Laplace's equation in presence of a dipole (perfect or physical)

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Discussion Overview

The discussion revolves around the application of Laplace's and Poisson's equations in the context of electrostatic potential related to dipoles, specifically addressing whether Laplace's equation is valid at the location of a dipole or if Poisson's equation should be used instead. The conversation includes theoretical considerations and problem-solving approaches related to dipoles embedded in dielectric materials.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning
  • Homework-related

Main Points Raised

  • Some participants argue that Poisson's equation should be used for the electrostatic potential at the location of a dipole, while Laplace's equation applies elsewhere.
  • One participant describes the charge distribution for an idealized dipole as a delta distribution and its derivative, indicating that the potential satisfies Laplace's equation except at the dipole.
  • Another participant questions the sign in the charge distribution expression, suggesting a possible oversight.
  • A participant presents a problem involving a point dipole in a dielectric sphere and inquires about solving it using Laplace's equation and the superposition principle.
  • Responses to the problem suggest using Laplace's equation outside the sphere and Poisson's equation inside, while also noting the need to check boundary conditions and correct algebraic mistakes.
  • Some participants emphasize that the potential should satisfy Poisson's equation everywhere, with the defined source charge density.

Areas of Agreement / Disagreement

Participants express differing views on whether Laplace's or Poisson's equation is appropriate at the dipole location, indicating a lack of consensus. Additionally, there are multiple approaches suggested for solving the problem involving the dipole in a dielectric sphere.

Contextual Notes

Participants highlight the importance of charge distribution definitions and boundary conditions in their discussions, but specific assumptions and limitations in the problem-solving process remain unresolved.

Ahmed1029
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TL;DR
I'm wondering if the laplacian of the electrostatic potential function will still be zero at the location of a dipole.
Does Laplace's equation hold true for electrostatic potential at the location of a dipole? Or should poisson's equation be used?
 
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You need to use Poisson’s equation. However, just as for a point charge, you need to be wary of what charge distribution you put in. In the case of a point charge, the charge distribution is a three-dimensional delta distribution. In the case of an idealised dipole it is a delta distribution in two directions and a derivative of a delta distribution in the direction of the dipole:
$$
\rho = \vec p \cdot \nabla \delta^{(3)}(\vec x).
$$

This means the potential will satisfy the Laplace equation everywhere except at the dipole.
 
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Orodruin said:
You need to use Poisson’s equation. However, just as for a point charge, you need to be wary of what charge distribution you put in. In the case of a point charge, the charge distribution is a three-dimensional delta distribution. In the case of an idealised dipole it is a delta distribution in two directions and a derivative of a delta distribution in the direction of the dipole:
$$
\rho = \vec p \cdot \nabla \delta^{(3)}(\vec x).
$$

This means the potential will satisfy the Laplace equation everywhere except at the dipole.
Shouldn't we have a minus sign here?
 
LCSphysicist said:
Shouldn't we have a minus sign here?
Possibly, I did not think too much about signs.

(As Feynman allegedly said: Factors of 2, pi, and i are only for publication purposes 😉)
 
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so consider the following problem :

"A point dipole p is imbedded at the center of a sphere of linear
dielectric material (with radius R and dielectric constant e). Find the electric po-
tential inside and outside the sphere."

How can I solve it only using Laplace's equation? Do I use the superposition principle ?
 
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Ahmed1029 said:
so consider the following problem :

"A point dipole p is imbedded at the center of a sphere of linear
dielectric material (with radius R and dielectric constant e). Find the electric po-
tential inside and outside the sphere."

How can I solve it only using Laplace's equation? Do I use the superposition principle ?
Solve Laplace equation outside.
Solve Poisson equation inside.
Reject terms that blows up as r goes to infinity.
Check the boundary conditiions at the sphere.
Realize that you have made an algebric mistake.
Returns to step 1
Realize you have made another algebraic mistake.
Returns to step 1.
Get the right answer.

That't the recipe
 
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Orodruin said:
This means the potential will satisfy the Laplace equation everywhere except at the dipole.
I think it is much better to say that the potential will satisfy the Poisson equation everywhere, with source charge density the one you defined.
 
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Delta2 said:
I think it is much better to say that the potential will satisfy the Poisson equation everywhere, with source charge density the one you defined.
Got it, thanks!
 
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