Paper 2, Section II, B

Methods | Part IB, 2013

The steady-state temperature distribution u(x)u(x) in a uniform rod of finite length satisfies the boundary value problem

Dd2dx2u(x)=f(x),0<x<lu(0)=0,u(l)=0\begin{gathered} -D \frac{d^{2}}{d x^{2}} u(x)=f(x), \quad 0<x<l \\ u(0)=0, \quad u(l)=0 \end{gathered}

where D>0D>0 is the (constant) diffusion coefficient. Determine the Green's function G(x,ξ)G(x, \xi) for this problem. Now replace the above homogeneous boundary conditions with the inhomogeneous boundary conditions u(0)=α,u(l)=βu(0)=\alpha, \quad u(l)=\beta and give a solution to the new boundary value problem. Hence, obtain the steady-state solution for the following problem with the specified boundary conditions:

D2x2u(x,t)+tu(x,t)=x,0<x<1u(0,t)=1/D,u(1,t)=2/D,t>0\begin{aligned} &-D \frac{\partial^{2}}{\partial x^{2}} u(x, t)+\frac{\partial}{\partial t} u(x, t)=x, \quad 0<x<1 \\ &u(0, t)=1 / D, \quad u(1, t)=2 / D, \quad t>0 \end{aligned}

[You may assume that a steady-state solution exists.]

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