This is a heat conducting problem: u_(t) = u_(xx) u(x,t)=w(x,t)+ψ(x) u(x,0)=cos(∏x) u_(x)(0,t)=0 u_(x)(1,t)=0
Here is what I have been trying: The homogenous solution (ψ(x) = 0) is of the form \[u(x,t) = G(0)e^{-λ^{2}t}(A*\sinλx + B*\cosλx)\] -> (i) \[u(x,0) = \cos\pi x = G(0)(A*\sinλx + B*\cosλx)\] (ii), \[u_{x}(0,t) = 0 = G(0)e^{-λ^{2}t}(Aλ*\cos0 - Bλ*\sin0) = AλG(0)e^{-λ^{2}t}\] (iii), \[u_{x}(1,t) = 1 = G(0)e^{-λ^{2}t}(Aλ*\cosλ - Bλ*\sinλ)\] -> \[\cos\pi x = G(0)B*\cosλx, 1 = -BλG(0)e^{-λ^{2}t}\sinλ\] Since (ii) -> A = 0
Since (ii) -> A = 0 thats right
and u can drop G(0)
you need to apply the other boundary condition(u_x(12,t)=0) in order to determine the possible values for lambda., after which the general solution will be a sum over lamda values.
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