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PHYSICS 312
Problem set 3:
A rod of length a is initially (t=0) at temperature T=0. It is put into convective contact with a fluid with temperature T0. The temperatures at the ends (x=0) and (x=a) are kept at T=0, but towards the middle the temperature rises towards T0. Assume that the temperature distribution satisfies the differential equation

\begin{displaymath}\frac{\partial^2T}{\partial x^2}-\gamma^2(T-T_0)=\frac{1}{k}\frac{\partial T}{\partial t}\end{displaymath}

for t>0, with k and $\gamma$ constants.

a:
Find the steady state temperature distribution TS(x).
b:
Find the differential equation satisfied by the transient.

u(x,t)=T(x,t)-TS(x)

c:
What is the initial temperature distribution for the transient?
d:
Solve the transient problem formally, by assuming that the initial temperature u(x,0) has a Fourier sine series:

\begin{displaymath}u(x,0)=\sum_{n=0}^\infty c_n\sin(\frac{n\pi x}{a})\end{displaymath}

(for this part of the problem you don't need to calculate the Fourier coefficients).
e:
Could you find the time dependent temperature distribution directly without subtracting the steady state?
f:
Plot the temperature distribution at time t=1 for $a=k=\gamma=T_0=1$. (For this part of the problem you need to compute the first few Fourier coefficients either with or without the steady state subtracted.) Return to title page.

 

Birger Bergersen
2000-01-23