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

机译:具有非线性频移和增长饱和效应的驱动和相互耦合的相对论磁控管模型

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Abstract: 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:摘要:从动范德波尔-达芬方程已被用于建模由外部锁定信号驱动的相对论磁控管的行为。作者继续研究驱动的范德波尔-达芬方程,并提出了研究范德波尔-达芬方程作为相互耦合的相对论磁控管模型的初步结果。提出了一种在信号X(t)及其时间导数X(t)均可用的情况下,以缓慢变化的幅度近似确定信号的幅度和相位的方法。当将二阶微分方程和此类方程的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)均可用。在这种情况下,可以确定幅度和相位而无需在快速时标上求平均值。因此,保留了某些动态信息,如果有必要在快速的时间范围内进行平均,则会丢失这些动态信息。在相互驱动配置中,两个振荡器线性地与时间延迟线性耦合的情况下,为了简化问题,使用了缓慢变化的幅度和相位近似。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。研究此系统的重要步骤是确定固定振幅和相位差。在振荡器之间的频率不匹配为零且最优耦合延迟相位为零的情况下,通过耦合质量因子和振荡器增长率与固有频率之比的函数,可以分析得出固定幅度和耦合功率。除非这些参数足够大,否则将无法实现由于耦合而导致的相干功率的潜在增加。

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