Solve the following equation: -4u + 3u_{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.

Question image

Understand the Problem

The question asks us to solve the given partial differential equation (PDE) which involves mixed partial derivatives and a sinusoidal term. The PDE is defined on a square region with specified boundary conditions (u=0 on all sides). We need to find the function u(x, y) that satisfies both the equation and the boundary conditions. The equation isn't the standard Laplace Equation, but rather a modified version.

Answer

$u(x,y) = \frac{1 - \cosh(4y - 2\pi)}{8(1 + \cosh(4\pi))}sin(2x)$
Answer for screen readers

$u(x,y) = \frac{1 - \cosh(4y - 2\pi)}{8(1 + \cosh(4\pi))}sin(2x)$

Steps to Solve

  1. Assume a Solution Form

Since the boundary conditions are $u(0, y) = u(\pi, y) = u(x, 0) = u(x, \pi) = 0$ and there is a $sin(2x)$ term, we assume a solution of the form:

$u(x, y) = X(x)Y(y)$.

  1. Consider the form of $X(x)$

Given the $sin(2x)$ term in the equation and the boundary conditions $u(0, y) = u(\pi, y) = 0$, we can deduce that $X(x)$ should be proportional to $sin(2x)$. So, we assume: $u(x, y) = f(y)sin(2x)$

  1. Substitute into the PDE

Substitute $u(x, y) = f(y)sin(2x)$ into the given PDE: $-4u + 3u_{xx} + u_{yy} + sin(2x) = 0$

$-4f(y)sin(2x) + 3f(y)(-4)sin(2x) + f''(y)sin(2x) + sin(2x) = 0$

  1. Simplify the equation

Divide the entire equation by $sin(2x)$ (since $sin(2x)$ is not always zero in the given domain): $-4f(y) - 12f(y) + f''(y) + 1 = 0$ $f''(y) - 16f(y) + 1 = 0$ $f''(y) - 16f(y) = -1$

  1. Solve the homogeneous equation

Solve the homogeneous equation $f''(y) - 16f(y) = 0$. The characteristic equation is $r^2 - 16 = 0$, which gives $r = \pm 4$. The homogeneous solution is $f_h(y) = c_1e^{4y} + c_2e^{-4y}$.

  1. Find a particular solution

For a particular solution, let $f_p(y) = A$. Then $f_p''(y) = 0$. Substituting into $f''(y) - 16f(y) = -1$, we get $0 - 16A = -1$, so $A = \frac{1}{16}$. Thus, $f_p(y) = \frac{1}{16}$.

  1. General solution

The general solution is $f(y) = f_h(y) + f_p(y) = c_1e^{4y} + c_2e^{-4y} + \frac{1}{16}$.

  1. Apply boundary conditions

We know $u(x, 0) = 0$ and $u(x, \pi) = 0$, so $f(0) = 0$ and $f(\pi) = 0$. $f(0) = c_1 + c_2 + \frac{1}{16} = 0$ $f(\pi) = c_1e^{4\pi} + c_2e^{-4\pi} + \frac{1}{16} = 0$

From the first equation, $c_2 = -c_1 - \frac{1}{16}$. Substituting into the second equation: $c_1e^{4\pi} + (-c_1 - \frac{1}{16})e^{-4\pi} + \frac{1}{16} = 0$ $c_1(e^{4\pi} - e^{-4\pi}) = \frac{1}{16}e^{-4\pi} - \frac{1}{16}$ $c_1(e^{4\pi} - e^{-4\pi}) = \frac{1}{16}(e^{-4\pi} - 1)$ $c_1 = \frac{e^{-4\pi} - 1}{16(e^{4\pi} - e^{-4\pi})} = \frac{e^{-4\pi} - 1}{16(e^{4\pi} - e^{-4\pi})} \cdot \frac{e^{4\pi}}{e^{4\pi}} = \frac{1 - e^{4\pi}}{16(e^{8\pi} - 1)}$ $c_1 = \frac{-(e^{4\pi} - 1)}{16(e^{8\pi} - 1)} = \frac{-(e^{4\pi} - 1)}{16(e^{4\pi} - 1)(e^{4\pi} + 1)} = -\frac{1}{16(e^{4\pi} + 1)}$

$c_2 = -c_1 - \frac{1}{16} = \frac{1}{16(e^{4\pi} + 1)} - \frac{1}{16} = \frac{1 - (e^{4\pi} + 1)}{16(e^{4\pi} + 1)} = \frac{-e^{4\pi}}{16(e^{4\pi} + 1)}$

$f(y) = -\frac{e^{4y}}{16(e^{4\pi} + 1)} - \frac{e^{-4\pi}e^{-4y}}{16(e^{4\pi} + 1)} + \frac{1}{16}$ = $\frac{1}{16} - \frac{e^{4y} + e^{4(\pi - y)}}{16(e^{4\pi} + 1)}$

$f(y) = \frac{e^{4\pi} + 1 - e^{4y} - e^{4(\pi - y)}}{16(e^{4\pi} + 1)}$

  1. Final Solution

$u(x, y) = f(y)sin(2x)$ $u(x, y) = \frac{e^{4\pi} + 1 - e^{4y} - e^{4(\pi - y)}}{16(e^{4\pi} + 1)}sin(2x)$ Which can also be written as: $u(x,y) = \frac{1 - \cosh(4y - 2\pi)}{8(1 + \cosh(4\pi))}sin(2x)$

$u(x,y) = \frac{1 - \cosh(4y - 2\pi)}{8(1 + \cosh(4\pi))}sin(2x)$

More Information

The solution involves solving a non-homogeneous PDE with given boundary conditions. We used the method of separation of variables and superposition to arrive at the final answer. The boundary conditions significantly helped in determining the constants of integration. Since all sides are zero, the solution becomes simpler.

Tips

  • Forgetting to include the particular solution when solving non-homogeneous differential equations.
  • Incorrectly applying boundary conditions, which can lead to incorrect constants of integration.
  • Making algebraic errors when simplifying the equation.

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