A method of modulating the amplitude and phase of multifrequency signals DEVICE AND ITS IMPLEMENTATION

摘要

the device of the method u043cu043eu0434u0443u043bu00a0u0446u0438u0438 amplitude and phase u043cu043du043eu0433u043eu0447u0430u0441u0442u043eu0442u043du044bu0445 signals u0441u043eu0441u0442u043eu00a0u0449u0435u0435 from a high-frequency signal u043du0435u0443u043fu0440u0430u0432u043bu00a0u0435u043cu043eu0439 part quite u043du043du043eu0439 as reactive u0447u0435u0442u044bu0440u0435u0445u043fu043eu043bu044eu0441u043du0438u043au0430, u0443u043fu0440u0430u0432u043bu00a0u0435u043cu043eu0439 part connected in parallel to a source of low frequency u0443u043fu0440u0430u0432u043bu00a0u044eu0449u0435u0433u043e signal u043eu0442u043bu0438u0447u0430u044eu0449u0435u0435u0441u00a0, cb u0440u0430u0432u043bu00a0u0435u043cu0430u00a0 part is in the form of u0442u0440u0435u0445u043fu043eu043bu044eu0441u043du043eu0433u043e u0443u043fu0440u0430u0432u043bu00a0u0435u043cu043eu0433u043e elementincluded u043du0435u0443u043fu0440u0430u0432u043bu00a0u0435u043cu043eu0439 part and the load, a u0447u0435u0442u044bu0440u0435u0445u043fu043eu043bu044eu0441u043du0438u043a designed as a symmetrical bridge circuit u0441u043eu0435u0434u0438u043du0435u043du0438u00a0 four jet u0434u0432u0443u0445u043fu043eu043bu044eu0441u043du0438 in parallel to this connection includes a load u0434u043bu00a0 pass high-frequency signal with arbitrary u0438u043cu043fu0435u0434u0430u043du0441u0430u043cu0438 at three specified frequencies and u0434u0432u0443u0445u043fu043eu043bu044eu0441u043d ica with rockets u0441u043eu043fu0440u043eu0442u0438u0432u043bu0435u043du0438u00a0u043cu0438 u04451k, u04452k, u04453k,X4k symmetrical pavement scheme implemented in sequential circuit Ln, cn, in parallel to the u0438u043du0434u0443u043au0442u0438u0432u043du043eu0441u0442u044cu044e L0n, with jet u0441u043eu043fu0440u043eu0442u0438u0432u043bu0435u043du0438u00a0 u0434u0432u0443u0445u043f u043eu043bu044eu0441u043du0438u043au043eu0432 at each of the three fixed frequency k chosen by the following mathematical expression.;X1k = X3k = - x22 - x21; X2k = X4k = - x22 + x21;;;;;;;;where;;; k = 1, 2, 3 - number; n = 1, 2, 3 is the number of u0434u0432u0443u0445u043fu043eu043bu044eu0441u043du0438u043au0430 u0441u0447u0438u0442u0430u00a0 by high-frequency signal source;;;;;;;;;;;;;;;;;;;;;;;; r0k, x0k - real and imaginary parts of the complex u0441u043eu043fu0440u043eu0442u0438u0432u043bu0435u043du0438u00a0 raised source signal; ru043dk, u0445u043dk raised real and imaginary part of the complex is u0441u043eu043fu0440u043eu0442u0438 u0432u043bu0435u043du0438u00a0;; workload;;;; real and imaginary parts of the complex by the matrix elements u0441u043eu043fu0440u043eu0442u0438u0432u043bu0435u043du0438u0439 u0442u0440u0435u0445u043fu043eu043bu044eu0441u043du043eu0433u043e u0443u043fu0440u0430u0432u043bu00a0u0435u043cu043eu0433u043e element in two u0441u043eu0441u0442u043eu00a0u043du0438u00a0u0445, u043eu043fu0440u0435u0434u0435u043bu00a0u0435u043cu044bu0445 two u00a0 u0443u0440u043eu0432u043du00a0u043cu0438 current and u043du0430u043fu0440u00a0u0436u0435u043du0438u00a0 low-frequency signal source u0443u043fu0440u0430u0432u043bu00a0u044eu0449u0435u0433u043e; m21n, 21n - raised u043eu0442u043du043eu0448u0435u043du0438u00a0 modules and the phases of the transfer in the two sta u043eu00a0u043du0438u00a0u0445 u0443u043fu0440u0430u0432u043bu00a0u0435u043cu043eu0433u043e elements at three frequencies; u044522,x21 - optimal numerical u0437u043du0430u0447u0435u043du0438u00a0 matrix elements u0441u043eu043fu0440u043eu0442u0438u0432u043bu0435u043du0438u0439.