An ideal inductor-capacitor circuit stores charge obeying

PHYSICS · Subjective · Fermi University Physics · Computational Physics · Electricity, Magnetism & Electromagnetism · Simulating classical dynamical systems

Computational Physics, Ch Stepping the equations of motion: four integrators measured

Problem

An ideal inductor-capacitor circuit stores charge q(t)q(t) obeying q¨=−q/(LC)\ddot q = -q/(LC), with L=0.20 HL = 0.20\,\mathrm{H} and C=5.0×10−4 FC = 5.0\times10^{-4}\,\mathrm{F}, so the natural angular frequency is ω0=1/LC\omega_0 = 1/\sqrt{LC}. The circuit's oscillation is integrated by plain Euler with Δt=2.0×10−4 s\Delta t = 2.0\times10^{-4}\,\mathrm{s}. (a) Without running the integration, predict the factor by which the stored energy has grown after 100100 complete oscillation periods. (b) State, without computing a new number, how the energy would behave over the same 100100 periods if the circuit were instead integrated by Euler-Cromer at the same step, using the fact that Euler-Cromer's oscillator energy is known to stay bounded within a band of a few per cent, with no trend, even after 10510^5 periods.

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