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Additive Manufacturing at PM Titanium 2015<br />

| contents page | news | events | advertisers’ index | contact |<br />

GN<br />

Trial<br />

GN Temperature<br />

GN<br />

Time<br />

Average<br />

Microhardness<br />

Yield<br />

strength<br />

UTS<br />

EL<br />

Surface<br />

N 2<br />

°C hrs HV MPa MPa % wt%<br />

370 1032 1226 6.9<br />

1 800 4 505 986 1036 4.6 8.5-8.8%<br />

2 900 4 582 885 912 2.9 12-13%<br />

3 900 5 574 875 956 5.2 15-16%<br />

4 900 6.5 660 855 878 2.5 11-18%<br />

5 1030 3 610 765 775 1.2 12-20%<br />

Table 1 Gas nitriding trials with different nitriding processing conditions and mechanical properties of gas nitrided Ti64<br />

bars produced by SLM (compared with the as-built, untreated condition) [3]<br />

Ti-alloys. generate The beneficial microhardness effects of billet, in terms forged and extruded retardation Ti64-samples of crack were growth within at theΔK<br />

range of<br />

360-380 HV [34].<br />

of crack propagation rates. The crack below 20 MPa√m. From data points<br />

Table 2: Gas nitriding trials with different nitriding processing conditions and mechanical properties<br />

of<br />

propagation<br />

gas nitrided Ti64<br />

rates<br />

bars<br />

of<br />

produced<br />

the EBM-built<br />

by SLM.<br />

at very low rates of crack growth<br />

samples GN are GNplotted in GNFig. 8. The Average a threshold Yield of UTS 10 MPa√m ELcan Surface be N 2<br />

Trial results Temperature coincide with Time each other Microhardnessestimated. strength This is higher than the<br />

ºC hrs HV MPa MPa % wt%<br />

except for HT6/HIP. This implies that threshold value of 3.5 MPa√m cited<br />

370 1032 1226 6.9<br />

the 1 temperature 800 increase 4 from HT1 505 for SLM-fabricated 986 1036 Ti-6Al-4V 4.6 in 8.5the<br />

- 8.8%<br />

to 2 HT5/HIP 900 does not influence 4 crack 582 as-built 885 state. 912 2.9 12 - 13%<br />

3 900 5 574 875 956 5.2 15 - 16%<br />

propagation noticeably. At a stress The fracture surfaces of samples<br />

4 900 6.5 660 855 878 2.5 11 - 18%<br />

intensity 5 range 1030 ΔK of 20 3 MPa√m, a 610 HT1 to 765HT5/HIP 775 are smooth, 1.2 whereas 12 - 20%<br />

crack growth rate of 2.5×10 -4 mm/ the fracture surface of HT6/HIP<br />

Ti64 bars produced by SLM (average microhardness of 370 HV, as reported in Table 2) showed no<br />

significant cycle was difference observed. in hardness This value compared is to Ti64 features billet material. a higher Gas nitrided roughness. Ti64 bars High produced<br />

by in SLM good showed agreement a significant with increase the data in average microhardness, roughness of as reported the fracture in Table surface 2. Maximum is<br />

values of microhardness were recorded for a long duration of GN time for 6.5 hours (Trial 4). The<br />

lowest<br />

for solution<br />

GN temperature<br />

treated<br />

(800<br />

and overaged<br />

ºC) for 4 hours (Trial<br />

linked<br />

1) recorded<br />

to crack<br />

least<br />

closure<br />

improvement<br />

in titanium<br />

in terms of<br />

microhardness. Ti-6Al-4V exhibiting The average a bimodal microhardness showed with an increasing a large α-colony trend with size. the increase This, of GN<br />

temperature microstructure. from 800 The ºC to data 900 presently ºC, while the time together was kept same. with However, the lower with tensile the increase yield of<br />

GN time from 5 to 6.5 hours, the average microhardness increased significantly for gas nitrided<br />

Ti64 available bars at temperature shows that of the 900 plane ºC. On strain the other hand, strength, the gas nitrided leading Ti64 to bars a larger at a temperature plastic of<br />

1030 fracture ºC (above toughness -transus KIC for exceeds titanium alloys) for zone 3 hours at the (Trial crack 5) tip, showed is responsible a low average<br />

microhardness 50 MPa√m for compared all heat to Ti64 treatments. bars nitrided for 6.5 for hours the reduced (Trial 4). Maximum crack propagation values of average<br />

microhardness (660 HV) for the gas nitrided Ti64 bars produced by SLM reported low tensile<br />

properties, HT6, however, while gas nitrided causes Ti64 a distinct bars produced by rate SLM observed with high in values sample of tensile HT6/HIP. properties<br />

reported lowest values of average microhardness (505 HV). Microhardness profiles are very<br />

suitable to evaluate the extent of the N 2 diffusion into the sample. The microhardness for cross<br />

section of eight gas nitrided Ti64 bars (Trial 2 and Trial 3) produced by SLM was examined and<br />

plotted, as shown in Fig. 3.<br />

600<br />

550<br />

500<br />

450<br />

400<br />

350<br />

Trial 2<br />

Trial 3<br />

Untreated<br />

300<br />

5 10 15 20 25 30<br />

Distance from edge ( µm)<br />

Figure 3. Microhardness for cross section of Ti64 bars produced by SLM and gas nitrided at 900 ºC<br />

for 4 and 5 hours (GN Trial 2 and Trial 3)<br />

Fig. 10 Microhardness profiles through the cross-sections of Ti-6Al-4V bars<br />

produced by SLM and gas nitrided at 900ºC for 4 and 5 hours (Trial 2 and Trial 3<br />

in Table 1) [3]<br />

Influence of gas nitriding of<br />

titanium alloy bars made by<br />

Selective Laser Melting<br />

A paper presented by Stella Raynova,<br />

University of Waikato, New Zealand,<br />

on behalf of the authors Aamir<br />

Mukhtar, Peter Franz, Warwick<br />

Downing and Graeme Smith<br />

(TiDA Ltd. New Zealand) and Ben<br />

Jackson (University of Waikato),<br />

studied the influence of a gas<br />

nitriding treatment on the mechanical<br />

properties of Ti-6Al-4V bars produced<br />

by Selective Laser Melting.<br />

SLM offers a number of advantages<br />

compared to conventional<br />

production techniques such as a<br />

reduction in production steps, high<br />

material use efficiency and near net<br />

shape production capability. The layer<br />

by layer building processes in SLM<br />

enables the production of parts with a<br />

high geometrical complexity, allowing<br />

a greater freedom of design.<br />

However, the unique conditions<br />

during the SLM process can also<br />

give rise to problems. Because of the<br />

short interaction times and accompanying<br />

highly localised heat input, large<br />

thermal gradients exist during the<br />

process. These lead to the build-up<br />

of internal stresses, attributed to<br />

shrinkage during cooling. The rapid<br />

solidification also leads to segregation<br />

phenomena and the development of<br />

non-equilibrium phases (columnar<br />

growth).<br />

To overcome these problems and<br />

strengthen SLM parts, different heat<br />

treatments (i.e. stress relieving,<br />

58 Metal Additive Manufacturing | Autumn/Fall 2015<br />

© 2015 Inovar Communications Ltd Vol. 1 No. 3

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