← 2022 Paper 2

UPSC 2022 Maths Optional Paper 2 Q6a — Step-by-Step Solution

20 marks · Section B

Heat equation · PDEs · asked 3× in 14 yrs · Read the full method →

Question

Solve ut=uxxu_t=u_{xx}, 0<x<l0<x<l, t>0t>0, with u(0,t)=u(l,t)=0u(0,t)=u(l,t)=0 and u(x,0)=x(l−x)u(x,0)=x(l-x).

Technique

Standard heat-equation separation; Fourier sine series of x(l−x)x(l-x) — only odd modes.

Solution

Setup. Standard heat equation with homogeneous Dirichlet BC. Separation of variables.

Step 1 — Separate variables

u(x,t)=X(x)T(t)u(x,t)=X(x)T(t). Substitute: XT′=X′′T⇒T′/T=X′′/X=−λ2XT'=X''T\Rightarrow T'/T=X''/X=-\lambda^2.

Spatial: X′′+λ2X=0X''+\lambda^2 X=0, X(0)=X(l)=0X(0)=X(l)=0. Eigenfunctions Xn=sin⁡(nπx/l)X_n=\sin(n\pi x/l), eigenvalues λn=nπ/l\lambda_n=n\pi/l.

Temporal: T′=−λn2T⇒Tn=e−n2π2t/l2T'=-\lambda_n^2 T\Rightarrow T_n=e^{-n^2\pi^2 t/l^2}.

Step 2 — General solution

u(x,t)=∑n=1∞Bnsin⁡ ⁣(nπxl)e−n2π2t/l2.u(x,t)=\sum_{n=1}^\infty B_n\sin\!\left(\dfrac{n\pi x}{l}\right)e^{-n^2\pi^2 t/l^2}.

Step 3 — Apply IC u(x,0)=x(l−x)u(x,0)=x(l-x)

∑Bnsin⁡(nπx/l)=x(l−x)\sum B_n\sin(n\pi x/l)=x(l-x), the Fourier sine series.

Bn=2l∫0lx(l−x)sin⁡(nπx/l) dx.B_n=\dfrac{2}{l}\int_0^l x(l-x)\sin(n\pi x/l)\,dx.

This is the same integral computed in 2015 P1 Q7(a). The result:

Step 4 — Final solution

Answer

  u(x,t)=∑n=1n odd∞8l2n3π3sin⁡ ⁣(nπxl)e−n2π2t/l2.  \boxed{\;u(x,t)=\sum_{\substack{n=1\\n\text{ odd}}}^\infty\dfrac{8l^2}{n^3\pi^3}\sin\!\left(\dfrac{n\pi x}{l}\right)e^{-n^2\pi^2 t/l^2}.\;}
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