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Boltzmann relation : ウィキペディア英語版
Boltzmann relation

In a plasma, the Boltzmann relation describes the number density of an isothermal charged particle fluid when the thermal and the electrostatic forces acting on the fluid have reached equilibrium.
In many situations, the electron density of a plasma is assumed to behave according to the Boltzmann relation, due to their small mass and high mobility.
==Equation==

If the local electrostatic potentials at two nearby locations are φ1 and φ2, the Boltzmann relation for the electrons takes the form:
:n_e (\phi_2) = n_e(\phi_1) e^
where ''n''e is the electron number density, ''T''e the temperature of the plasma, and ''k''B is Boltzmann constant.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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