The Richardson-Dushman equation relates the current density of a thermionic emission to the work function (W) and temperature (T) of the emitting material:
js = A T2 exp(-W/kT)
where
js is the current density of the emission (mA/mm2)
A is Richardson's constant (approx. 1202 mA/mm2K2).
T is temperature (K)
W is the work function of the cathode material (J)
k is the Boltzmann constant (1.38066E-23 J/K)
In Cathode Emissions in CPO, A is treated as an empirical constant. In fact, js may be entered directly.
