Solving electrostatic, rotationally symmetric 3D problem with conformal mapping?

In summary, the conversation discusses the use of conformal mapping and complex numbers to solve 2D problems. While this method is effective for 2D problems, it is not applicable to 3D axial-rotationally symmetric problems or azimuthally symmetric 3D problems. The use of conformal mapping was also mentioned in a reference text by Weber, but it was found to be an approximation and not a general solution.
  • #1
Gerenuk
1,034
5
I heard that one can solve 2D problem with conformal mapping of complex numbers.
Is it possible to use this method for 3D axial-rotationally symmetric problems (which are effectively 2D with a new term in the differential equation)?
 
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  • #2
Azimuthally symmetric 3D problems have different solutions than 2D ones, so solution approaches are not interchangeable. Take a cut through a cylinder including the axis--it looks like a rectangle, but radial solutions are Bessel functions. The sine/cosine solutions you'd get from solving it as a 2D rectangle are flat out wrong.
 
  • #3
I know that.
I was wondering if one can still use some kind of complex variable method such as conformal mapping to treat this 2D problem.
 
  • #4
To be clear on what you mean by "this" 2D problem:
Solution of 2D problem in a planar boundary like rectangle--yes
Solution of 3D azimuthally symmetric problems--no.

Actually, Weber recounts that Maxwell evaluated the capacitance of parallel plates with guard rings by approximating as a 2D conjugate-function solution valid far from the axis. The general answer is no.

Weber, Electromagnetic Fields, Vol. 1: Mapping and Fields, Wiley, 1950.
 
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Related to Solving electrostatic, rotationally symmetric 3D problem with conformal mapping?

1. What is conformal mapping and how does it relate to electrostatic problems?

Conformal mapping is a mathematical technique used to transform a complex problem into a simpler, more manageable one. In the context of electrostatic problems, conformal mapping can be used to map a complex 3D problem onto a simpler, rotationally symmetric 2D problem. This simplifies the problem and allows for easier solution using known techniques.

2. How do you solve electrostatic problems using conformal mapping?

To solve an electrostatic problem using conformal mapping, the first step is to map the 3D problem onto a 2D domain using a conformal mapping function. Once the problem is simplified to a 2D domain, known techniques such as the method of images or separation of variables can be used to solve the problem. Finally, the solution can be mapped back to the original 3D domain to obtain the complete solution.

3. What are the benefits of using conformal mapping to solve electrostatic problems?

Using conformal mapping to solve electrostatic problems has several benefits. It simplifies the problem by reducing it to a 2D domain, making it easier to solve using known techniques. It also allows for visualization of the problem in 2D, providing insight into the behavior of the electric field. Additionally, conformal mapping can be used to solve problems with complex geometries that are difficult to solve using other methods.

4. Are there any limitations to using conformal mapping to solve electrostatic problems?

While conformal mapping is a powerful technique for solving electrostatic problems, it does have some limitations. It works best for problems with rotationally symmetric geometries and may not work well for problems with irregular or non-symmetric geometries. Additionally, conformal mapping may not provide an exact solution to the problem but rather an approximation.

5. Can conformal mapping be applied to other types of problems?

Yes, conformal mapping can be applied to a variety of problems in physics, engineering, and mathematics. It is commonly used in fluid dynamics, heat transfer, and electromagnetic problems. It can also be used in other areas such as image processing and computer graphics. The key is to find a conformal mapping function that can transform the problem into a simpler form without changing its essential characteristics.

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