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 gives
so the wave equation becomes
Thus is independent of , and integration gives the countertravelling decomposition of the one-dimensional wave equation
Conversely, differentiating this expression twice verifies the wave equation for any sufficiently differentiable .
The two initial conditions give
Differentiating the first and solving these two equations for the derivatives gives
For a fixed reference point , their antiderivatives can be written
Substituting 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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