Take the constant speed parameter , so and are independent characteristic coordinates. The chain rule gives
Applying these operators twice to a twice differentiable function yields
Consequently the wave equation reduces to . Integrate first with respect to , obtaining , and then with respect to , allowing a separate integration function of . The general local solution is
with arbitrary sufficiently differentiable functions and . For , the first profile travels towards negative and the second towards positive . Substitution directly checks the equation. Initial or boundary conditions select the two profiles; none are specified here. This is D'Alembert's formula in characteristic form.

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