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| | KINETICPHENOMENA |
 | | In the presence of collisions, the particle flow is no longer continuous, because particles change their velocity sharply with each collision, i.e., they disappear at specific points of velocity space and appear at other points. |
 | | Expression (5.14), therefore, is valid for multiple Coulomb collisions and for describing the interaction of an electron with wave fields (if the change of momentum and energy during absorption and emission of field quanta are sufficiently small). |
 | | We note that, in the Fokker-Planck approximation, the effect of small angle, multiple Coulomb collisions on the distribution function is similar to the effect of external fields, because in both cases the particle velocities vary in a continuous manner. |
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