Abstract

AbstractNumerical solutions of a nonlinear system of equations describing the evolution of the strongly dissipative beam‐plasma instability are presented (time or space dependence of the unstable waves, the evolution of the beam distribution function and the corresponding phase space representations are given). Such an instability establishes if the linear growth rate of the unstable waves is small in comparison to the effective collision frequency of the electrons of the dissipative plasma. It is shown that after saturation of the instability there is an efficient energy transfer from the directed motion of the beam electrons to the thermal motion of the plasma electrons. Arguments are given that the strongly dissipative beam‐plasma instability is possibly the basic plasma heating mechanism which operates in the quasi‐stationary state of the beam plasma discharge. Self‐consistent initial conditions are used for the numerical calculations. Formation and evolution of dissipative structures (vortex structure, chaotic structure) were observed. A profound investigation of the chaotic or turbulent beam relaxation mechanism is presented. Such a relaxation mechanism develops in the case of the nonresonant dissipative instability (e.g. in resistive wall‐electron beam amplifiers). The method of investigation of dissipative structures presented in this paper (application of Shannon's information theory and results of the theory of dynamical systems with chaotic behaviour) can be extended to studies of other beam‐plasma systems within the framework of partial kinetic description.

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