What's wrong? Electric potential of a point on a ring

AI Thread Summary
The discussion focuses on calculating the electric potential at the origin of a uniformly charged ring, revealing that the potential diverges due to the ring's infinitesimal thickness, which implies an infinite charge density at points on the ring. It is clarified that while the electric field and potential are infinite at the ring's circumference, they remain well-defined for points inside or outside the ring. The conversation also touches on the behavior of potential near line charges, noting that it diverges logarithmically as one approaches the charge. Additionally, the distinction between volume and surface charge densities is emphasized, with the potential being well-defined for surface charges despite infinite density at the surface. The discussion concludes with references to literature on the topic, suggesting further reading for deeper understanding.
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So I have a ring(red) of uniform charge ##\lambda## per unit length, and I want to calculate the electric potential at the origin (actually on any point of the ring). It is clear that the ring is given by the equation $$r=2 R \sin \theta$$, in polar coordinates, where R is the radius of the ring. Since potential is given by $$V = \frac{1}{4 \pi \epsilon_0} \int \frac{dq}{r}$$, and $$dq = d\ell \lambda$$, but $$d\ell = \sqrt{(\frac{dr}{d\theta})^2 + r^2} d\theta = 2R d\theta$$. Therefore, $$V = \frac{1}{4 \pi \epsilon_0} \int \frac{d\ell \lambda}{r} = \frac{1}{4 \pi \epsilon_0} \int^{\pi}_{0} \frac{2R\lambda}{2R \sin \theta} d\theta = \frac{1}{4 \pi \epsilon_0} \lambda \int^{\pi}_{0} \frac{1}{\sin \theta} d\theta$$, which does not converge... what's wrong?

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Yes because the ring is infinitesimally thin and has finite charge density ##\lambda## the electric field (and potential) is infinite for points on the ring circumference. Electric field and Potential are well defined for points on the interior or the exterior of the ring though.
Hold on for a minute while I locate a previous thread where this was discussed in more detail.

Here it is
https://www.physicsforums.com/threads/what-is-the-tension-in-a-charged-ring.990825/post-6360966
 
My explanation is that we know from Gauss's law in differential form that $$\nabla\cdot\vec{E}=\frac{\rho}{\epsilon_0}$$ and $$\nabla^2 V=-\frac{\rho}{\epsilon_0}$$.

Where ##\rho## is the volume (not the linear) charge density. Because the ring is infinitesimally thin the ##\rho## of the ring become infinite for points on the ring, hence from the above two equations, electric field and potential become infinite too.
 
Delta2 said:
My explanation is that we know from Gauss's law in differential form that $$\nabla\cdot\vec{E}=\frac{\rho}{\epsilon_0}$$ and $$\nabla^2 V=-\frac{\rho}{\epsilon_0}$$.

Where ##\rho## is the volume (not the linear) charge density. Because the ring is infinitesimally thin the ##\rho## of the ring become infinite for points on the ring, hence from the above two equations, electric field and potential become infinite too.
Uh oh! I spent quite some time wondering where did I get it wrong... Luckily I asked. thanks!
 
Delta2 said:
Because the ring is infinitesimally thin the ρ of the ring become infinite for points on the ring
Oh yes, just curious, for surface charge density, like a thin sheet of charge, we also assume that it's infinitesimally thin. Does this also mean that ##\rho## is infinite?
 
Delta2 said:
My explanation is that we know from Gauss's law in differential form that $$\nabla\cdot\vec{E}=\frac{\rho}{\epsilon_0}$$ and $$\nabla^2 V=-\frac{\rho}{\epsilon_0}$$.

Where ##\rho## is the volume (not the linear) charge density. Because the ring is infinitesimally thin the ##\rho## of the ring become infinite for points on the ring, hence from the above two equations, electric field and potential become infinite too.
This argument is unfortunately invalid as it does not work for a surface charge where the volume charge density becomes formally infinite at the surface, but the potential is well defined.

Instead, we need to argue how the potential behaves as we get closer to the wire. As we approach a line charge and the distance ##\ell## to the charge is much smaller than the curvature radius of the line, the porential behaves as proportional to ##\ln(\ell)## (it must because of the divergence theorem). Therefore, the potential diverges and the field diverges as ##1/\ell##.
 
Yes ok I see now, infinity of the divergence of a field at a point doesn't necessarily imply infinity of the field at that point.
 
Delta2 said:
Yes ok I see now, infinity of the divergence of a field at a point doesn't necessarily imply infinity of the field at that point.
Indeed, but almost always. The exception is when the source is spread over a hypersurface of one dimension lower than the space itself. The reason is that the one-dimensional Green function of the Laplace operator does not diverge, but for any higher dimension it does
 
Orodruin said:
Indeed, but almost always
Thanks good to know that .
 
  • #10
Orodruin said:
This argument is unfortunately invalid as it does not work for a surface charge where the volume charge density becomes formally infinite at the surface, but the potential is well defined.

Instead, we need to argue how the potential behaves as we get closer to the wire. As we approach a line charge and the distance ##\ell## to the charge is much smaller than the curvature radius of the line, the porential behaves as proportional to ##\ln(\ell)## (it must because of the divergence theorem). Therefore, the potential diverges and the field diverges as ##1/\ell##.

Orodruin said:
Indeed, but almost always. The exception is when the source is spread over a hypersurface of one dimension lower than the space itself. The reason is that the one-dimensional Green function of the Laplace operator does not diverge, but for any higher dimension it does

Are there any discussions (in books, articles) about these? The closest I found is Jackson pg. 32 the paragraph below equation (1.23) "For colume or surface distributions of charge, the potential is everywhere continuous... from the fact that E is bounded". Maybe one can carry out the limiting procedures themselves to verify, as suggested by Jackson...

Thanks in advance!
 
  • #11
@Orodruin? Do you know where to read up on the green's function thing?
 
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