3. Experimental Results and Discussion
3-1 Effect of Ti/C atom ratio in TiCx raw powder on sintering behavior
The relationship between sintering temperature and hardness on each alloy is shown in Fig.4. W2 and W3 alloys showed higher hardness than W1 alloy in the whole range of sintering temperature, and W3 reached maximum hardness of HRA88.7 at sintering temperature of 1573K. Considering from the relationship between sintering temperature and relative density on each alloy (Fig.5) and measured results of linear shrinkage, the progress of densification was W3 alloy, W2 alloy and W1 alloy in decreasing order as compared each other at the same sintering temperature. Fig.6 shows SEM image photograph of microstructure for each alloy at sintering temperature of 1573K. For every alloys, gray white area and dark area are ß -Ti phase and TiCx phase respectively. Analyzing these photographs, it can be seen that alloy phase content of TiCx is W3 alloy, W2 alloy and W1 alloy in decreasing order. From the above, it is supposed that the reasons, which hardness of W2 and W3 alloys is higher than that of W1 alloy in the range of lower temperature, are the acceleration of densification and increase of alloy phase content of TiCx due to increase of Ti/C atom ratio in TiCx raw powder.
<Fig.4> The relationship between sintering temperature and hardness on each alloy.
<Fig.5> The relationship between sintering temperature and relative density on each alloy.
<Fig.6> SEM image of W1, W2 and W3 alloy sintered at 1573K.
Also the X-ray diffraction patterns of these alloys sintered at 1573K are shown in Fig.7. While every alloys mainly consisted of ß-Ti phase and TiCx phase, it was found that the peak of retained W increased with increase of Ti/C atom ratio. Table 3 shows the estimated Ti/C atom ratio in TiCx phase after calculating lattice parameter by peak position data of TiCx phase. Then, the reason that alloy phase content of TiCx is W3 alloy, W2 alloy and W1 alloy in decreasing order, is that Ti/C atom ratio in TiCx phase changes according to change of Ti/C atom ratio in TiCx raw powder.
<Fig.7> The X-ray diffraction patterns of W1, W2 and W3 alloys sintered at 1573K.
<Table 3> Lattice parameter and Ti/C ratio in TiCx phase of W1, W2 and W3 alloys
| |
W1 alloy (TiC1.0) |
W2 alloy (TiC0.75) |
W3 alloy (TiC0.5) |
Lattice parameter
(nm) |
4.317 |
4.314 |
4.307 |
Estimated Ti/C atom
ratio in TiCx phase |
TiC0.62 |
TiC0.60 |
TiC0.55 |
Change of Ti/C atom ratio
in TiCx phase after
sintering |
△0.38
[TiC1.0→TiC0.62] |
△0.15
[TiC0.75→TiC0.60] |
▲0.05
[TiC0.50→TiC0.55] |
Fig.8 indicates the relationship between 3 points bending transverse rupture strength (TRS) and sintering temperature on each alloy. The position of maximum TRS of W1, W2 and W3 existed at sintering temperature of 1673, 1673 and 1573K respectively, and the maximum TRS value were W3, W2 and W1 in decreasing order. The sintering temperature for maximum TRS shifted on the lower temperature side because the sintering densification was accelerated by increasing Ti/C atom ratio in TiCx raw powder as stated above.
<Fig.8> The relationship between 3 points bending transverse rupture strength (TRS)
and
sintering temperature on each alloy.
Fig.9 shows SEM image of microstructure of W1 and W3 alloy sintered at the range of 1373 to 1873K. According to the audit observation, it could be found that TRS decreased because of increase of pore up to the maximum TRS temperature, because of coarsening of ß-Ti and TiCx phase over the temperature respectively. Also, it was confirmed that for W1 alloy coarse TiCx phase was first crystallized (TiC1.0 + Ti → TiCx), that for W3 alloy the densification was accelerated through starting sintering densification among fine TiCx raw powders at lower temperature (TiCx+TiCx→TiCx').
<Fig.9> SEM images of microstructure of W1 and W3 alloy sintered at the range of 1373 to 1873K