Problem with partial differential equation. Solution included:
boundary conditions of u(x, t): u(0, t) = 0 u(pi, t) = 0 u(x, 0) = 0 \[\frac{ \delta u }{ \delta t } |_{t = 0} = sinx\] delta is partial derivative (because o.s. doesn't have the symbol yet) this is a wave equation problem: \[a^2\frac{ \delta^2 u }{ \delta x^2 } = \frac{ \delta^2 u }{ \delta t^2 }\] solution is here: http://img23.imageshack.us/img23/6848/l3tj.jpg i understand everything, and I have solved others. my only problem is the B1 term they introduced when solving for Bn (which turned out to = 0) using the fourier series method. I don't understand how it was obtained. Please explain or point me to the right resource :)
@Euler271 "openstudy" just uses MathJax which most definitely supports \(\partial\)
thanks for letting me know ^_^
@Euler271 \(\partial=\text{\partial}\)
Oh that's what it is o_o
If you see something on OpenStudy and don't know how to produce it in LaTex, just select the offending math, right click and do Show Math As>TeX Commands
This solution manual text really sucks... :-p
forget the solution manual ... do it on your own. there are couple of inconsistencies with what you mention. for eg; you have u(x,0) = 0, solution assumes u_t(x,0) = 0
i don't understand what you see wrong with it. solution in textbook respects u_t(x, 0) = sinx I just don't understand what B1 is. Bn is solved using fourier sine series. How do you find B1?
You find it via comparison ... there is \(T'(0) = 0 \) . it's supposed to be \(T(0) = 0 \)
the solution is of the form X*T ... all those values of n consist of your solution. so you using superposition principle. Use boundary condition on X and T to simplify. |dw:1371323294729:dw||dw:1371323386702:dw|
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