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Representation of Transmission Lines: Comparison of Models and Parameters Distributed Discrete Parameters

机译:传输线表示:模型和参数的比较分布式离散参数

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A transmission line is characterized by the fact that its parameters are distributed along its length. This fact makes the voltages and currents along the line to behave like waves and these are described by differential equations. In general, the differential equations mentioned are difficult to solve in the time domain, due to the convolution integral, but in the frequency domain these equations become simpler and their solutions are known. The transmission line can be represented by a cascade of π circuits. This model has the advantage of being developed directly in the time domain, but there is a need to apply numerical integration methods. In this work a comparison of the model that considers the fact that the parameters are distributed (Universal Line Model) and the fact that the parameters considered concentrated along the line (π circuit model) using the trapezoidal integration method, and Simpson's rule Runge-Kutta in a single-phase transmission line length of 100 km subjected to an operation power.
机译:传输线的特征在于其参数沿其长度分布。这一事实使沿线的电压和电流表现得像波,并且这些都由微分方程描述。通常,由于卷积积分,提到的微分方程在时域中很难求解,但是在频域中,这些方程变得更简单并且其解是已知的。传输线可以由π电路的级联表示。该模型的优点是可以直接在时域中进行开发,但是需要应用数值积分方法。在这项工作中,模型的比较考虑了参数分布的事实(通用线模型)和使用梯形积分法和辛普森法则的Runge-Kutta来考虑的参数沿线集中的事实(π电路模型)。在100 km的单相传输线中,其长度要受到工作功率的影响。

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