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2.7 Time-Domain Analysis of Nonlinear Dynamic Circuits 119<br />

equations is then solved for the voltages and currents using the multi-dimensional Newton-Raphson<br />

method.<br />

Circuit equations are usually stiff, which means that their solutions involve both very rapid and very<br />

slow transients. To avoid loss of accuracy and convergence problems during rapid transients as well<br />

as excessive computation time requirements for slow transients the step size is chosen adaptively at<br />

each time step according to the curvature of the waveform. Whenever a waveform changes quickly<br />

the step size is cut back whereas it is increased during periods of latency. The behavior of the<br />

step size control algorithm depends on the values of five parameters which will be discussed in the<br />

following section. The associated NDAESolve options by which the default parameter settings can be<br />

changed are StartingStepSize, MaxStepSize, MinStepSize, StepSizeFactor, and MaxDelta.<br />

Figure 7.3 shows a flow graph of the algorithm implemented in NDAESolve.

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