G. Lins et al., THE THERMAL-BEHAVIOR OF TANTALUM CARBIDE CATHODES IN PSEUDOSPARK SWITCHES, IEEE transactions on plasma science, 23(3), 1995, pp. 375-380
Pseudospark cathodes made of either tungsten, tungsten with an additio
n of rhenium (WRe26), or tungsten with inclusions of tantalum carbide
grains (WRe3TaC30) were investigated by laser-induced fluorescence on
metal vapors and by measurements of the cathode power loss, Excitation
temperatures of tungsten vapor are considerably higher (T-ex less tha
n or equal to 8300 K) for the purely metallic cathodes than for WRe3Ta
C30 (T-ex less than or equal to 4000 K), Furthermore;the increase of t
he excitation temperature with the current amplitude, dT(ex)/di, is ab
out ten times less for WRe3TaC30 than for the other materials, Similar
ly, the cathode surface temperature T-s estimated from a comparison of
the ratio of vapor densities of tungsten and rhenium with the ratio o
f their equilibrium vapor pressures is much higher (T-s approximate to
7000 K) for WRe26 than for WRe3TaC30 (T-s approximate to 4500 K, Fina
lly, the power loss to the cathode is about equal for the tungsten and
WRe26 cathodes (e,g,, 200 W at a repetition rate of 230 Hz and 9-kA p
eak current), but it is 30% less for the tantalum carbide cathode, irr
espective of the pulse repetition rate, Consequently, due to their low
er power dissipation, WRe3TaC30 cathodes can be used for much higher c
urrents than the purely metallic cathodes. The physical reason for the
favorable thermal behavior of the WRe3TaC30 cathode is attributed to
the fact that the electrical conductivity of tantalum carbide increase
s with increasing temperature.