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ECH5842 CHEMICAL ENGINEERING ANALYSIS R.Chella

HOMEWORK Fall'97



1. Consider the inhomogeneous, two-dimensional diffusion equation

\begin{displaymath}
u_t - u_{xx} - u_{yy} = e^{-\vert x\vert}y\sin \omega t, \qquad \
 -\infty < x < \infty, \qquad 0 \leq y \leq \pi\end{displaymath}

The boundary conditions are:

and the initial condition is:

\begin{displaymath}
u(x,y,0) = \left\{\begin{array}
{ll}
 a = {\rm constant} &\m...
 ... x\vert \leq 1$}\\  
 0 & \mbox{otherwise}
 \end{array} \right.\end{displaymath}

Use Fourier transforms with respect to x and eigenfunction expansions with respect to y to derive an integral representation of the form:

\begin{displaymath}
u(x,y,t) = \frac{1}{\sqrt{2 \pi}}\int_{-\infty}^{\infty}\
\overline{u}(\omega,y,t) e^{-i \omega x}d\omega\end{displaymath}

for the solution. You need not evaluate the inversion integral explicitly. However, give the explicit series form for $\overline{u}(\omega,y,t)$.



2. Solve using Fourier transforms:

\begin{displaymath}
u_t - u_{xx} = 0, \qquad 0 \leq x < \infty, t \gt 0\end{displaymath}

with initial condition:

u(x,0) = 0

and boundary conditions:

Compare with the solution obtained in class using the Laplace Transform technique.



3. Show using Fourier transforms that the solution to:

\begin{displaymath}
u_t - u_{xx} + tu = 0, \qquad 0 \leq x < \infty, t \gt 0\end{displaymath}

with initial condition:

u(x,0) = e-x

and boundary conditions:

is

\begin{displaymath}
u(x,t)= \frac{2}{\pi}e^{-t^2/2} \int_0^\infty \
\frac{e^{-\omega^2 t} \cos \omega x}{1+\omega^2} \ d\omega\end{displaymath}



4.Consider the diffusion equation with variable coefficient:

Solve using integral transforms. (a) What is the most general choice for the constants C1, C2, and C3 for which the solution can be obtained in similarity form? (b) For the choice of constants in part (a), calculate the solution and evaluate all integration constants explicitly.


Ravindran Chella