PDE: separation of variables problem

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SUMMARY

The discussion focuses on solving the partial differential equation (PDE) given by u_tt - u_xx - u = 0 with specific boundary and initial conditions. The separation of variables technique is employed, leading to the formulation of two ordinary differential equations (ODEs). The first ODE for X(x) results in the characteristic equation yielding roots that depend on the separation constant K. The correct value of K is determined to be K = n^2*pi^2 - 1, which aligns with the boundary conditions. The solution for T(t) is derived as T'' - (n^2*pi^2 - 1)T = 0, leading to the final solution form involving sine and cosine functions.

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eckiller
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I am to reduce the following PDE to 2 ODEs and find only the particular solutions:

u_tt - u_xx - u = 0; u_t(x,0) = 0; u(0,t) = u(1,t) = 0

I guess u = X(x)T(t), and plug u_tt, u_xx into PDE and divide by u to get:

T''/T = X''/X + 1 = K

I solve X'' + (1-K)X = 0 first.

From characteristic equation, r = +- sqrt(1-K)

Becausse of boundary conditions, we must have 1-K < 0

So r = +- i sqrt(K-1)

(I think I make an error somewhere around here...)

==> u = c1 cos(sqrt(K-1)x) + c2 sin(sqrt(K-1)x)

From boundary conditions, c1 =0, and sin(sqrt(K-1)) = 0 => sqrt(K-1) = n*pi

=> K-1 = n^2*pi^2
=> K = n^2*pi^2 + 1

Correct so far?

Now for T:

T'' - KT = 0

T'' - (n^2*pi^2 + 1)T = 0

r = +- sqrt(n^2*pi^2+1)

I think my K = n^2*pi^2 + 1 is wrong because it is strictly positive and I don't think an e^t solution will satisfy the initial condition.

Please help.

The book's answer is cos( sqrt(n^2*pi^2-1)t) * sin(n*pi*x)
 
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When you separate variables and equate to a separation constant, usually need to check the boundary conditions against a positive, negative, and zero separation constant. For now, these types of equations just have a negative separation constant. That is:

\frac{T^{&#039;&#039;}}{T}=\frac{X^{&#039;&#039;}}{X}+1=K=-\lambda;\quad \lambda&gt;0

So, need to solve:

\frac{X^{&#039;&#039;}}{X}+1=-\lambda

or:

X^{&#039;&#039;}+X(1+\lambda)=0

Solving for the roots:

m=\pm \sqrt{-(1+\lambda)}

Thus have:

X(x)=A_1Cos(\sqrt{1+\lambda}x)+A_2Sin(\sqrt{1+\lambda}x)

Substituting the boundary conditions yield:

\lambda=(n\pi)^2-1;\quad n&gt;0

and:

X(x)=A_2Sin(n\pi x)

Can you do T now?

Edit: Also, I think you need another constraint to obtain a particular solution, you know, wave equations usually specify the initial velocity as well.
 
Last edited:

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