Piecewise initial condition heat equation

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SUMMARY

The discussion focuses on solving the heat equation with specific initial conditions using Fourier series. The initial condition is defined piecewise as \( f(x) \), with values of 0 and 100 across specified intervals. The coefficients \( A_m \) are calculated using the formula \( A_m = \frac{200}{m\pi}\left[\cos\left(\frac{\pi}{3}m\right) - \cos\left(\frac{2\pi}{3}m\right)\right] \). It is concluded that a sufficient number of terms must be used in the Fourier series to accurately represent the piecewise function, particularly for abrupt changes in the initial condition.

PREREQUISITES
  • Understanding of Fourier series and their application in solving partial differential equations.
  • Familiarity with the heat equation and boundary conditions.
  • Knowledge of piecewise functions and their graphical representation.
  • Proficiency in calculus, particularly integration techniques.
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  • Explore the derivation and application of Fourier series in solving the heat equation.
  • Investigate the impact of increasing the number of terms in Fourier series on the approximation of piecewise functions.
  • Learn about convergence criteria for Fourier series, especially for functions with discontinuities.
  • Study the behavior of the heat equation under various initial and boundary conditions.
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Mathematicians, physicists, and engineering students focusing on heat transfer, as well as educators and researchers interested in the application of Fourier analysis to solve differential equations.

raditzan
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Homework Statement


I have the solution to the heat equation, with the BC's and everything but the IC applied. So I am just trying to solve for the coefficients, the solution without the coefficients is
$$u(x,t) = \sum_{n=1}^{\infty} A_n\sin(nx)e^{-n^2t}$$
If the initial condition is ##u(x,0) = f(x)## such that $$f(x) = \begin{cases}
0 & 0 < x < \frac{\pi}{3} \\
100 & \frac{\pi}{3} < x < \frac{2\pi}{3} \\
0 & \frac{2\pi}{3} < x < \pi
\end{cases}
$$
I used the formula $$A_m = \frac{2}{\pi}\int_0^\pi f(x)\sin(mx)dx=\frac{200}{m\pi}\bigg[\cos(\frac{\pi}{3}m) - cos(\frac{2\pi}{3}m)\bigg]$$

I couldn't find a pattern in the coefficients other than all the even indices go to ##0##. Also is this even correct? When I try to graph this at ##t=0## it isn't giving me the piecewise function ##f(x)##. Is it just that I didn't use enough terms to make it noticeable? Also how would I show that at any time ##t>0## the temperature distribution in the rod achieves a local maximum at ##x=\pi/2##?
 
Last edited:
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That's right. Use more terms. I used 100, and it was still pretty rough. Fourier sums like your solution work well for smooth functions, abrupt changes like that require a lot of terms to reproduce.
 
raditzan said:
I used the formula $$A_m = \frac{2}{\pi}\int_0^\pi f(x)\sin(mx)dx=\frac{200}{m\pi}\bigg[\cos(\frac{\pi}{3}m) - cos(\frac{2\pi}{3}m)\bigg]$$

I couldn't find a pattern in the coefficients other than all the even indices go to ##0##. Also is this even correct? When I try to graph this at ##t=0## it isn't giving me the piecewise function ##f(x)##. Is it just that I didn't use enough terms to make it noticeable? Also how would I show that at any time ##t>0## the temperature distribution in the rod achieves a local maximum at ##x=\pi/2##?

$$\cos(\frac{\pi}{3}m) - cos(\frac{2\pi}{3}m)=\cos\left(\frac{\pi}{3}m\right)-2\cos^2\left(\frac{\pi}{3}m\right)+1$$
m=1: ##\frac{1}{2}-\frac{1}{2}+1=1##
m = 2: ##-\frac{1}{2}-\frac{1}{2}+1=0##
m=3: ##-1-2+1=-2##
m=4: ##-\frac{1}{2}-\frac{1}{2}+1=0##
m=5: ##1##
m=6: ##0##
m=7: ##1##
m=8: ##0##
m=9: ##-2##

There are 3 separate summations.

For m=6k+1 (k=0,1,2,...), the coeff is 1
For m = 6k+3 (k=0,1,2,..), the coeff is -2
For m = 6k+5 (k=0,1,2,...), the coeff is 1
 

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