Fourier Transform to solve heat equation in infinite domain

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Homework Help Overview

The discussion revolves around the application of the Fourier Transform to solve the heat equation in an infinite domain. The heat equation is presented, and participants are examining the steps involved in transforming and integrating the equation.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants are discussing the integration of the transformed equation with respect to time and the implications of including a function of alpha as part of the solution. Questions are raised about the nature of the integration constant and its dependence on the variables involved.

Discussion Status

There is an ongoing exploration of the integration process and the role of the constant term in the solution. Participants are clarifying concepts related to arbitrary functions and their relevance in the context of partial differential equations.

Contextual Notes

Participants are navigating the complexities of integrating functions that depend on multiple variables and discussing the implications of treating constants as functions of other variables in the context of solving differential equations.

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I'm having trouble following a step in my notes:

first off the heat equation is given by:

[tex]\frac{\partial u}{\partial t}=k^{2}\frac{\partial^{2}u}{\partial x^{2}}[/tex]

then take the Fourier transform of this w.r.t.x, where in this notation the Ftransform of u(x,t) is denoted by U(alpha,t):

[tex]\frac{\partial U}{\partial t}=-\alpha^{2}k^{2}U[/tex]

***it is this step I don't quite follow**** integrate with respect to t:

[tex]U=c(\alpha)e^{-k^{2}\alpha^{2}t}[/tex]

Can someone please explain this step ie. how do you know what limits to integrate between and how do you know that the rights side of the equation ends up in the form?:

[tex]c(\alpha)e^{-k^{2}\alpha^{2}t}[/tex]

obviously an intermediate step is:

[tex]\partial U=-k^{2}\alpha^{2}Udt[/tex]
 
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[tex]\partial U=-k^{2}\alpha^{2}Udt[/tex]

Here, the terms concerning U need to be brought on to the left hand side, and then both sides integrated. You will end up with x as a function of ln(y), then exponentiating both sides will give you the form you have
 
thanks.

and the c(alpha) term multiplying it...that's got nothing to do with the integration itself, right? it's added in there to make the solution more general...?
 
Well alpha is presumably the variable you use for the Fourier transform of your function, so it is to say, since when solving the resulting ODE you integrated the RHS with respect to t, it is entirely possible that the standard integration constant is instead a function of alpha. (Since d/dt (alpha) = 0)
 
and how do you know d/dt(alpha)=0?
 
C(alpha) is a function of alpha only, so it's derivative with respect to t = 0

So instead of adding a constant, you add an arbitrary function of the non integrating variables.
 
thanks. I have not seen that before, does that "function of integration" have a name that I could look up in a calculus book?
 
It should be mentioned when you solved basic PDEs.

For example if U is a function of (t,x)

Ut = f(t,x)

You would integrate wrt t, and add an arbitrary function of x.

When I was taught this, he simply called them arbitrary functions. I'm not sure if they have a special name.
 

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