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Solve the following differential equation using Galerkin Method

Solve the following differential equation using Galerkin Method

$\frac{d^2 \phi}{dx^2}+cos \pi x = 0 \hspace{2cm}0 \leq x \leq 1$

Boundary conditions are $\phi(0)=0 \hspace{0.5cm} \phi(1) = 0$

Find $\phi(0.25), \phi(0.5) \hspace{0.2cm} \& \hspace{0.2cm} \phi(0.75)$.

Compare your answers with exact solution.


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Given differential equation $ \frac{d^2 \phi}{dx^2} + cos\pi x = 0 $ where $ 0 \leq x \leq 1 $ with boundary conditions $ \phi (0) = 0; \phi (1) = 0 $

Approximate solution is given by,

$ \phi = C_0 + \sum [C_i sin (\frac{\pi}{2}(2i-1)x)] $ ......(0)

At x = 0, $\phi = 0, \,\,\, \therefore C_0 = 0 \\ \therefore \phi = \sum [C_i sin (\frac{\pi}{2}(2i-1)x)] $

Since the order of D.E is 2, so i will be of order 3

$ \therefore \phi = C_1 sin (\frac{\pi x}{2}) + C_2 sin (\frac{3\pi x}{2}) + C_3 sin (\frac{5\pi x}{2}) $

At x = 1, $\phi = 0 $

$ \therefore 0 = C_1 - C_2 + C_3 \\ \therefore C_2 = C_1 + C_3 $

Equation (1) becomes,

$ \phi = C_1 sin (\frac{\pi x}{2}) + (C_1 + C_3) sin (\frac{3\pi x}{2}) + C_3 sin (\frac{5\pi x}{2}) \\ \phi = C_1[ sin (\frac{\pi x}{2}) + sin (\frac{3\pi x}{2})] + C_3 [sin (\frac{3\pi x}{2}) + sin (\frac{5\pi x}{2})] $

Differentiating the above equation, we get,

$ \frac{d\phi}{dx} = C_1\frac{\pi}{2}[cos(\frac{\pi x}{2}) + 3 cos(\frac{3\pi x}{2}) + C_3\frac{\pi}{2}[3cos(\frac{3\pi x}{2}) + 5cos(\frac{5\pi x}{2}) $

Again differentiating above equation, we get,

$ \frac{d^2\phi}{dx^2} = -C_1 \frac{\pi^4}{4}(sin\frac{\pi x}{2} + 9sin\frac{3 \pi x}{2}) - C_3 \frac{\pi^2}{4}(9sin\frac{3 \pi x}{2} + 25sin\frac{5 \pi x}{2}) $

Residual function is given by,

$ - \frac{d^2\phi}{dx^2} - cos\pi x = R $

Substituting the value of $ (- \frac{d^2\phi}{dx^2}) $ in above equation, we get,

$ \frac{\pi^4}{4} [C_1 (sin\frac{\pi x}{2} + 9sin\frac{3 \pi x}{2}) + C_3 (9sin\frac{3 \pi x}{2} + 25sin\frac{5 \pi x}{2})] - cos \pi x = R $

Weighted Integral form,

$ \int_0^1 w_i R \,\, dx = 0 $

w$_i$ = coefficient of constant from $\phi$

For i = 1, $ w_1 = sin \frac{\pi x}{2} + sin \frac{3 \pi x}{2} \\ \therefore \frac{\pi^2}{4} \int_0^1 (sin \frac{\pi x}{2} + sin \frac{3 \pi x}{2}) [C_1 (sin\frac{\pi x}{2} + 9sin\frac{3 \pi x}{2}) + C_3 (9sin\frac{3 \pi x}{2} + 25sin\frac{5 \pi x}{2}) - cos \pi x] \,\, dx = 0 \\ 5C_1 + 2.84C_3 - 0.069 = 0 \\ 5C_1 + 2.84C_3 = 0.069 \,\,\,\,\, .....(A)$

For i = 2, $ w_2 = sin \frac{3 \pi x}{2} + sin \frac{5 \pi x}{2} \\ C_1 \int_0^1 (sin\frac{3 \pi x}{2} + sin\frac{5 \pi x}{2}) (sin \frac{\pi x}{2} + sin \frac{3 \pi x}{2}) \,\, dx + C_3 \int_0^1 (sin\frac{3 \pi x}{2} + sin\frac{5 \pi x}{2}) (9 sin\frac{3 \pi x}{2} + 25 sin\frac{5 \pi x}{2}) \,\, dx - \int_0^1 (sin\frac{3 \pi x}{2} + sin\frac{5 \pi x}{2}) cos \pi x \,\, dx = 0 \\ 3.9C_1 +14.75C_3 - 0.207 = 0 \\ \therefore 3.9C_1 +14.75C_3 = 0.207 \,\,\,\,\,\, .....(B) $

Solving (A) and (B), we get,

C$_1$ = 0.0069 and C$_3$ = 0.0122

Approximate solution is given by,

$ \phi = 0.0069 (sin \frac{\pi x}{2} + sin \frac{3 \pi x}{2}) + 0.0122(sin \frac{3 \pi x}{2} + sin \frac{5 \pi x}{2}) $

i) At x = 0.25; $\phi$ = 0.02210

ii) At x = 0.5; $\phi$ = 0.03155

iii) At x = 0.75; $\phi$ = 0.0249

Exact solution:

$ - \frac{d^2 \phi}{dx^2} - cos \pi x = 0 \\ i.e. - \frac{d^2 \phi}{dx^2} = cos \pi x $

Integrating above equation, we get,

$ - \frac{d \phi}{dx} = - sin \frac{\pi x}{\pi} + C_1 $

Again integrating, we get,

$ - \phi = - cos \frac{\pi x}{\pi^2} + C_1x + C_2 \\ C_2 = \frac{1}{\pi^2} $

Imposing boundary condition

At x = 0; $\phi$ = 0

$ 0 = - \frac{1}{\pi^2} + C_2 \\ \frac{1}{\pi^2} = C_2 $

$ \therefore - \phi = - cos \frac{\pi x}{\pi^2} + C_1x + \frac{1}{\pi^2} $

At x = 1; $\phi_1$ = 0

$ \therefore 0 = \frac{1}{\pi^2} + C_1 + \frac{1}{\pi^2} \\ C_1 = - \frac{2}{\pi^2} \\ \therefore - \phi = - cos \frac{\pi x}{\pi^2} - \frac{2x}{\pi^2} + \frac{1}{\pi^2} \\ \therefore \phi = cos \frac{\pi x}{\pi^2} + \frac{2x}{\pi^2} - \frac{1}{\pi^2} $

At x = 0.25; $\phi$ = 0.0207

At x = 0.5; $\phi$ = 0

At x = 0.75; $\phi$ = - 0.02098

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