Electric field of a long round bar

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Homework Help Overview

The discussion revolves around proving that the electric field around a long conductive round bar of radius R is equivalent to that of a long thin wire, with the charge assumed to be concentrated along the center line. The participants explore the application of Gauss's law in this context.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the application of Gauss's theorem to derive the electric field, considering both the charge per unit length and the charge per unit surface. Questions arise about the validity of their methods and the implications of using different unit systems.

Discussion Status

The discussion includes attempts to clarify the relationship between the electric field expressions derived for both the conductive bar and the thin wire. Some participants express discomfort with their understanding, while others affirm the correctness of the approaches taken. There is an ongoing exploration of the implications of their findings.

Contextual Notes

Participants note that the results may vary depending on the unit system used, specifically mentioning the cgs system where ε0=1. There is also mention of the need to clarify assumptions regarding charge distribution.

Karol
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Homework Statement


I have to prove that the electric field round a long conductive round bar of radius R is equal to that of a long thin wire, meaning the charge is on the center line

Homework Equations


The Gauss theorem:
##E\times A=q##
Where A is the area of the surface and q is the charge enclosed in it

The Attempt at a Solution


To find the field E when the charge is concentrated on the axis i take a round long volume with radius r:
##E\times 2\pi rl=\lambda l\rightarrow E=\frac{\lambda}{2\pi r}##
Where [itex]\lambda[/itex] is the charge per unit length.
The field near a round bar:
##E\times 2\pi rl=\sigma\cdot 2\pi R l##
Where [itex]\sigma[/itex] is the charge per unit surface, since the charge is concentrated only on the surface.
But [itex]\sigma\cdot 2\pi R l=\lambda l[/itex]
They both are the charge per unit length. and so is if i use the charge per unit mass.
I feel uncomfortable
 
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Karol said:

Homework Statement


I have to prove that the electric field round a long conductive round bar of radius R is equal to that of a long thin wire, meaning the charge is on the center line

Homework Equations


The Gauss theorem:
##E\times A=q##
Where A is the area of the surface and q is the charge enclosed in it

It is true if you use cgs system of units where ε0=1.

Karol said:

The Attempt at a Solution


To find the field E when the charge is concentrated on the axis i take a round long volume with radius r:
##E\times 2\pi rl=\lambda l\rightarrow E=\frac{\lambda}{2\pi r}##
Where [itex]\lambda[/itex] is the charge per unit length.

Correct.

Karol said:
The field near a round bar:
##E\times 2\pi rl=\sigma\cdot 2\pi R l##
Where [itex]\sigma[/itex] is the charge per unit surface, since the charge is concentrated only on the surface.
But [itex]\sigma\cdot 2\pi R l=\lambda l[/itex]
Simplifying, you get that E=σ R/r and σ =λ/(2πR). Substitute the second equation into the first, what do you get? Is E the same as in case of a thin long wire at the centre?
 
I get ##E=\frac{\lambda}{2\pi r}## like for a long thin wire at the center, and that's good, but i feel uncomfortable with that, is that the method to prove it?
 
You do not need to feel uncomfortable, it was the right proof. :) Good job!
 
Thanks
 

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