Resonance problem involving Laplace transformations

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SUMMARY

The discussion focuses on determining the resonance conditions for a harmonic oscillator described by the differential equation y'' + ω²y, driven by half- and full-wave rectified sine waves. It establishes that the sine wave sin(t) drives the oscillator into resonance at ω = 1. The Laplace transform of the half-wave rectified sine wave is given by Y(s) = (1 + e^{-sπ}) / [(s² + 1)(1 - e^{-s2π})(s² + ω²)] + (sy(0) + y'(0)) / (s² + ω²). Participants express uncertainty about handling the term (1 - e^{-s2π}) in the denominator while finding the poles of Y(s).

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Homework Statement



The sine wave sin(t) will only drive the harmonic oscillator y'' + \omega ^2 y into resonance when \omega = 1. For what values of \omega will the half- and full-wave rectified sine waves drive the harmonic oscillator into resonance.

Homework Equations





The Attempt at a Solution



Starting with the half-wave rectified sine wave;

Taking the Laplace transform of both sides and rearranging for Y(s);

Y(s)= \frac{1+e^{-s\pi}}{(s^2+1)(1-e^{-s2\pi})(s^2+ \omega ^2)} + \frac{sy(0)+y'(0)}{s^2+\omega^2}


From here I think I need to find the poles of Y(s) but I am unsure what to do with the (1-e^{-s2\pi}) in the denominator of the first term. Similar problem when looking at the full-wave rectified sine curve.
 
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Ok, first of all, this is the math part of the forum, so if you want help solving an ODE, you'll have to actually tell us what it is -- we won't necessarily know what you mean simply by giving a physical description.
 

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