Problem #5

UCI. MAE200B, winter 2006. by nasser Abbasi.

Problem: Solve the following problems by transform methods

(a) MATH

Consider the special case when MATH. Sketch the corresponding MATH for various values of $t>0$.

Solution for part (a)

Some definitions first. The Fourier transform is defined as (using textbook definition)

MATH

and the inverse Fourier transform is

MATH

And the convolution is defined as

MATH

The shift property:

If $f\left( x\right) $ has Fourier transform MATH then MATH has the Fourier transform MATH

The delay property:

If $f\left( x\right) $ has fourier transform MATH then MATH has fourier transform MATH

If $f\left( x\right) $ has fourier transform MATH then MATH has fourier transform MATH

and

MATH

And the property of differentiation MATH

Now start the solution by assuming that MATH

Start by taking the fourier transform of each term in the PDE w.r.t $x$, and assume that MATH

and assume that the fourier transform of $f\left( x\right) $ is MATH

Hence

MATH

and

MATH

and

MATH

Now take the fourier transform of the PDE and using the above relations

MATH

Hence this is now a first order ODE, the solution is

MATH

To find the solution MATH then take the inverse fourier transform of the above

MATH

Using the delay property we get

MATH

Hence the solution is

MATH

When MATH, MATH hence

MATH

Hence the solution is MATH

The effect of the term MATHis to introduce the term $+ct$ in the exponential as shown above. $ct$ has units of distance, so the term $x+ct$ acts as a shift in distance. So it is a transport phenomena. I.e. diffusion with mass transport.

This is a plot of the solution, I picked $x=0$ where the dirac delta function is to show how $u$ changes with time at that location.


Figure


Problem: Solve the following problems by transform methods

(b) MATH

Solution for part (b)

Start by taking the fourier transform of each term in the PDE w.r.t $x$, and assume that MATH

and assume that the fourier transform of $f\left( x\right) $ is MATH

Hence

MATH

and

MATH

Now take the fourier transform of the PDE w.r.t $x$ and using the above relations

MATH

Hence this is now a first order ODE, nonhomogeneous. Star by solving the homogeneous ODE. The solution is

MATH

To find the solution MATH then take the inverse fourier transform of the above

MATH

I am not sure if we should assume that MATH as well as part(a) as the problem was not clear. To precessed, I assume so, else not knowing what $f\left( x\right) $ is one can not do anything more here.

When MATH, MATH hence

MATH

Hence the homogeneous solution is MATH

Not knowing what MATH is, assume that the particular solution is MATH which can be found by using method of finding integrating factors, hence the solution is MATH


Problem: Solve the following problems by transform methods

(c) MATH

Solution for part (c)

MATH

Take fourier transform w.r.t $x$, assume that MATH

Take fourier transform of the PDE we obtain

MATH

This is a second order ODE, the characteristic equation is

MATH

solution is

MATH

Using the second B.C. that MATH, this implies that $A$ must be zero, else $u$ will not vanish as $y$ goes to $\infty$. Hence we obtain

MATH

Hence MATH

But MATH

Hence (1) becomes

MATH

at $y=0$, MATH hence

MATH

Hence MATH

So the solution is

MATH


Problem: Solve the following problems by transform methods

(d) MATH

Solution for part (d)

Taking Fourier transform w.r.t $x$

assume that MATH

MATH

MATH

Hence the PDE becomes

MATH

This is a second order ODE. The characteristic equation is

MATH

Hence MATH

Hence the solution is MATH

Apply BC, at $t=0\ $

MATH

Apply second BC

MATH

at $t=0$ ,MATH hence

MATH

Hence we have 2 equations

MATH

Solve for A,B

MATH

Hence MATH

and MATH

Hence solution is

MATH

Hence MATH

But MATH

and

MATH

Where MATH is the sign function which gives -1, 0 or 1 depending on whether $a$ is negative, zero, or positive

and

MATH

and

MATH

HenceMATH