How Do You Solve Differential Equations Using Fourier Transform?

Click For Summary

Homework Help Overview

The discussion revolves around solving differential equations using Fourier transforms, specifically focusing on the inverse Fourier transform and its application in deriving solutions for a given problem involving temperature distribution over time and space.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the steps needed to evaluate the Fourier transform and its inverse, particularly emphasizing the importance of the initial conditions. There is an exploration of the mathematical expressions involved in the transformation process.

Discussion Status

Some participants have provided guidance on evaluating the initial condition and its role in the Fourier transform process. There is acknowledgment of a mistake in the original poster's approach, leading to further clarification on the sequence of transformations required.

Contextual Notes

The original poster expresses uncertainty regarding the correctness of their derived expression and notes discrepancies with expected results. The discussion includes references to specific mathematical forms and conditions that need to be satisfied for the solution.

unscientific
Messages
1,728
Reaction score
13

Homework Statement



2me31hl.png


Part (a): State inverse Fourier transform. Show Fourier transform is:
Part (b): Show Fourier transform is:
Part (c): By transforming LHS and RHS, show the solution is:
Part(d): Using inverse Fourier transform, find an expression for T(x,t)

Homework Equations


The Attempt at a Solution



Part(d)
T_{(x,t)} = \int_{-\infty}^{\infty} T e^{-Dk^2t}e^{ikx} dk
= \int_{-\infty}^{\infty} (T_0 + \sum_{m=1}^{\infty} Tm cos(\frac {m\pi x}{L}) e^{-Dk^2t + ikx} dk
= \int_{-\infty}^{\infty} T_0 e^{-Dk^2t + ikx} dk + \sum_{m=1}^{\infty} T_m cos(\frac {m \pi x}{L}) \int_{-\infty}^{\infty} e^{-Dk^2t + ikx} dk

Attempt at evaluating the integral, letting a^2 = \frac {1}{Dt}

\int_{-\infty}^{\infty} e^{-(\frac{k^2}{a^2} - ikx)} dx
= \int_{-\infty}^{\infty} e^{-\frac{({k - \frac{ixa^2}{2}})^2}{a^2}} e^{-\frac {x^2a^2}{4}} dk
= e^-{\frac{x^2a^2}{4}} \int_{-\infty - i\frac{x^2a^2}{4}}^{\infty - i\frac {x^2a^2}{4}} e^{- \frac{k^2}{a^2}} dk
= e^{\frac {-x^2a^2}{4}} \sqrt{\pi a^2} = \sqrt {\frac{\pi}{Dt}} e^{\frac {-x^2a^2}{4}}

But this appears to be wrong as their final expression do not have the factor of √(1/t) in their coefficients..
 
Last edited:
Physics news on Phys.org
First you have to evaluate \tilde{T}(k,0) from the initial condition which is given in the position domain as T(x,0)! Then you can plug it into the general solution and Fourier transform back!
 
vanhees71 said:
First you have to evaluate \tilde{T}(k,0) from the initial condition which is given in the position domain as T(x,0)! Then you can plug it into the general solution and Fourier transform back!

Ha ha, that's a silly mistake I made!

So I must Fourier transform the initial condition, then plug it back in, then inverse Fourier transform everything?
 

Similar threads

Replies
1
Views
2K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 6 ·
Replies
6
Views
2K
  • · Replies 11 ·
Replies
11
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
Replies
1
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
Replies
2
Views
2K