Gauss's law for a charged ring

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Discussion Overview

The discussion revolves around the application of Gauss's law to determine the electric field produced by a uniformly charged ring along its axis. Participants explore the conceptual challenges of using Gauss's law in this scenario, particularly when considering a Gaussian sphere that does not enclose any charge.

Discussion Character

  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that according to Coulomb's law, the electric field along the axis of the charged ring is proportional to Qz/(R^2+z^2), indicating a net field exists.
  • The same participant expresses confusion about using Gauss's law, stating that if a Gaussian sphere is placed at the center of the ring and encloses no charge, the electric field should be zero, which contradicts the finite electric field observed along the axis.
  • Another participant clarifies that Gauss's law pertains to the surface integral of the electric field, not the field at every point, and that the integral can be zero even if the field is not.
  • A different participant adds a visual explanation regarding field lines, stating that field lines entering the Gaussian sphere must also exit, reinforcing the idea that the total flux is zero due to the absence of enclosed charge.
  • A later reply reiterates that while Gauss's law is always valid, its effectiveness as a calculational tool depends on matching the symmetry of the electric field with that of the Gaussian surface.

Areas of Agreement / Disagreement

Participants generally agree on the validity of Gauss's law but express differing views on its applicability to the specific scenario of the charged ring and the chosen Gaussian surface. The discussion remains unresolved regarding the best approach to conceptualize the electric field in this context.

Contextual Notes

Participants acknowledge that the symmetry of the electric field produced by the ring does not align with the symmetry of the spherical Gaussian surface, which complicates the application of Gauss's law.

CuicCuic
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Hello physics world,

I am having a hard time understanding a rather simple thing. Let's consider the electric field produced by a uniformly charged ring of radius R, at a position $z$ along the ring's axis. From Coulomb's law in every textbook, we know that E_z∝Qz/(R^2+z^2). That is, there is a net field produced by the ring along its axis.

Now, if we consider the same problem with Gauss's law, I run into a conceptual problem. Let's say we take a Gaussian sphere with radius r, smaller than R, whose center is placed at the center of the ring. In that case, there is no charge enclosed within the Gaussian surface. So Gauss's law should say that the electric field must be zero. But we know that the electric field is finite along $z$ and does not cancel out from $z$ and $-z$. Instead it seems to me that the flux would be 2E_z.

There must be something wrong with my understanding of Gauss's Law, because as I understand it, if there is not charge inside the Gaussian sphere, the electric field flux through that sphere is 0. Any help clarifying this would be sincerely appreciated.

(I know that using Gauss's law for this problem is not a good idea because the field will not be constant in the surface integral. My question is thus rather conceptual.)
 
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Gauss's law applies to the surface integral of E, not E at every point.
It can only give E at each point if there is enough symmetry to say that E is constant on the surface.
Although E is not zero within your sphere, its integral over the surface of the sphere is zero.
 
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Or more visually, if you can imagine what the field lines look like for this situation: over some parts of your Gaussian sphere, the field lines enter the sphere, but over other parts, they leave the sphere. Field lines cannot simply "disappear into thin air", and there is no charge inside the sphere, so any field line that enters the sphere must leave the sphere somewhere else.
 
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Excellent responses! Thank you very much for clarifying the situation.
 
CuicCuic said:
Hello physics world,

I am having a hard time understanding a rather simple thing. Let's consider the electric field produced by a uniformly charged ring of radius R, at a position $z$ along the ring's axis. From Coulomb's law in every textbook, we know that E_z∝Qz/(R^2+z^2). That is, there is a net field produced by the ring along its axis.

Now, if we consider the same problem with Gauss's law, I run into a conceptual problem. Let's say we take a Gaussian sphere with radius r, smaller than R, whose center is placed at the center of the ring. In that case, there is no charge enclosed within the Gaussian surface. So Gauss's law should say that the electric field must be zero. But we know that the electric field is finite along $z$ and does not cancel out from $z$ and $-z$. Instead it seems to me that the flux would be 2E_z.

There must be something wrong with my understanding of Gauss's Law, because as I understand it, if there is not charge inside the Gaussian sphere, the electric field flux through that sphere is 0. Any help clarifying this would be sincerely appreciated.

(I know that using Gauss's law for this problem is not a good idea because the field will not be constant in the surface integral. My question is thus rather conceptual.)
Conceptually or otherwise, the point is that: Gauss'slaw says that if the net charge is zero inside a Gaussian surface, the total flux over the surface is zero. It does not say that the electric field is zero. Generally, Gauss's law is always true, but as a calculational tool, it has limited usefulness. You must match the symmetry of the field, with the symmetry of the Gaussian surface, if you need to calculate the field. In your case, the field of the ring has a very different symmetry compared to the symmetry of the spherical Gaussian surface you chose.
 

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