Periodic Solutions to DE with Extra Condition: Solving for Unknown Constants

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The discussion focuses on solving the differential equation f'' + λf = 0 with the periodic condition f(r) = f(r + π). For λ = 0, the solution is a constant, while for other values of λ, substituting λ = k² leads to the general solution f(r) = A cos(kr) + B sin(kr). The periodic condition results in a relationship that indicates k must be an even integer, which directly influences the value of λ. This understanding helps specify the solutions further based on the periodicity condition.
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I don't know how to use the extra condition given in the this problem:


f^{\prime\prime}+\lambda f = 0, f=f\left(r\right)
f\left(r\right) = f\left(r+\pi\right)

For \lambda = 0, the solution is some constant.
For other \lambda, I put \lambda=k^2, and get


f^{\prime\prime}+k^2 f = 0,

which has the solution


f\left(r\right)=A\cos\left(kr\right)+B\sin\left(kr\right).

The condition now gives


A\cos\left(kr\right)+B\sin\left(kr\right)=<br /> A\cos\left(kr+k\pi\right)+B\sin\left(kr+k\pi\right).

How can I use this to further specify the solution?
 
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Well, you know that \cos{x} + \sin{x} = \cos{(x+2n\pi)} + \sin{(x+2n\pi)} for all x only when n is an integer. What does that tell you about k, and therefore \lambda?
 
Oh, right, so k must be an even integer.
Thank you. :smile:
 
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