Use the Fourier transform directly to solve the heat equation

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SUMMARY

The discussion focuses on solving the heat equation with a convection term using the Fourier transform. The equation presented is \( u_t = ku_{xx} + \mu u_x \) with the initial condition \( u(x,0) = \phi(x) \). The Fourier transform leads to the ordinary differential equation \( U_t = -k w^2 U - i w \mu U \), resulting in the solution \( U(w) = A(w) e^{(\mu i w - k w^2)t} \). Participants emphasize the importance of applying the inverse Fourier transform and the convolution theorem to retrieve the solution in the spatial domain.

PREREQUISITES
  • Understanding of Fourier transforms and their properties
  • Familiarity with solving ordinary differential equations (ODEs)
  • Knowledge of the convolution theorem
  • Basic concepts of heat equations in partial differential equations (PDEs)
NEXT STEPS
  • Study the application of the inverse Fourier transform in solving PDEs
  • Explore the convolution theorem in the context of Fourier transforms
  • Learn about the stability and boundedness conditions for solutions of heat equations
  • Investigate specific examples of initial conditions \( \phi(x) \) and their impact on the solution
USEFUL FOR

Mathematicians, physicists, and engineers working with heat transfer problems, as well as students studying partial differential equations and Fourier analysis.

richyw
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Homework Statement



Use the Fourier transform directly to solve the heat equation with a convection term
u_t =ku_{xx} +\mu u_x,\quad −infty&lt;x&lt;\infty,\: u(x,0)=\phi(x),<br /> assuming that u is bounded and k &gt; 0.<br /> <br /> <h2>Homework Equations</h2><br /> <br /> fourier transform<br /> inverse Fourier transform<br /> convolution thm<br /> <br /> <h2>The Attempt at a Solution</h2><br /> <br /> taking the FT of both sides i get <br /> U_t=-k w^2U-iw\mu U<br /> U(0,t)=\Phi(w,0)<br /> I solved the ode and got <br /> U(w)=e^{(\mu i w- w^2k)t}<br /> but now I am a bit confused on the next step, is this where I want to get my initial condition involved, or do I want to try and get it back as u(x,t) using inverse FT. I can see that my solution is a gaussian multiplied by another function of F, so I think I might be able to use convolution thm?
 
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richyw said:

Homework Statement



Use the Fourier transform directly to solve the heat equation with a convection term
u_t =ku_{xx} +\mu u_x,\quad −infty&lt;x&lt;\infty,\: u(x,0)=\phi(x),<br /> assuming that u is bounded and k &gt; 0.<br /> <br /> <h2>Homework Equations</h2><br /> <br /> fourier transform<br /> inverse Fourier transform<br /> convolution thm<br /> <br /> <h2>The Attempt at a Solution</h2><br /> <br /> taking the FT of both sides i get <br /> U_t=-k w^2U-iw\mu U<br /> U(0,t)=\Phi(w,0)
<br /> Don&#039;t you mean ##U(\omega,0) = \Phi(\omega,0)##? <br /> <br /> <blockquote data-attributes="" data-quote="" data-source="" class="bbCodeBlock bbCodeBlock--expandable bbCodeBlock--quote js-expandWatch"> <div class="bbCodeBlock-content"> <div class="bbCodeBlock-expandContent js-expandContent "> I solved the ode and got <br /> U(w)=e^{(\mu i w- w^2k)t}<br /> but now I am a bit confused on the next step, is this where I want to get my initial condition involved, or do I want to try and get it back as u(x,t) using inverse FT. I can see that my solution is a gaussian multiplied by another function of F, so I think I might be able to use convolution thm? </div> </div> </blockquote>You left out the arbitrary constant when you solved for ##U(\omega,t)##. You should have ##U(\omega,t) = A(\omega) e^{(i\mu\omega-k\omega^2)t}.##
 

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