Potential of a solid, double cone shaped charge distribution

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Discussion Overview

The discussion revolves around the analytical expression for the electrostatic potential generated by a charge distribution confined to a double cone shaped region. Participants explore the implications of a beam of charged particles converging to a focus and then diverging, with a focus on the charge density's relationship to the cross-sectional area of the beam. The scope includes theoretical considerations and mathematical reasoning related to electrostatics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • Some participants inquire about the specific points where the potential is needed, indicating a need for clarity in the problem statement.
  • One suggestion is to consult Smythe's "Static and Dynamic Electricity" for potential solutions, highlighting the complexity of the problem.
  • A participant describes the process of computing the potential at a point created by a uniformly charged disk and suggests integrating this over the double cone structure.
  • Another participant notes that the problem is complicated, even for simpler cases like a disk, and proposes using elliptic integrals for potential calculations.
  • A different approach is suggested involving the geometry of the cones and integrating over the linear charge density, indicating that the calculations are not straightforward.

Areas of Agreement / Disagreement

Participants express varying degrees of uncertainty regarding the complexity of the problem and the methods to approach it. There is no consensus on a definitive solution or method, and multiple approaches are discussed without resolution.

Contextual Notes

The discussion reveals limitations in the clarity of the problem statement and the assumptions made regarding the charge distribution and potential calculations. The mathematical steps involved in the proposed solutions remain unresolved.

Who May Find This Useful

This discussion may be of interest to those studying electrostatics, particularly in relation to complex charge distributions and potential calculations in theoretical physics.

Philip Koeck
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Does anybody know if there is an analytical expression for the electrostatic potential produced by a charge distribution confined to a double cone shaped region. Think of a beam of charged particles converging to a focus and then diverging again. The total charge in each thin, cross-sectional slab of this beam has to be constant. Therefore the charge density is inversely proportional to the local, cross-sectional area of the beam. The beam (double cone) can be treated as extending infinitely far in both directions.
Something similar might also help.
 
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You've forgotten to precise at which points you need the potential.
 
If you seek an analytical solution I suggest checking Smythe "Static and Dynamic Electricity". The number of cases it deals with is very large (if the solution isn't there I can't imagine other book)
 
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coquelicot said:
You've forgotten to precise at which points you need the potential.
Everywhere. Both inside and outside the charge distribution.
 
Philip Koeck said:
Does anybody know if there is an analytical expression for the electrostatic potential produced by a charge distribution confined to a double cone shaped region. Think of a beam of charged particles converging to a focus and then diverging again. The total charge in each thin, cross-sectional slab of this beam has to be constant. Therefore the charge density is inversely proportional to the local, cross-sectional area of the beam. The beam (double cone) can be treated as extending infinitely far in both directions.
Something similar might also help.

In general the problem amount to computing the potential V(t, r) at a point (x,y,z), created by a disk of radius r at ordinate t along a given axis (the axis is fixed), and uniformly charged with a total charge q. Once you have it, you sum ##\int_{-\infty}^{+\infty} V(|\alpha t|) dt##, where ##\alpha## is the coefficient giving the aperture of the cones.
Hope this will help.
 
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coquelicot said:
Added: this article seems to suggest this is far from being a simple problem, even for the case of a simple disk.
https://www.sciencedirect.com/science/article/pii/S0893965911002564
Yes, it seems so. One way to do it would be to take the potential of a ring, which involves an elliptic integral, then integrate over such rings with different radii to get a disk, and then integrate over z as you described earlier. The integrals are probably nightmares.
 
You may try another attack: Let O be the point of crossing of the two cones. Let M be a point in the space, and L be a straight line passing through O.
W.l.g, O is the origin and the axis of the two cones is the x-axis. Now, w.l.g, M is in the plane x-y.
Let d be the distance of a point x on L to M, that is ##d = h \cot(\alpha)## where h is the orthogonal distance of M to d. It may be possible to compute ##\int_{-\infty}^{+\infty} \rho(\alpha) d\ d\alpha##, that is, the potential created by L, while ##\rho## is the linear density of charge inherited from the disk of the double cone it is crossing (compute it). Then you have to sum in spherical coordinates the potential generated by the lines L you've just found (:biggrin:). Definitely not trivial.
 
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