Abstract
A new and basic theory o f ion—ion recombination as a function of gas density is developed from basic microscopic principles. A key equation for the distribution in phase space of ion pairs is derived together with an expression for the resulting rate
x
o f recombination. Further development of the theory leads to interesting insights into the full variation with N of
a
,which is shown to yield the correct limits at low and high N .The recombination rate
a
is determined by the limiting step of the rate
a
rn
for ion reaction and of the rate
a
tr
for ion transport to the reaction zone. A n analytical solution of the time-dependent Debye—Smoluchowski equation, which is a natural consequence o f this theory, is provided for transport—reaction under a general interaction
V
, for an instantaneous reaction (
a
rn
>
a
tr
) and for a finite rate (
a
rn
~
a
tr
) of reaction with in a kinetic sink rendered compressible by variation of gas density. Expressions for the transient recombination rates are then derived, and are illustrated . The exhibited time dependence lends itself to eventual experimental verification at high N. A theory that investigates the variation o f a with ion density is also developed. Here the ion—ion interaction
V
can no longer be assumed ab initio to be pure coulomb but is solved self-consistently with the recombination . Recombination rates for various systems are illustrated as a function of
N
by a simplified method for the reaction rate. Finally, two theoretical procedures are proposed for the solution o f the general phasespace ion distributions.
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