- 2070 Bhadra · 10 marks
Heat equation, insulated ends, u(x,0)=x
Short answer
Separate variables and use insulated boundary conditions to get a cosine series. The solution is u(x,t) = L/2 − (4L/π²) Σ_{n odd} (1/n²) cos(nπx/L) e^{−c²n²π²t/L²}. As t→∞, u→L/2.
Solve one dimensional heat equation ∂u/∂t = c² ∂²u/∂x² under the boundary condition ∂u/∂x = 0 when x = 0 and x = L and initial condition u(x, 0) = x for 0 < x < L.
Problem. u_t = c² u_xx on 0 < x < L, with u_x(0, t) = u_x(L, t) = 0 and u(x, 0) = x.
Step 1: separate variables. u = X(x)T(t): X″/X = T′/(c²T) = k. For u to stay bounded as t → ∞, k ≤ 0.
- k = 0: X = A + Bx, T = constant
- k = −p²: X = A cos px + B sin px, T = e^{−c²p²t}
Step 2: insulated ends.
- k = 0: X′ = B = 0, so X = constant (accepted).
- k = −p²: X′(0) = 0 gives B = 0; X′(L) = 0 gives sin pL = 0, so p = nπ/L.
Step 3: general solution.
u(x, t) = a₀ + Σ_{n=1}^{∞} aₙ cos(nπx/L) e^{−c²n²π²t/L²}
Step 4: initial condition u(x, 0) = x (cosine series on (0, L)):
a₀ = (1/L) ∫₀^L x dx = L/2
aₙ = (2/L) ∫₀^L x cos(nπx/L) dx
= (2/L) [ x (L/nπ) sin(nπx/L) + (L/nπ)² cos(nπx/L) ]₀^L
= (2/L) (L²/n²π²) [ (−1)ⁿ − 1 ]
= 2L [ (−1)ⁿ − 1 ] / (n²π²)
So aₙ = −4L/(n²π²) for odd n, and aₙ = 0 for even n.
Answer:
u(x, t) = L/2 − (4L/π²) Σ_{n = 1,3,5,…} (1/n²) cos(nπx/L) e^{−c²n²π²t/L²}
As t → ∞, u → L/2, the average of the initial temperature.
(Numerical check: L = 2, x = 0.7: the series at t = 0 gives 0.70000 ✓.)
✓ Answer checked by Claude Opus 5.5 (high effort)
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