For , let denote the time factor normalized by , . By superposition the Fourier sine series solution is
At , its initial velocity is . Multiply by , integrate on , and use the permitted interchange and Fourier orthogonality. This yields the requested integral expression
Under , is unchanged and . Hence every even-index Fourier coefficient is zero, including .
For odd , use and the product-to-sum formula:
Thus
In particular and . An explicit version of the solution of a differential equation is
Only the first, overdamped normal mode, the third, critically damped normal mode, and the odd underdamped normal modes of index at least five occur. No odd-index Fourier coefficient vanishes.

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