Ordinary differential equations and BVP

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SUMMARY

The discussion focuses on solving a boundary value problem (BVP) for the partial differential equation (PDE) given by Ut - Uxx = e^(-2t)sin(πx/L) with boundary conditions U(0,t) = 0 and U(L,t) = 0, and initial condition U(x,0) = sin(πx/L). The method of separation of variables is employed, leading to the trial solution U(x,t) = X(x)T(t). The basis functions are calculated as Xn = √(2/L)sin(nπx/L) for n = 1, 2, with eigenvalues λn = -((nπ)/L)². The final solution is expressed as U(x,t) = [c1sin(ax)exp(-a²t) + sin(ax)exp(-2t)/(a²-4)].

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  • Understanding of partial differential equations (PDEs)
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akanksha331
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Solve BVP by separating variables and using eigenfunction expansion method




PDE:Ut-Uxx=e-2tsin(pi x/L) U=U(x,t),x(0,L)
BC1:U(0,t)=0
BC2:U(L,t)=0
IC:U(x,0)=sin(pi x/L)
U(x,t)=X(x)T(t),X''=(lambda) X ,lambda is the separation of parameter.

I have calculated the basis functions as Xn=root(2/L)sin((n pi x) /L) for n=1,2 and labdan=-((n pi)/L)2

Please help to solve the problem
 
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akanksha331 said:
Solve BVP by separating variables and using eigenfunction expansion method




PDE:Ut-Uxx=e-2tsin(pi x/L) U=U(x,t),x(0,L)
BC1:U(0,t)=0
BC2:U(L,t)=0
IC:U(x,0)=sin(pi x/L)
U(x,t)=X(x)T(t),X''=(lambda) X ,lambda is the separation of parameter.

I have calculated the basis functions as Xn=root(2/L)sin((n pi x) /L) for n=1,2 and labdan=-((n pi)/L)2

Please help to solve the problem

Your PDE is not homogeneous. You have:
<br /> u_{t} - u_{xx} = e^{-2t} \sin\frac{\pi x}L<br />

Let's try looking for a separable solution u(x,t) = X(x)T(t). Substituting that into the PDE, we get
<br /> T&#039; X - T X&#039;&#039; = e^{-2t} \sin\frac{\pi x}L<br />
Oh dear. Dividing by XT isn't necessarily going to give us terms which are functions of a single variable and whose sum is a constant, so the standard method doesn't work (or rather, we are forced to make particular choices for X and T in order to do that, and those choices don't lead to a solution of the PDE).

But if we look at the initial and boundary conditions, we see that the initial condition is a constant multiple of \sin \frac{\pi x}L and the boundary conditions require that u vanish at points where \sin \frac{\pi x}L vanishes. This suggests that we should try X(x) = \sin \frac{\pi x}L.
 
Make a trial solution e^(-2t)*F(t)*G(x)

That will remove one part of your problem.
 
I am a little unsure if I have the correct approach but here goes

U(x,0) = X(x)T(0) = sin(pi*x/L) (the initial condition)

Let a=pi/L then X(x) = sin(ax)/T(0), Here, X(0)T(t) = X(L)T(0) = 0 (the boundary conditions)

Substituting this back in the original equation gives:

d/dt[T(t)]*sin(ax) + T(t)*sin(ax)*a^2 = exp(-2t)*sin(ax)*T(0)

Solving this gives:

T(t) = c0*exp(-a^2*t) + T(0)*exp(-2t)/(a^2-4)

U(x,t) = X(x)*T(t) = [ c1*sin(ax)*exp(-a^2*t) + sin(ax)*exp(-2t)/(a^2-4) ]

Is the answer correct? How to use eigen function expansion method ?
 

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