the BEM-based code. Practical<br />

inspection methods <strong>for</strong> complicated geometry often include methods <strong>for</strong> edge signal suppression.<br />

These will be reviewed and extended as needed, and methods will be developed <strong>for</strong> the<br />

characterization of their capability to reduce this component of noise.<br />

Application to a Simple Geometry: Flat Plates: The elements of the new methodology will be<br />

demonstrated by predicting the POD of notches and fatigue cracks in flat plates. Both differential<br />

reflection and wide field probes will be considered. A set of samples containing representative<br />

notches and cracks will first be obtained. These will be scanned to develop a data base, from<br />

which smaller data bases of noise and flaw response signals can be extracted. The noise data will<br />

be analyzed to yield a statistical model of the noise distribution, including its functional <strong>for</strong>m and<br />

procedures <strong>for</strong> determining its parameters. The data will also be analyzed to determine the extent<br />

to which the noise is controlled by surface finish, microstructure, or other effects. The flaw signals<br />

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will be used to validate the physical models <strong>for</strong> flaw response. These, as well as the noise<br />

distribution, will <strong>for</strong>m the basis <strong>for</strong> the <strong>for</strong>mulation of a physical model <strong>for</strong> the signal distribution. In<br />

the <strong>for</strong>mulation of this model, attention will be paid to providing “hooks” which will allow a crack<br />

morphology database to be introduced at a later time (the development of such a database is not<br />

priced in this proposal). From the statistical models of noise and signal, POD, PFA and ROC<br />

curves will be determined.<br />

Based on the flat-plate demonstration, a first generation methodology will be specified. This will<br />

include procedures <strong>for</strong> each of the steps mentioned above. The methodology will be validated by<br />

exercising it on a set of existent samples and comparing the results to those of existent<br />

methodologies such as a-hat versus a. The conditions under which one or the other breaks down<br />

and the degree of agreement between their predictions will be noted and interpreted. Particular<br />

attention will be paid to the sparseness of data that can be accommodated by the new<br />

methodology, and the time that would be required <strong>for</strong> its implementation in the field. The new<br />

methodology will be used to make predictions of POD, as influenced by a variety of parameters, <strong>for</strong><br />

use by the lifting community.<br />

Application to a Complex Geometry: Blade Slots: A demonstration will then be conducted on a<br />

blade slot, using a differential reflection probe. The same steps will be followed as in the flat plate<br />

demonstration, modified by insights gained in the <strong>for</strong>mulation of the first generation methodology,<br />

and considering the edge geometry signals as sources of noise in the analysis of the data. Poorly<br />

managed edge responses can easily mask defect responses. One must assume that the<br />

inspection procedure incorporates appropriate mechanisms (e.g., by correct choices of probes and<br />

scans, and/or by signal processing) so that the edge contamination is suppressed. This is the<br />

reason <strong>for</strong> the consideration of the differential reflection probe, which is frequently used to suppress<br />

edge responses in the field. The edge signal remaining is effectively a source of noise. Our new<br />

POD/PFA methodology will be designed to quantify the edge-suppression capabilities as well as<br />

the other sources of noise. Once the signal and noise distributions are determined, following<br />

procedures already discussed, predictions will be made of the POD, PFA and ROC.<br />

Based on the experiences gained in the blade slot demonstration, a second generation<br />

methodology will be <strong>for</strong>mulated. The second generation methodology will be validated by<br />

exercising it on an independent set of blade slot samples and comparing the results to those of<br />

existent methodologies such as a-hat versus a. The conditions under which one or the other<br />

breaks down and the degree of agreement between their predictions will be noted and interpreted.<br />

Particular attention will be paid to the sparseness of data that can be accommodated by the new<br />

methodology, and the time that would be required <strong>for</strong> its implementation in the field. After<br />

validation, the new methodology will be used to make predictions of POD, as influenced by a<br />

variety of parameters, <strong>for</strong> use by the lifing community.<br />

Improvement/Transfer of the POD/PFA Methodology Software to the OEMs: In order <strong>for</strong> the new<br />

methodology to have full impact on the damage tolerant design and management of rotating<br />

components of aircraft engines, it is essential that the necessary tools, i.e., software <strong>for</strong><br />

implementing the methodology, the associated modules <strong>for</strong> predicting flaw and noise response as<br />

influenced by geometry, and materials characterization procedures to efficiently provide input to<br />

them, be in a <strong>for</strong>m that can be readily used by the OEMs. These tools will be developed,<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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incorporating the results of the previously described major work elements. For example,<br />

procedures will be specified <strong>for</strong> the determination of the signal and noise distributions, defining the<br />

relative roles of empirical data and physical models. A final <strong>for</strong>m of the methodology will be<br />

produced, including software incorporating all experiences gained in the execution of the subtask.<br />

This will be transferred to the OEMs and documented in a final report.<br />

Objective/Approach Amendments: Objective and approach remain as originally proposed in July<br />

1998.<br />

Progress (January 1, 2002 – March 31, 2002):<br />

On March 16, 2000 the FAA issued instructions to end all expenditures on Task 3, other than those<br />

associated with the RDB technical plan, with a restart to be considered once the sources of the<br />

discrepancy had been resolved. On March 14, 2001, the FAA has indicated that work is to be<br />

resumed on sub-tasks 3.1.1 and 3.1.2, but discussions have not yet been held regarding the restart<br />

of Task 3.1.3.<br />

Plans (April 1, 2002 – June 30, 2002):<br />

At the present time, no activity is planned <strong>for</strong> this period.<br />

Milestones:<br />

Revised dates of TBD are shown <strong>for</strong> most of the tasks, given that work has been stopped while the<br />

problems with the random defect block are being addressed.<br />

Original<br />

Date<br />

Revised<br />

Date<br />

Description<br />

Status<br />

Workshop and Implementation Plan<br />

6 months TBD Establish implementation plan <strong>for</strong> adaptation of the<br />

methodology to eddy current inspection. Define<br />

data needed by Inspection Systems Capability<br />

Working Group to generate POD/PFA estimates<br />

and provide guidance to Inservice Inspection<br />

working group. (All)<br />

18 months TBD Application to a Simple Geometry: Flat Plates<br />

24 months TBD Development of Key Additional Ingredients <strong>for</strong> POD<br />

Modeling<br />

Application to a Complex Geometry: Blade Slots<br />

Improvement/Transfer of the POD/PFA<br />

Methodology Software to the OEMs<br />

Deliverables:<br />

Validated POD/PFA methodology <strong>for</strong> ET inspection based on signal and noise distributions which<br />

incorporates false call considerations, can be applied to sparse data and can predict the results of<br />

similar inspections <strong>for</strong> which no data is available.<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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Estimates of POD/PFA <strong>for</strong> ET inspection Milestones: improvements made with ETC tools.<br />

Updates to default POD curves <strong>for</strong> RISC documents.<br />

Prototype software suitable <strong>for</strong> implementation of the methodology by the OEMs.<br />

Metrics:<br />

The methodology developed <strong>for</strong> estimating POD of eddy current inspections will be judged<br />

successful if three conditions are met. For data sets such as those used by existent<br />

methodologies, the new methodology should make comparable POD predictions. For sparse data<br />

sets, the new methodology should make sensible predictions when none are made by existents<br />

empirical methodologies. In either case these predictions should be able to be obtained with less<br />

expense and more rapidly than with existent methodologies.<br />

The updates to the POD curves will be judged successful if they are incorporated by RISC in life<br />

management guideline materials.<br />

The software produced to implement the methodology will be judged successful if it is utilized by<br />

the members of ETC and the Rotor Integrity Subcommittee of AIA in life management decisions.<br />

The estimates of improvements af<strong>for</strong>ded by the advances in the ETC will be judged successful if<br />

they impact the acceptance of these technologies by the OEMs.<br />

Major Accomplishments and Significant Interactions:<br />

Date<br />

June 14-15,<br />

1999<br />

September 17,<br />

1999<br />

Description<br />

Technical Kick-off Meeting in West Palm Beach, FL<br />

Workshop to detail the approach <strong>for</strong> POD <strong>for</strong> EC. Included review of first draft of white paper and<br />

approach to the methodology.<br />

Publications and Presentations:<br />

Date<br />

Description<br />

Quarterly Report – January 1, 2002 –March 31, 2002<br />

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