1 / 24

The Laplace Equation

The Laplace Equation. Chris Olm and Johnathan Wensman December 3, 2008. Introduction (Part I). We are going to be solving the Laplace equation in the context of electrodynamics Using spherical coordinates assuming azimuthal symmetry

liviag
Download Presentation

The Laplace Equation

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. The Laplace Equation Chris Olm and Johnathan Wensman December 3, 2008

  2. Introduction (Part I) • We are going to be solving the Laplace equation in the context of electrodynamics • Using spherical coordinates assuming azimuthal symmetry • Could also be solving in Cartesian or cylindrical coordinates • These would be applicable to systems with corresponding symmetry • Begin by using separation of variables • Changes the system of partial differential equations to ordinary differential equations • Use of Legendre polynomials to find the general solution

  3. Introduction (Part II) • We will then demonstrate how to apply boundary conditions to the general solution to attain particular solutions • Explain and demonstrate using “Fourier’s Trick” • Analyzing equations to give us a workable solution

  4. The Laplace Equation • Cartesian coordinates • V is potential • Harmonic! • Spherical coordinates • r is the radius •  is the angle between the z-axis and the vector we’re considering •  is the angle between the x-axis and our vector

  5. Azimuthal Symmetry • Assuming azimuthal symmetry simplifies the system • In this case, decoupling V from Φ becomes

  6. Potential Function • Want our function in terms of r and θ • So • Where R is dependent on r • Θ is dependent on θ

  7. ODEs! • Plugging in we get: • These two ODEs that must be equal and opposite: . ↓ ↓

  8. General Solution for R(r) • Assume • Plugging in we get So • We can deduce that the equation is solved when k=l or k=-(l+1) • So our general solution for R(r) is

  9. General Solution for Θ(θ) • Legendre polynomials • The solutions to the Legendre differential equation, where l is an integer • Orthogonal • Most simply derived using Rodriques’s formula: • In our case x=cosθ so

  10. Let l=0: Let l=3: Θ(θ) Part 2 □ ↘ ↘ ↓ ↘ □

  11. The General Solution for V • Putting together R(r), Θ(θ) and summing over all l becomes

  12. Applying the general solution

  13. Example 1 • The potential is specified on a hollow sphere of radiusR What is the potential on the inside of the sphere?

  14. Applying boundary conditions and intuition • We know it must take the form • And on the surface of the sphere must be V0, also all Bl must be 0, so we get • The question becomes are there any Al which satisfy this equation?

  15. Yes! But doing so is tricky • First we note that the Legendre polynomials are a complete set of orthogonal functions • This has a couple consequences we can exploit

  16. Applying this property • We can multiply our general solution by Pl’’(cos θ) sin θ and integrate (Fourier’s Trick)

  17. Solving a particular case • We could plug this into our equation giving • In scientific terms this is unnecessarily cumbersome (in layman's terms this is a hard integral we don’t want or need to do)

  18. The better way • Instead let’s use the half angle formula to rewrite our potential as • Plugging THIS into our equation gives • Now we can practically read off the values of Al

  19. Getting the final answer • Plugging these into our general solution we get

  20. Example 2 • Very similar to the first example • The potential is specified on a hollow sphere of radius R • What is the potential on the outside of the sphere?

  21. Proceeding as before • Must be of the form • All Al must be 0 this time, and again at the surface must be V0, so • and

  22. Fourier’s Trick again • By applying Fourier’s Trick again we can solve for Bl • As far as we can solve without a specific potential

  23. Conclusion • By solving for the general solution we can easily solve for the potential of any system easily described in spherical coordinates • This is useful as the electric field is the gradient of the potential • The electric field is an important part of electrostatics

  24. References • 1)Griffiths, David. Introduction to Electrodynamics. 3rd ed. Upper Saddle River: Prentice Hall, 1999. • 2)Blanchard, Paul, Robert Devaney, and Glen Hall. Differential equations. 3rd ed. Belmont: Thomson Higher Education, 2006. • 3) White, J. L., “Mathematical Methods Special Functions Legendre’s Equation and Legendre Polynomials,” • http://www.tmt.ugal.ro/crios/Support/ANPT/Curs/math/s8/s8legd/s8legd.html, accessed 12/2/2008. • 4) Weisstein, Eric W. "Laplace's Equation--Spherical Coordinates." From MathWorld--A 5) Wolfram Web Resource. http://mathworld.wolfram.com/LaplacesEquationSphericalCoordinates.html, accessed 12/2/2008

More Related