Solve the following Laplace equation: -8u + 2u_{xx} + u_{yy} + sin(2x) = 0 on a square 0 < x, y < π subject to zero boundary conditions: u = 0 on top, bottom, left and right sides.... Solve the following Laplace equation: -8u + 2u_{xx} + u_{yy} + sin(2x) = 0 on a square 0 < x, y < π subject to zero boundary conditions: u = 0 on top, bottom, left and right sides. Find u(x, y).
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Understand the Problem
The question asks to solve a partial differential equation with given boundary conditions on a square. Specifically, it asks to find the solution u(x, y) to the equation -8u + 2u_{xx} + u_{yy} + sin(2x) = 0 on the square 0 < x, y < π with the boundary condition u = 0 on all sides of the square. This means that u(0, y) = u(π, y) = u(x, 0) = u(x, π) = 0.
Answer
$u(x, y) = \frac{1}{16} \left(1 - \frac{e^{4y} + e^{4(\pi-y)}}{e^{4\pi} + 1}\right) \sin(2x)$
Answer for screen readers
$u(x, y) = \frac{1}{16} \left(1 - \frac{e^{4y} + e^{4(\pi-y)}}{e^{4\pi} + 1}\right) \sin(2x)$
Steps to Solve
- Assume a solution form
Since the boundary conditions are $u=0$ on $x=0, x=\pi, y=0,$ and $y=\pi$, we can assume a solution of the form $u(x, y) = \sum_{n=1}^{\infty} \sum_{m=1}^{\infty} A_{nm} \sin(nx) \sin(my)$. However, due to the form of the forcing function $\sin(2x)$, we can try a simpler solution of the form $u(x, y) = X(x)Y(y)$. Furthermore, let's assume that the solution can be written as $u(x, y) = f(y) \sin(2x)$, as dictated by the forcing function.
- Substitute the assumed solution into the PDE
Substituting $u(x, y) = f(y) \sin(2x)$ into the given PDE $-8u + 2u_{xx} + u_{yy} + \sin(2x) = 0$, we have: $$ -8f(y)\sin(2x) + 2f(y) \frac{\partial^2}{\partial x^2}\sin(2x) + \frac{\partial^2}{\partial y^2}f(y) \sin(2x) + \sin(2x) = 0 $$
- Calculate the derivatives
Calculate the required derivatives: $\frac{\partial^2}{\partial x^2} \sin(2x) = -4\sin(2x)$, $\frac{\partial^2}{\partial y^2}f(y) = f''(y)$.
- Substitute derivatives back into equation
Substituting these derivatives into the equation, we get: $$ -8f(y)\sin(2x) + 2f(y)(-4\sin(2x)) + f''(y)\sin(2x) + \sin(2x) = 0 $$ $$ -8f(y)\sin(2x) - 8f(y)\sin(2x) + f''(y)\sin(2x) + \sin(2x) = 0 $$ $$ f''(y)\sin(2x) - 16f(y)\sin(2x) + \sin(2x) = 0 $$
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Simplify the equation Dividing by $\sin(2x)$ (since $\sin(2x) \neq 0$ for $0 < x < \pi$), we have: $$ f''(y) - 16f(y) + 1 = 0 $$ $$ f''(y) - 16f(y) = -1 $$
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Solve the homogeneous equation The homogeneous equation is $f''(y) - 16f(y) = 0$. The characteristic equation is $r^2 - 16 = 0$, which gives $r = \pm 4$. So the homogeneous solution is $f_h(y) = c_1e^{4y} + c_2e^{-4y}$.
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Find particular solution For a particular solution, we assume a constant solution $f_p(y) = A$. Then $f_p''(y) = 0$. Substituting into the non-homogeneous equation gives $0 - 16A = -1$, so $A = \frac{1}{16}$. Thus, $f_p(y) = \frac{1}{16}$.
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General Solution The general solution is $f(y) = f_h(y) + f_p(y) = c_1e^{4y} + c_2e^{-4y} + \frac{1}{16}$.
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Apply Boundary Conditions
Now, we apply the boundary conditions $u(x, 0) = 0$ and $u(x, \pi) = 0$, which implies $f(0) = 0$ and $f(\pi) = 0$. $f(0) = c_1e^{0} + c_2e^{0} + \frac{1}{16} = c_1 + c_2 + \frac{1}{16} = 0$. Thus, $c_1 + c_2 = -\frac{1}{16}$.
$f(\pi) = c_1e^{4\pi} + c_2e^{-4\pi} + \frac{1}{16} = 0$. Thus, $c_1e^{4\pi} + c_2e^{-4\pi} = -\frac{1}{16}$.
- Solve for coefficients We have the system of equations: $c_1 + c_2 = -\frac{1}{16}$ $c_1e^{4\pi} + c_2e^{-4\pi} = -\frac{1}{16}$ From the first equation, $c_2 = -\frac{1}{16} - c_1$. Substituting into the second equation: $c_1e^{4\pi} + (-\frac{1}{16} - c_1)e^{-4\pi} = -\frac{1}{16}$ $c_1e^{4\pi} - \frac{1}{16}e^{-4\pi} - c_1e^{-4\pi} = -\frac{1}{16}$ $c_1(e^{4\pi} - e^{-4\pi}) = \frac{1}{16}e^{-4\pi} - \frac{1}{16}$ $c_1 = \frac{\frac{1}{16}(e^{-4\pi} - 1)}{e^{4\pi} - e^{-4\pi}} = \frac{e^{-4\pi} - 1}{16(e^{4\pi} - e^{-4\pi})} = \frac{e^{-4\pi} - 1}{16(e^{4\pi} - e^{-4\pi})} = \frac{e^{-4\pi} - 1}{16(e^{4\pi} - e^{-4\pi})} \cdot \frac{e^{4\pi}}{e^{4\pi}} = \frac{1 - e^{4\pi}}{16(e^{8\pi} - 1)}$ $c_1 = \frac{-(e^{4\pi} - 1)}{16(e^{8\pi} - 1)} = -\frac{e^{4\pi} - 1}{16(e^{4\pi} - 1)(e^{4\pi} + 1)} = -\frac{1}{16(e^{4\pi} + 1)}$.
Now find $c_2$: $c_2 = -\frac{1}{16} - c_1 = -\frac{1}{16} + \frac{1}{16(e^{4\pi} + 1)} = \frac{-e^{4\pi} - 1 + 1}{16(e^{4\pi} + 1)} = \frac{-e^{4\pi}}{16(e^{4\pi} + 1)}$.
- Final Solution Therefore, $$ f(y) = -\frac{e^{4y}}{16(e^{4\pi} + 1)} - \frac{e^{-4y}e^{4\pi}}{16(e^{4\pi} + 1)} + \frac{1}{16} = \frac{1}{16} - \frac{e^{4y} + e^{4\pi-4y}}{16(e^{4\pi} + 1)} $$ $$ u(x, y) = f(y) \sin(2x) = \left( \frac{1}{16} - \frac{e^{4y} + e^{4\pi-4y}}{16(e^{4\pi} + 1)} \right) \sin(2x) $$ $$ u(x, y) = \frac{1}{16} \left(1 - \frac{e^{4y} + e^{4(\pi-y)}}{e^{4\pi} + 1}\right) \sin(2x) $$
$u(x, y) = \frac{1}{16} \left(1 - \frac{e^{4y} + e^{4(\pi-y)}}{e^{4\pi} + 1}\right) \sin(2x)$
More Information
The particular solution satisfies the given partial differential equation and the specified boundary conditions.
Tips
A common mistake when solving this type of problem is to incorrectly compute the derivatives or to incorrectly apply the boundary conditions. Another common mistake is to struggle with the algebra when solving for the coefficients $c_1$ and $c_2$. Additionally, mistakes often arise in solving the homogeneous and non-homogeneous equations due to algebraic errors in the process.
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