Due
to the high thermal conductivity of Cu, and the better spark erosion
resistance, low thermal expansion coefficient and high melting temperature of
W, tungsten copper electrodes have been widely used for machining die steel and
tungsten carbide work-piece. The materials normally used in EDM electrodes are
various types of copper, graphite, tungsten, brass and silver. But
copper-tungsten has better properties. The low melting point of Cu reduces the
resistance to electrode wear.
At high tungsten content, there is porosity in the
liquid phase sintered electrode due to the insolubility between the Cu and W.
This greatly impedes densification during the solution-reprecipitation stage of
liquid phase sintering. Hence, this makes it necessary to introduce another
material with high melting point. Materials having good electrical and thermal
conductivity with a high melting point are used preferably in copper-based
electrodes to resist electrode shape-loss.
Titanium
carbide (TiC) is an extremely hard refractory material with high melting
temperature, and high thermal shock and abrasion resistance. It is used mainly
for powder metallurgical parts including cutting tool tips, dies, wear parts
and resistant coating. In industry, the manufacturing of Cu-W composites is
usually done through infiltration of Cu into a porous, pre-sintered tungsten
compact, or through the liquid phase sintering of compacts pressed from mixed
powder.
In some researches, Cu-W/TiC was investigated and fabricated
through liquid phase sintering. In is reported that the additive metals (iron,
cobalt and nickel) can enhance densification in the liquid phase sintering of
Cu-W. In order to increase the densification of the Cu-W matrix, nickel (Ni)
was introduced. In addition, the densification of Cu-W/TiC sintered electrodes
can be improved by the addition of Ni. However, due to the insolubility of Cu,
W and Tic, and the amount of Cu apparently reduced by the cold welding in ball
milling, porosity cannot be avoided. Nevertheless, with increasing TiC, the
distribution of the particle size becomes narrow.
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