For and , D'Alembert's formula for the wave equation on the full real line isFor the specified initial data, define the cumulative initial-velocity integralThen . The initial velocity jumps at , so the resulting solution is interpreted piecewise classically, or as a weak wave-equation solution across the corresponding characteristic curves.
At , the interval of integration has half-width . Evaluating the cumulative integral in part a gives the even functionIt has value at zero and maxima at , then falls to zero at the two wavefronts.
At , the integration interval first moves through positive arguments, then crosses zero, and finally contains all of . The result isThe final plateau is the integral of the entire initial velocity profile divided by .
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