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chemical physics of discharges - Argonne National Laboratory

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Again if this power gain is equated to the loss <strong>of</strong> energy <strong>of</strong> electrons in<br />

elastic collisions with the gas molecules, as would occur in the steady state, then<br />

qEo<br />

where a f -. m<br />

E<br />

8<br />

From (26) one would expect the electron "temDerature" for fixed Eo to diminish<br />

with increasing frequency, but for pressures <strong>of</strong> the order <strong>of</strong> one torr and gas masses<br />

<strong>of</strong> around 30 AMU the electron temperature will remain near the dc value for frequencies<br />

usually employed for gas discharge work.<br />

B. Elastic Collisions, and Diffusion<br />

-<br />

Since in either dc or ac <strong>discharges</strong>, the electrons will have high temperatures,<br />

one can expect that all the manifestations <strong>of</strong> a kinetic temperature will be present.<br />

Particularly important among these is diffusion through elastic collisions. If only<br />

electrons are present in a neutral gas they will tend to diffuse as would any other<br />

gaseous component with a current density<br />

where ne is the number density <strong>of</strong> the electrons and De is the diffusion coefficient <strong>of</strong><br />

the electrons through the gas.<br />

will contain a mobility term as well so that<br />

I<br />

(25)<br />

If a field is also superposed, the current density \<br />

,<br />

where the minus sign in the second term indicates that because <strong>of</strong> the negative charge 4<br />

on the electrons, their motion will try to be in the direction opposite to that Of<br />

the applied field. pe is taken to be a positive number. Whether the electron motion<br />

is diffusion-dominated or field dominated depends on whether the first term<br />

l<br />

is larger<br />

'1

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