Write , where and . The chain rule givesFor a twice continuously differentiable classical solution, mixed partial derivatives commute, so the wave equation becomesHence depends only on . Integrating first in yields the countertravelling decomposition of the one-dimensional wave equation:On a rectangular domain in this follows immediately; on the full line for , the connected characteristic slices give the same representation. The two terms travel at wave speed one in opposite directions.
Impose the initial conditions. At ,Differentiate the first identity and combine:If , then and . Substitution cancels and the arbitrary base point , giving D'Alembert's formula:For example, and make this a classical solution of the wave equation satisfying both initial conditions. The same formula defines a weak solution for less regular data, including the continuous piecewise smooth data of part (b).
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