1. **State the problem:** Solve the partial differential equation (PDE) $$\frac{\partial u}{\partial t} = \frac{1}{4} \frac{\partial^2 u}{\partial x^2}$$ with boundary conditions $$u(0,t) = 0$$ and $$u(2,t) = 0$$ for $$t > 0$$, and initial condition $$u(x,0) = 2 \sin\left(\frac{\pi x}{2}\right) - \sin(\pi x)$$ for $$0 \leq x \leq 2$$.
2. **Use separation of variables:** Assume $$u(x,t) = X(x)T(t)$$.
3. Substitute into the PDE:
$$X(x) T'(t) = \frac{1}{4} X''(x) T(t)$$
Divide both sides by $$X(x) T(t)$$:
$$\frac{T'(t)}{T(t)} = \frac{1}{4} \frac{X''(x)}{X(x)} = k$$
where $$k$$ is a separation constant.
4. Set $$k = -a^2$$ (to satisfy boundary conditions and get nontrivial solutions):
$$\frac{X''(x)}{X(x)} = -a^2 \implies X''(x) + a^2 X(x) = 0$$
5. Solve the spatial ODE:
General solution:
$$X(x) = A \cos(ax) + B \sin(ax)$$
Apply boundary conditions:
- At $$x=0$$: $$u(0,t) = X(0)T(t) = 0 \implies X(0) = 0 \implies A = 0$$
- At $$x=2$$: $$X(2) = B \sin(2a) = 0$$
For nontrivial $$B \neq 0$$, require:
$$\sin(2a) = 0 \implies 2a = n\pi, n=1,2,3,...$$
Thus,
$$a_n = \frac{n\pi}{2}$$
6. So eigenfunctions are:
$$X_n(x) = \sin\left(\frac{n\pi x}{2}\right)$$
7. Solve the temporal ODE:
$$T'(t) = -\frac{1}{4} a_n^2 T(t) = -\frac{1}{4} \left(\frac{n\pi}{2}\right)^2 T(t) = -\frac{n^2 \pi^2}{16} T(t)$$
General solution:
$$T_n(t) = C_n e^{-\frac{n^2 \pi^2}{16} t}$$
8. The general solution is a sum over all $$n$$:
$$u(x,t) = \sum_{n=1}^\infty C_n e^{-\frac{n^2 \pi^2}{16} t} \sin\left(\frac{n\pi x}{2}\right)$$
9. Use initial condition to find coefficients $$C_n$$:
$$u(x,0) = 2 \sin\left(\frac{\pi x}{2}\right) - \sin(\pi x) = \sum_{n=1}^\infty C_n \sin\left(\frac{n\pi x}{2}\right)$$
Comparing terms, only $$n=1$$ and $$n=2$$ appear:
$$C_1 = 2, \quad C_2 = -1$$
10. **Final solution:**
$$\boxed{u(x,t) = 2 e^{-\frac{\pi^2}{16} t} \sin\left(\frac{\pi x}{2}\right) - e^{-\frac{\pi^2}{4} t} \sin(\pi x)}$$
Heat Equation F6247B
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