For a classical solution take twice differentiable, so that the second derivatives exist. Direct use of the chain rule giveswith the two profile arguments as specified. Thus .
To prove generality, introduce characteristic coordinates , , whose Jacobian determinant is . For the differential operator isThe equation becomes . Integrating once in each variable yieldsThis is the countertravelling decomposition of the one-dimensional wave equation, with wave speed . Once differentiability alone is not sufficient for a classical second-order equation; the displayed argument uses the required second derivatives.
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