What are the differences between laplace & fourier transform

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SUMMARY

The discussion clarifies the distinct applications of Laplace and Fourier transforms in solving partial differential equations (PDEs). Laplace transforms are primarily utilized when initial conditions are defined at time t=0, allowing for the incorporation of these conditions into the transformed equations. In contrast, Fourier transforms are advantageous for analyzing spatial variables, particularly when combined with Laplace transforms to simplify PDEs. This hybrid approach facilitates the derivation of Green's functions, essential for various applications in mathematical physics.

PREREQUISITES
  • Understanding of partial differential equations (PDEs)
  • Familiarity with Laplace transforms
  • Knowledge of Fourier transforms
  • Basic concepts of Green's functions
NEXT STEPS
  • Study the application of Laplace transforms in initial value problems
  • Explore Fourier transforms in the context of signal processing
  • Learn about the derivation and applications of Green's functions
  • Investigate the Fourier-Laplace transform technique for solving PDEs
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Mathematicians, engineers, and physicists who are involved in solving differential equations and analyzing systems with initial conditions will benefit from this discussion.

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What are the differences?
I mean when we will make a decision "hmm now i must use laplace transform or now i must use Fourier transform".

What are the absences in laplace transform so Fourier design a new transfom?

I want to know these transforms' main idea, differences.

I am looking for your answers.

Thanks .
Sincerely;
 
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in applications you usually use Laplace transforms when you have initial conditions for a p.d.e. and u start at t=0. Thats because when you Laplace transform derivatives you get the initial conditions into the p.d.e.

Often you Fourier-Laplace transforms differential equations too. If you have a p.d.e. for u(r,t) you can Fourier transform the position and Laplace transform the time. Then you get an easier equation for
u(k,z), where k is the wave-vector. This is very useful when you want to derive the Greenfunction for a particular problem.
 

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