Solving Laplace's Eq with Mixed BCs

In summary, the problem of solving Laplace's equation on a rectangle with mixed boundary conditions can be solved using the boundary conditions $u_y(x,0) = 0$ and $u_x(L,y) + u(L,y) = 0$. The solution can be expressed as a sum of cosine functions with coefficients determined by the eigenvalues, which can be found by setting the tangent of the eigenvalues equal to their reciprocal. The solution is then simplified further by setting the coefficient of the $B_n$ term to 0, resulting in a solution of the form $u(x,y) = \sum_{n = 1}^{\infty}A_n\cos\lambda_nx\cosh\lambda
  • #1
Dustinsfl
2,281
5
Solve Laplace’s equation $\nabla^2u = 0$ on the rectangle with the following boundary conditions:
$$
u_y(x,0) = 0\quad u_x(0,y) = 0\quad u(x,H) = f(x)\quad u_x(L,y) + u(L,y) = 0.
$$

How are mixed BC handled?
 
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  • #2
Consider the boundary conditions $u_x(0,y) = 0$ and $u_x(L,y) + u(L,y) = 0$.
Therefore, if $u(x,y)$ is of the form $u(x,y) = \varphi(x)\psi(y)$, $\varphi_n(x) = A\cos\lambda_nx$ and the eigenvalues are determined by
$$
\tan\lambda_n = \frac{1}{\lambda_n}.
$$
So we have that
$$
\begin{alignat*}{3}
u(x,y) & = & \sum_{n = 1}^{\infty}A\cos\lambda_nx(B\cosh\lambda_ny + C\sinh\lambda_ny)\\
& = & \sum_{n = 1}^{\infty}\cos\lambda_nx(A_n\cosh\lambda_ny + B_n\sinh\lambda_ny)
\end{alignat*}
$$
Now because of the first boundary condition, $u_y(x,0)$, we have that $B_n = 0$.
Therefore, the solution is of the form
$$
u(x,y) = \sum_{n = 1}^{\infty}A_n\cos\lambda_nx\cosh\lambda_ny.
$$
 
Last edited:

Related to Solving Laplace's Eq with Mixed BCs

1. How do you solve Laplace's equation with mixed boundary conditions?

To solve Laplace's equation with mixed boundary conditions, you can use the method of separation of variables. This involves separating the variables and solving the resulting ordinary differential equations. You can also use numerical methods such as finite difference or finite element methods.

2. What are mixed boundary conditions in Laplace's equation?

Mixed boundary conditions in Laplace's equation refer to a combination of Dirichlet and Neumann boundary conditions. This means that the boundary conditions specify both the value of the unknown function and its normal derivative at the boundary.

3. What is an example of solving Laplace's equation with mixed boundary conditions?

An example of solving Laplace's equation with mixed boundary conditions is finding the steady-state temperature distribution in a rectangular plate with one side held at a constant temperature and the other sides insulated.

4. What are some challenges in solving Laplace's equation with mixed boundary conditions?

One challenge in solving Laplace's equation with mixed boundary conditions is that the boundary conditions may not be compatible, meaning that there is no solution that satisfies all of the conditions. Another challenge is that the problem may have multiple solutions.

5. How do you verify the solution to Laplace's equation with mixed boundary conditions?

To verify the solution to Laplace's equation with mixed boundary conditions, you can use the method of superposition. This involves adding the solutions to the individual boundary conditions and comparing it to the overall solution. You can also use numerical methods to check for convergence and accuracy.

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