Gauss' Law: Cylindrical Symmetry

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Discussion Overview

The discussion centers around the application of Gauss' Law to a positively charged rod with uniform charge density, specifically examining the electric field inside the rod and the assumptions made regarding cylindrical symmetry. Participants explore the implications of these assumptions and the conditions under which Gauss' Law can be applied.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant notes that when deriving the electric field equation using Gauss' Law, the assumption is made that the radius R of the charged rod is significantly smaller than the length L of the cylinder.
  • Another participant suggests that in an ideal scenario where the charged rod is infinitely long, the cylindrical symmetry allows for the application of Gauss' Law even for points inside the charged body.
  • A participant questions the assumption that the electric field inside the rod can be considered zero, arguing that a uniformly charged rod should produce some electric field within it, except at the center where fields may cancel.
  • In response, one participant agrees that the assumption of zero electric field does not make sense, indicating a disagreement on this point.
  • Another participant introduces the idea that if the rod is a conductor, then charge resides on the surface, leading to no electric field inside, but suggests that for this discussion, a uniform charge density within an insulating rod should be assumed.

Areas of Agreement / Disagreement

Participants express disagreement regarding the electric field inside the charged rod, with some arguing it should be zero while others contend it should not. The discussion remains unresolved on this point, with multiple competing views presented.

Contextual Notes

Participants highlight the importance of the assumptions made regarding the nature of the rod (insulating vs. conducting) and the implications of these assumptions on the electric field calculations. There is also mention of the ideal conditions required for applying Gauss' Law effectively.

Arsenal
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Say we are looking at a positively charged rod with uniform charge density and a radius of R.

When using Gauss' law and taking a cylindrical surface we use the formula
E = lambda/2*pi*epsilon*r

When we derive this equation we are assuming R is significantly smaller than L and so we consider the charged body to be similar to an rod that is co-axial to the Gaussian cylinder.

What if we want to consider what E is inside the cylinder at say r=R/2

I have read on another forum that we would consider the electric field inside the rod as 0 but that doesn't make sense because a charged rod with uniform charge density will have some electric field inside the rod as long as we are not right in the center where the field would cancel each other out.

If we do consider the EF inside the rod to be 0 then we must be assuming that the diifference between the magnitude of the EF caused from the opposite sides of the rod is insignificant but I do not see this assumption clarified anywhere.

Could someone please clarify this for me?

Thanks
 
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Arsenal said:
When we derive this equation we are assuming R is significantly smaller than L and so we consider the charged body to be similar to an rod that is co-axial to the Gaussian cylinder.

If you assume an ideal scenario in which the uniformly charged body is infinitely long, the cylindrical symmetry is perfect, and you can apply Gauss's law and the Gaussian cylindrical surface for any radius, even one inside the charged body.

The assumption that R must be much less than L is then the condition for using the above ideal scenario to model a real world scenario where L is never infinite.
 
Arsenal said:
What if we want to consider what E is inside the cylinder at say r=R/2

Remember Gauss's Law says: the total flux of E through a closed surface equals the total charge enclosed by the surface, divided by \epsilon_0.

1. What is the total charge enclosed by a cylinder of length L and radius r, and with a uniform charge density \rho?

2. Assuming that E is directed radially outward, and uniform over the outer surface of the cylinder, because of the cylindrical symmetry, what is the total flux through the surface, in terms of the unknown value of E?
 
"I have read on another forum that we would consider the electric field inside the rod as 0 but that doesn't make sense".
It doesn't make sense.
 
Well it might make sense. If the rod is not perfectly insulating, then it is a conductor. All charge appears on the surface of conductors, since in electrostatics, there is no E-field inside a conductor.

For the purpose of this question, I think you would be expected to assume a uniform charge density within the (insulating) rod.
Peter
 

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