Abstract

This paper describes a new solution formulation for fully nonlinear and unsteady planar flow of an electron beam in a diode. Using characteristic variables - i.e., variables that follow particle paths - the solution is expressed through an exact analytic, but implicit, formula for any choice of incoming velocity v0v_0, electric field E0E_0 and current J0J_0. For steady solutions, this approach clarifies the origin of the maximal current JmaxJ_max, derived by Child and Langmuir for v0=0v_0=0 and by Jaffe for v0>0v_0>0. The implicit formulation is used to find (1) unsteady solutions having constant incoming flux J0>JmaxJ_0>J_max, which leads formation of a virtual cathode, and (2) time-periodic solutions whose average flux exceeds the adiabatic average of JmaxJ_max.

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