Given an arbitrary harmonic solution to the wave equation
find the general solution, i.e. find the coefficients and given the following boundary conditions:
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The condition y ( 0 , t ) = 0 gives the condition B − A = 0 on the coefficients, i.e. A = B . The condition y ( L , 0 ) = 1 then gives:
1 = A sin L + A sin L ⟹ A = 2 sin L 1 .
Substituting in, one finds the solution:
y ( x , t ) = 2 sin L 1 sin ( x − v t ) + 2 sin L 1 sin ( x + v t ) = sin L sin x cos v t .