Solve an ODE using Fourier series

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SUMMARY

The discussion focuses on solving the ordinary differential equation (ODE) ##y''(t)+ay(t)=y(t+\pi)## using Fourier series, specifically when the parameter ##a=(-1)^n+n^2##. The participants derive that for a non-trivial solution, the coefficients ##c_n## must satisfy the condition ##[a-(n^2+(-1)^n)]c_n=0##. They conclude that valid solutions exist for specific integer values of ##m##, leading to the forms ##c_me^{imt}+c_{-m}e^{-imt}## for non-zero ##m## and a constant solution for ##m=0##.

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  • Basic grasp of integer sequences and properties of even and odd functions.
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psie
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Homework Statement
Find the values of the constant ##a## for which the problem ##y''(t)+ay(t)=y(t+\pi), \ t\in\mathbb R##, has a solution with period ##2\pi## which is not identically zero. Determine all such solutions.
Relevant Equations
The complex Fourier series of a ##2\pi## periodic function, namely ##\sum_{n\in\mathbb Z} c_ne^{int}##.
I've assumed ##y(t)## to be the sum of a complex Fourier series, and we get $$\sum (-n^2)c_ne^{int}+\sum ac_ne^{int}=\sum c_ne^{int}e^{in\pi},$$ which we can write as $$\sum ((-n^2)+a)c_ne^{int}=\sum (-1)^n c_ne^{int}.$$ We see here that equality holds if ##a=(-1)^n+n^2##. But how do I solve ##y''(t)+ay(t)=y(t+\pi)## when ##a=(-1)^n+n^2##. I don't think I understand the problem fully.
 
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The functions ##e^{int}## are linearly independent, so you must have
$$\sum_{n=-\infty}^\infty \underbrace{[a-(n^2+(-1)^n)]c_n}_0 e^{int} = 0.$$ To get a non-trivial solution, ##a=m^2+(-1)^m## for some ##m \in \mathbb{Z}##. (Don't use ##n## because that's the dummy variable.)

What do you get if ##m=1##? ##m=2##?
 
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vela said:
What do you get if ##m=1##? ##m=2##?
Hmm, we need ##[a-(n^2+(-1)^n)]c_n## to be zero for all ##n## and we want a non-trivial solution, so ##c_n## can’t be zero for all ##n##. It can be non-zero when ##n=m##. I guess we can allow for the coefficient ##n=-m## also to be non-zero, since ##a(m)## is even.

For example, if ##m=1##, we should get ##c_1e^{it}+c_{-1}e^{-it}## being the only terms that remain. The solution takes the form ##c_me^{imt}+c_{-m}e^{-imt}## for ##m\neq 0##. For ##m=0##, we get that the only coefficient that can be nonzero is ##c_0##, a constant solution.
 
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