Differential equation with twosided decay exponential

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Homework Help Overview

The discussion revolves around solving a differential equation of the form y''(t) - k^2 y(t) = e^{-a|t|}, where a and k are positive real numbers. The original poster attempts to find a solution using Fourier transforms but encounters issues with the absolute value in the exponential term.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the original poster's approach of using Fourier transforms and question the handling of the absolute value in the exponential function. Suggestions include branching the solution into two cases based on the sign of t and evaluating the Fourier transform separately for each case.

Discussion Status

There is ongoing exploration of the problem, with participants offering different perspectives on how to approach the solution. Some guidance has been provided regarding the need to consider the absolute value in the context of the Fourier transform, but no consensus has been reached on the correct method to unify the solutions for both cases.

Contextual Notes

The discussion highlights the challenge of incorporating the absolute value in the solution and the implications of the Fourier transform on the resulting function. Participants express uncertainty about the mathematical reasoning behind the observed behavior of the solution across the domain.

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Homework Statement


Solve
y''(t) - k^2 y(t) = e^{-a|t|} where a and k are both positive and real.

Homework Equations



The solution was obtained trough a Fourier transform.

The Attempt at a Solution



I got the solution

y(t) = \frac{ke^{-at} - ae^{-kt}}{k(a^2 - k^2)}

but when i plug it back into the differential equation i just get
e^{-at}
how could I get the absolute value back in there?

Might there be anything wrong with my solution procedure?
 
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Start your solution again but branch it into two cases straight away, one for t\geq 0 and another for t < 0. Solve them separately, then only at the end try to unify them into 1 solution.
 
Hmm.. Where might this branching take place? I considered to do a branch when i took the Fourier transform of e^{-a|t|}, but here i found that

\int_{-\infty}^{\infty} e^{-a |t|}e^{-i \omega t} dt = \int_{-\infty}^{\infty} e^{-a |t|} ( \cos(\omega t) + i \sin (\omega t)) dt

so the sine term drops out and since the rest of the integrand is even we're left with

2 \int_{0}^{\infty} e^{-a t } \cos(\omega t) dt

which I evaluated, isolated for Y(\omega) and took the inverse transform.
 
I can't see anything wrong with that so frustratingly I can't see a mathematical reason as to why the solution only ending up solving correctly for half the domain. In any case though, to fix you solution you can just replace all t's with |t|'s .
 
That's very weird indeed. I know that I got the right transform.. and I don't see how that absolute value can appear in the inverse transform which is just
y(t) = \frac{1}{\sqrt{2 \pi}} \int_{-\infty}^{\infty} Y(\omega) e^{i \omega} d\omega
Well thanks for helping me out anyway! You've been really helpfull :)
 

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