Engine Titanium Consortium - Center for Nondestructive Evaluation ...
Engine Titanium Consortium - Center for Nondestructive Evaluation ...
Engine Titanium Consortium - Center for Nondestructive Evaluation ...
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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 />
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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 />
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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 />
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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 />
print date/time: 6/6/2002 - 8:39 AM – Page 12
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 />
Quarterly Report – January 1, 2002 –March 31, 2002<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 />
print date/time: 6/6/2002 - 8:39 AM – Page 16
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 />
print date/time: 6/6/2002 - 8:39 AM – Page 19
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 />
Quarterly Report – January 1, 2002 –March 31, 2002<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 />
Quarterly Report – January 1, 2002 –March 31, 2002<br />
print date/time: 6/6/2002 - 8:39 AM – Page 24
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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print date/time: 6/6/2002 - 8:39 AM – Page 25
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 />
Quarterly Report – January 1, 2002 –March 31, 2002<br />
print date/time: 6/6/2002 - 8:39 AM – Page 26
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 />
Quarterly Report – January 1, 2002 –March 31, 2002<br />
print date/time: 6/6/2002 - 8:39 AM – Page 27
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 />
print date/time: 6/6/2002 - 8:39 AM – Page 28
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 />
Quarterly Report – January 1, 2002 –March 31, 2002<br />
print date/time: 6/6/2002 - 8:39 AM – Page 30
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 />
Quarterly Report – January 1, 2002 –March 31, 2002<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 />
print date/time: 6/6/2002 - 8:39 AM – Page 38
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 />
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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 />
print date/time: 6/6/2002 - 8:39 AM – Page 40
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 />
Quarterly Report – January 1, 2002 –March 31, 2002<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 />
Quarterly Report – January 1, 2002 –March 31, 2002<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 />
Quarterly Report – January 1, 2002 –March 31, 2002<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 />
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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 />
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