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Homework Statement
Show that if the displacement of the waves on a membrane of width b is given by the superposition
z=A_1\exp^{i(\omega t-(k_1x+k_2y))}+A_2\exp^{i(\omega t-(k_1x-k_2y))}
with z=0 when y=0 and y=b then the real part of z is
z=2A_1sin(k_2)sin(\omega t-k_1x) where k_2=\frac{n\pi}{b}
Homework Equations
The Attempt at a Solution
So I've found that A_1=-A_2 and k_2=\frac{n\pi}{b}, but I don't quite see how I can show that the real part of z is z=2A_1sin(k_2)sin(\omega t-k_1x). Can someone please provide some guidance?