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Models of driven and mutually coupled relativistic magnetrons with nonlinear frequency-shift and growth-saturation effects

机译:具有非线性频移和生长饱和效应的驱动和相互耦合的相互耦合的相互耦合磁控磁控磁控磁像

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The driven van der Pol-Duffing equation has been used to model the behavior of a relativistic magnetron driven by an external locking signal. The authors continue the study of the driven van der Pol-Duffing equation and present initial results of the investigation of coupled van der Pol-Duffing equations as models of mutually coupled relativistic magnetrons. A method is presented for determining the amplitude and phase of a signal in the slowly-varying amplitude approximation in the case that both the signal, X(t), and its time derivative, X(t), are available. When second-order differential equations and coupled systems of such equations are used as models of driven and coupled nonlinear oscillators, both X(t) and X(t) are available. In this case, it is possible to determine the amplitude and phase without averaging over a fast time scale. Thus certain dynamical information is retained that is lost if it is necessary to average over a fast time scale. In the case of two oscillators linearly coupled with time delays in the mutual drive configuration, the slowly varying amplitude and phase approximation has been used in order to simplify the problem. In general, behavior of the oscillator amplitudes, as well as the phase difference between oscillators, must be considered. An essential step in studying this system is the determination of stationary amplitudes and phase difference. In the case of zero frequency mismatch between oscillators and optimum coupling delay phase, stationary amplitudes and coupled power are obtained analytically as functions of coupling quality factor and ratio of oscillator growth rate to natural frequency. Unless these parameters are sufficiently large, the potential increase in coherent power delivered due to coupling will not be realized.
机译:已经用于将由外部锁定信号驱动的相对论磁控管的行为模拟了由外部锁定信号的相位磁控管的行为。作者继续研究从动van der Pol-Duffing方程的研究,并将耦合范德波·杜蹄型方程的研究的初始结果作为相互耦合的相对论磁控管的模型。提出了一种方法,用于确定信号,x(t)及其时间导数x(t)的情况下的缓慢变化幅度近似中的信号的幅度和相位。当这种等式的二阶微分方程和耦合系统用作驱动和耦合非线性振荡器的模型时,x(t)和x(t)都可用。在这种情况下,可以在不在快速时间尺度上平均的情况下确定幅度和阶段。因此,如果在快速时间尺度上是必要的,则保留某些动态信息。在两个振荡器线性耦合的振荡器的情况下,使用缓慢变化的幅度和相位近似以简化问题。通常,必须考虑振荡器幅度的行为以及振荡器之间的相位差。研究该系统的重要步骤是确定静止幅度和相位差。在振荡器和最佳耦合延迟阶段之间的零频失配的情况下,分析地获得固定幅度和耦合功率,作为耦合质量因子和振荡器生长速率与自然频率的比率的函数。除非这些参数足够大,否则不会实现由于耦合而递送的相干功率的潜在增加。

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