How should I show that solutions can be expressed as a Fourier series?

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Homework Help Overview

The discussion revolves around expressing solutions of a differential equation as a Fourier series. The context involves a second-order linear differential equation with periodic solutions, specifically focusing on the angular frequency and its representation in series form.

Discussion Character

  • Exploratory, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants are exploring how to represent solutions of the differential equation in terms of a Fourier series. There are inquiries about the necessary steps to demonstrate this representation and the implications of the periodic nature of the solutions.

Discussion Status

The discussion is ongoing, with participants seeking clarification on the work done so far and how to proceed with substituting the proposed series into the differential equation. Guidance has been offered regarding the substitution of the series form to analyze the relationship between the angular frequency and the coefficients.

Contextual Notes

There is an emphasis on understanding the periodicity of the solutions and the specific form of the Fourier series being considered. Participants are also reflecting on the initial conditions and their impact on the solution's representation.

Math100
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Homework Statement
Consider the equation ## \ddot{x}+x+\epsilon(\alpha x^2\operatorname{sgn}(x)+\beta x^3)=0, 0<\epsilon<<1, \alpha>0, \beta>0 ##, where ## \alpha ## and ## \beta ## are constants, and the signum function, ## \operatorname{sgn}(x) ##, is defined by ## \operatorname{sgn}(x)=1 ## for ## x>0 ##, ## \operatorname{sgn}(x)=0 ## for ## x=0 ## and ## \operatorname{sgn}(x)=-1 ## for ## x<0 ##. With initial condition ## x(0)=0 ##, show that solutions with angular frequency ## \omega ## can be expressed as a Fourier series of the form ## x(t)=\sum_{k=1}^{\infty}B_{2k-1}\sin((2k-1)\omega t)=B_{1}\sin\omega t+B_{3}\sin 3\omega t+\cdots ##.
Relevant Equations
None.
Proof:

Let ## \epsilon=0 ##.
Then the unperturbed equation is ## \ddot{x}+x=0 ## and the general solution is
## x(t)=A\sin\omega t+B\cos\omega t ## where ## \omega=1 ## is the angular frequency
with the constants ## A ## and ## B ##.
With the initial condition ## x(0)=0 ##, we have that ## B=0 ##.
This gives ## x(t)=A\sin\omega t ## where ## A ## is a constant.
Note that the function of ## x(t)=A\sin\omega t ## is periodic and odd.

From the work/proof shown above, how should I show that solutions with angular frequency ## \omega ##
can be expressed as a Fourier series of the given form on the problem? What needs to be done?
 
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Math100 said:
From the work/proof shown above, how should I show that solutions with angular frequency ## \omega ##
can be expressed as a Fourier series of the given form on the problem? What needs to be done?
Can you show the work you've done on this problem so far?
 
renormalize said:
Can you show the work you've done on this problem so far?
That's all the work I have so far.
 
Math100 said:
That's all the work I have so far.
OK, can you substitute the form ##x(t)=\sum_{k=1}^{\infty}B_{2k-1}\sin((2k-1)\omega t)=B_{1}\sin\omega t+B_{3}\sin 3\omega t+\cdots## into the differential equation to see what you can learn about ##\omega## and the coefficients ##B_{2k-1}##?
 

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