Volume Charge Density in a long Cylinder

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SUMMARY

The discussion focuses on calculating the volume charge density within a long solid cylinder of radius R, using a cylindrical Gaussian surface of radius r (where r < R). The user seeks to determine the enclosed charge (q) in terms of charge density (ρ), length (L), and radius (r). The correct approach involves integrating the charge density over the volume of the Gaussian surface, leading to the conclusion that q = ρ * (π * r² * L). The user expresses confusion regarding the relationship between q and the total charge (Q) of the cylinder, which is defined as Q = ρ * (π * R² * L).

PREREQUISITES
  • Understanding of Gaussian surfaces in electrostatics
  • Familiarity with volume charge density (ρ) and linear charge density (λ)
  • Basic knowledge of electric field calculations in cylindrical coordinates
  • Ability to perform volume integrals in physics
NEXT STEPS
  • Study the application of Gauss's Law in cylindrical symmetry
  • Learn about the derivation of electric fields from volume charge densities
  • Explore the differences between volume charge density and linear charge density
  • Review examples of Gaussian surfaces in various geometries
USEFUL FOR

Students studying electrostatics, physics educators, and anyone seeking to deepen their understanding of charge distribution in cylindrical geometries.

MtHaleyGirl
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I am never sure if I am on the right track when answering my homework problems. Anyway the problem involves a long solid cylinder of radius R and uniform charge distribution throughout its volume. We are supposed to choose a cylindrical gaussian surface of radius r and length L with r < R - so the gaussian surface is inside the cylinder. We are 1st supposed to determine q(enclosed) in terms of ρ (rho), L and r - and of course any other relevant constants. So first off - I am looking at the flux within the cylinder --- already I am nervous about this because I cannot think of how to imagine the flux within this cylinder... and then considering E ? So to further explain where I am at - since the cylinder is "very very long" I have capped off the gaussian cylinder inside the whole. 1st off - is q(enclosed) a ratio of the whole Q ? or is it constant within the cylinder (I don't think q = Q). I want to consider q/Q - where q = π(pi) r² L then Q = π R² L - then I want to take q/Q = (π(pi) r² L )/(π R² L ) - cancel the π(pi) and L to get q =(Qr²)/R² - then I wonder if I am getting anywhere = also does q = ρL - it shows in my book that q = λL (λ is linear charge density) and I don't know if it works for volume charge density too... :rolleyes: - feeling like a physics flunky...
 
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Thanks, but I've been there - the gaussian surface is always shown outside the original cylinder, that is why I am confused... :confused:
 
MtHaleyGirl said:
Thanks, but I've been there - the gaussian surface is always shown outside the original cylinder, that is why I am confused... :confused:

Recall that all you care about is the net charge INSIDE the Gaussian surface, so we can ignore anything outside the surface. To get the charge inside, just take the volume integral over the charge density.

-Dan
 
No No No! :smile: I've been to hyperphysics lots - the Gaussian surface is a cylinder within another cylinder. All of the examples I have seen the cylinder is used through a plane or around another cylinder. The Charged Cylinder is of radius R and the Gaussian surface is radius r r < R... Does that make sense? I'm no physics genius and when I am given a problem outside the regular examples I feel like my brain is being scrambled - - - thanks though
 
using vectors, i make the electric field E = -lamda/2pi(sqrt.[r^2-s^2])epsilon

r^2 = s^2 +(c-a)^2, (and b is c-a), therefore rearrange, (c-a)^2 is (r^2-s^2)

does this help?
 

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