Gauss's law for a charged ring

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SUMMARY

The discussion centers on the application of Gauss's law to a uniformly charged ring of radius R and the electric field produced along its axis. The electric field E_z is proportional to Qz/(R^2+z^2), indicating a net field along the axis. However, when considering a Gaussian sphere of radius r centered at the ring, the confusion arises because there is no charge enclosed, leading to the assumption that the electric field must be zero. Participants clarify that Gauss's law states that if the net charge is zero inside a Gaussian surface, the total flux is zero, but this does not imply that the electric field itself is zero.

PREREQUISITES
  • Understanding of Coulomb's law and electric fields
  • Familiarity with Gauss's law and its mathematical formulation
  • Knowledge of electric field symmetry
  • Conceptual grasp of Gaussian surfaces in electrostatics
NEXT STEPS
  • Study the implications of electric field symmetry in electrostatics
  • Learn about different types of Gaussian surfaces and their applications
  • Explore advanced topics in electrostatics, such as multipole expansions
  • Investigate the limitations of Gauss's law in non-uniform electric fields
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Physics students, educators, and anyone interested in deepening their understanding of electrostatics and the application of Gauss's law in complex scenarios.

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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