Solving Integral Using Laplace Transform

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Discussion Overview

The discussion revolves around the computation of the integral $$ \int_0^ \infty \frac{ \cos xt}{1 + t^2} \, dt $$ using different transform methods, specifically the Laplace transform and the Fourier transform. The scope includes mathematical reasoning and exploration of various approaches to solve the integral.

Discussion Character

  • Exploratory, Technical explanation, Debate/contested, Mathematical reasoning

Main Points Raised

  • One participant suggests using the Laplace transform, noting the factor \( \frac{1}{1 + t^2} \) relates to the Laplace transform of \( \sin x \).
  • Another participant proposes using the Fourier transform instead, arguing it is simpler and provides an alternative formulation of the integral.
  • A later reply asks if there is a way to approach the problem using the Laplace transform despite the preference for the Fourier method.
  • Another participant speculates about potentially using the convolution theorem as a method to solve the integral.

Areas of Agreement / Disagreement

Participants express differing preferences for using the Laplace transform versus the Fourier transform, indicating a lack of consensus on the best approach to solve the integral.

Contextual Notes

Participants have not resolved the mathematical steps involved in applying the Laplace transform, and there are assumptions about the applicability of different transformation methods that remain unexamined.

pierce15
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I posted this in the homework section, but I haven't received any help, so hopefully putting it in this section won't be an issue. I'm trying to compute the integral

$$ \int_0^ \infty \frac{ \cos xt}{1 + t^2} \, dt $$

using the Laplace transform. The first thing that catches my eye is the 1 /(1 + t^2) factor, which is equal to the Laplace transform of sin x:

$$ = \int_0^\infty \cos xt \, L[ \sin x ] \, dt $$

Any ideas?
 
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Why do you want to use the Laplace transformation here? I'd rather use the Fourier transformation. It's simpler to put it first in the exponential form. Your Integral is
[tex]F(x)=\frac{1}{2}\int_0^{\infty} \frac{\exp(\mathrm{i} x t)+\exp(-\mathrm{i} x t)}{1+t^2}.[/tex]
Substituting [itex]t'=-t[/itex] in the second integral you get after some algebra
[tex]F(x)=\frac{1}{2} \int_{-\infty}^{\infty} \frac{\exp(\mathrm{i} x t)}{1+t^2}. \qquad (1)[/tex]
Now we use the fact that
[tex]\int_{-\infty}^{\infty} \frac{\mathrm{d} x}{2 \pi} \exp(-|x|) \exp(-\mathrm{i} t x)=\frac{1}{\pi (1+t^2)}.[/tex]
Thus (1) is (up to a factor [itex]\pi/2[/itex]) the inverse of this Fourier transform. This gives
[tex]F(x)=\frac{\pi \exp(-|x|)}{2}.[/tex]
 
Ok, thanks for that. Do you also see any way to do it with the Laplace transform?
 
Hm, I've no idea. Perhaps you can somehow use the convolution theorem with some clever trick?
 

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