Question #91730
Solve the heat conduction equation:
for the following boundary and initial conditions:

u(0,t) = u(5,t) = 0,
u(x,0) =2sin(πx)− 4sin(2πx)
1
Expert's answer
2019-07-17T09:51:13-0400
ut=κΔu\frac{\partial u}{\partial t} = -\kappa \Delta uu(0,t)=u(5,t)=0u(0, t) = u(5, t) = 0u(x,0)=2sin(πx)4sin(2πx)u(x, 0) = 2\sin(\pi x) -4\sin(2\pi x)

Let's find the solution in such a way:

u=T(t)X(x)u = T(t) X(x)TT(t)=κXX(x)=κλ\frac{T'}{T}(t) = -\kappa \frac{X''}{X}(x) = -\kappa\lambda

where lambda is a constant.

X+λX=0X'' + \lambda X = 0X(0)=X(5)=0X(0) = X(5) = 0

hence

X=sinnπ5xX = \sin \frac{n\pi}{5}x

while n is integer and

λ=(nπ5)2\lambda = \bigg(\frac{n\pi}{5}\bigg)^2

Thus

T=κλTT' = - \kappa\lambda TT=CeκλtT = C e^{-\kappa\lambda t}

The heat conduction equation is linear, therefore a sum of solutions is also a solution.

u(x,0)=2sin(πx)4sin(2πx)u(x, 0) = 2\sin(\pi x) -4\sin(2\pi x)λ1=(5π5)2,λ2=(52π5)2\lambda_1 = \bigg(\frac{5\pi}{5}\bigg)^2, \qquad \lambda_2 = \bigg( \frac{5\cdot 2\pi}{5}\bigg)^2u(x,t)=2eκπ2tsin(πx)4e4κπ2tsin(2πx)u(x, t) = 2e^{-\kappa \pi^2 t} \sin(\pi x) -4e^{-4\kappa\pi^2 t}\sin(2\pi x)


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