Solving Laplace's Equation for 2D isosceles right triangle

In summary: Yes I was actually considering that, but I wasn't completely sure if I was justified in thinking the diagonal would be zero. You suggesting it gives me more confidence in it, so I'll try that route. Thanks.
  • #1
Infernorage
24
0

Homework Statement


Find the two-dimensional solution to Laplace's equation inside an isosceles right triangle. The boundary conditions are as is shown in the picture:

laplace%20eq%20triangle_zpsf6unqero.png

The length of the bottom and left side of the triangle are both L.

Homework Equations


Vxx+Vyy=0
V=X(x)Y(y)
From the image, it is clear that two of the boundary conditions are...
V(0,y) = 1
V(x,0) = 1

The Attempt at a Solution


My problem is getting started. I need more boundary conditions, but I am not sure how to get them. Also, I need use superposition or something to impose periodicity onto some part of this problem, but I can figure out how to do it. Also, another option is the zero option where X(x) = Y(y) = 0, but that doesn't seem to work either.

The only other boundary condition I can think of is V(x,L-x) = 0, but that doesn't seem to be enough information.

Can anyone help me get started with this problem? Thanks in advance.
 
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  • #2
Why do you not think you have enough boundary conditions?
Given a (reasonably nice) region, it is sufficient to know the value on the boundary or the normal derivative on the boundary in order to solve the Laplace equation.
 
  • #3
Orodruin said:
Why do you not think you have enough boundary conditions?
Given a (reasonably nice) region, it is sufficient to know the value on the boundary or the normal derivative on the boundary in order to solve the Laplace equation.
Are my boundary conditions correct? It seems to me that either I don't have enough or perhaps the one on the diagonal is wrong because the subsequent equations for X(x), Y(y) and V don't seem to simplify enough when I plug the BC's in.
 
  • #4
There is no guarantee that your eigenfunctions or solution will be separable in x and y. The boundary conditions are sufficient for a solution to exist.
 
  • #5
Orodruin said:
There is no guarantee that your eigenfunctions or solution will be separable in x and y. The boundary conditions are sufficient for a solution to exist.
I'm pretty sure there is some way to find separable solutions, because the assignment is only about Laplace's equation involving separable solutions. However, I just can't seem to figure out how to apply the BC's to find the form of the solutions. This first step is what I am stuck on.
 
  • #6
There might be an easier way to do this, but here's a suggestion. Consider a square with V=1 along the left and bottom sides and V=-1 along the top and right sides. It seems plausible that you'll have V=0 along the diagonal going from the top left to bottom right, just as the problem requires, and with a square region, you'll be able to apply separation of variables in a straightforward way.
 
  • #7
vela said:
There might be an easier way to do this, but here's a suggestion. Consider a square with V=1 along the left and bottom sides and V=-1 along the top and right sides. It seems plausible that you'll have V=0 along the diagonal going from the top left to bottom right, just as the problem requires, and with a square region, you'll be able to apply separation of variables in a straightforward way.
Yes I was actually considering that, but I wasn't completely sure if I was justified in thinking the diagonal would be zero. You suggesting it gives me more confidence in it, so I'll try that route. Thanks.
 
  • #8
There is really no problem in doing this, it is simply an odd mirroring in the diagonal plane and is perfectly well motivated. The problem appears if you try to separate the solutions in the original region. The point here is that you will get solutions to the resulting inhomogeneous boundary conditions in the x- and y-directions separately. These will in the end add up in such a way tht they produce a zero on the diagonoal.
 

Related to Solving Laplace's Equation for 2D isosceles right triangle

What is Laplace's Equation for 2D isosceles right triangle?

Laplace's Equation for 2D isosceles right triangle is a mathematical equation used to describe the electric potential distribution in a 2D isosceles right triangle. It is a special case of Laplace's Equation and is often used in electrostatics and heat transfer problems.

How do you solve Laplace's Equation for 2D isosceles right triangle?

Solving Laplace's Equation for 2D isosceles right triangle involves using mathematical techniques such as separation of variables, Fourier series, and boundary conditions. It requires a deep understanding of calculus and linear algebra.

What are the applications of solving Laplace's Equation for 2D isosceles right triangle?

Solving Laplace's Equation for 2D isosceles right triangle has various applications in physics and engineering. It is commonly used in electrostatics to determine the electric potential distribution in a 2D isosceles right triangle. It is also used in heat transfer problems to calculate the temperature distribution in a 2D isosceles right triangle.

What are the challenges in solving Laplace's Equation for 2D isosceles right triangle?

Solving Laplace's Equation for 2D isosceles right triangle can be challenging due to the complexity of the equation and the need for advanced mathematical techniques. It also requires careful consideration of boundary conditions and initial conditions.

Are there any real-life examples where solving Laplace's Equation for 2D isosceles right triangle is useful?

Yes, there are many real-life examples where solving Laplace's Equation for 2D isosceles right triangle is useful. Some examples include calculating the electric potential distribution in a triangular-shaped electronic circuit or determining the temperature distribution in a triangular-shaped metal plate.

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