With and ,
so the wave equation becomes
Thus . At the initial data give
Solving for and and integrating gives d'Alembert's formula>
Extend the forcing oddly across the boundary:
The initial displacement is already odd, so its homogeneous evolution on the line is . Applying Duhamel's principle to the odd extension gives
The odd-reflection method makes . At the double integral vanishes together with its first time derivative, so the prescribed initial displacement and velocity are also satisfied.

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