The printed arguments and assume unit wave speed. For the stated wave equation with general , the correct arguments are and , as in the paper's subsequent formula. Equivalently, use rescaled time to obtain the printed unit-speed form.
Introduce coordinates , along the characteristic lines for the one-dimensional wave equation, and write . The chain rule givesso the wave equation becomesThus is independent of , and integration gives the countertravelling decomposition of the one-dimensional wave equationConversely, differentiating this expression twice verifies the wave equation for any sufficiently differentiable .
The two initial conditions giveDifferentiating the first and solving these two equations for the derivatives givesFor a fixed reference point , their antiderivatives can be writtenSubstituting the two travelling arguments cancels the constants and combines the integrals. This proves D'Alembert's formula with initial velocity:At the integral vanishes, giving ; differentiating by the fundamental theorem of calculus gives there. These checks also fix the sign and the factor .
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