Homogeneous Equation for Mixed Cauchy Problem

Submitted by Structure on Sun, 11/18/2007 - 19:13.

We try to solve homogeneous equation for mixed Cauchy problem with null boundary condition of a special form for the parabolic heat equation
$P(D)u=\frac{\partial u}{\partial t}(x,t)-\frac{\partial^2 u}{\partial x^2}(x,t)=0$
with initial condition
$u(x,0)=f(x)$
and boundary condition
$u(0,t)=0\:$ and $\frac{\partial u}{\partial x}(1,t)=0$

Look for a nonzero solution of the form u(x,t)=X(x)T(t).
We get T'(t)X(x)-T(t)X"(x)=0 or
$\frac{T'(t)}{T(t)}=\frac{X"(x)}{X(x)}=-\lambda^2$
(*)We get $T'(t)+\lambda^2T(t)=0$
(**) $X"(x)+\lambda^2X(x)=0\: X(0)=X'(1)=0$
Second equation has a solution of the form
$X(x)=a\cos(\lambda x)+b\sin(\lambda x)$
$X(0)=a=0\: X'(1)=b\lambda\cos\lambda =0$
$\lambda_n=\frac{(2n+1)\pi}{2}$
So $X_n(x)=\sin (\frac{(2n+1)\pi}{2}x)$
Equation (*) has solution
$T_n(t)=A_ne^{-\lambda^2_nt$
or $T_n(t)=A_ne^{-\frac{(2n+1)^2\pi^2t}{4}$
Look now for a solution of our equation
$u(x,t)=\sum_{n=1}^{+\infty}T_n(t)X_n(x)=\sum_{n=1}^{+\infty}A_ne^{-\frac{(2n+1)^2\pi^2t}{4}}\sin \frac{(2n+1)\pi}{2}x$
From $u(x,0)=\sum_{n=1}^{+\infty}A_n\sin \frac{(2n+1)\pi}{2}x=f(x)$ we have
$A_n=2\int_{0}^{1}f(x)\sin\frac{(2n+1)\pi x}{2}dx$
In a particular case all you have to do is to evaluate $A_n$ for the given function.

Navigation

User login

Homogeneous Equation for Mixed Cauchy Problem