Solid cylinder with nonuniform volume charge density?

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Homework Help Overview

The problem involves a long, non-conducting solid cylinder with a nonuniform volume charge density described by the function ρ = Ar², where A is a constant. The questions focus on determining the electric field at specific radial distances from the cylinder's axis.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to integrate the charge density to find the linear charge density and subsequently the electric field. They express confusion regarding the correctness of their integration method and seek clarification on potential missing constants.
  • Some participants question the integration steps taken by the original poster and suggest a different approach to integrating the charge density.
  • Others discuss the necessity of using cylindrical coordinates for the integration and highlight the importance of including the radial component in the calculations.

Discussion Status

Contextual Notes

Participants note that the integration must account for the cylindrical coordinate system, which may not have been familiar to the original poster. There is an emphasis on the need for proper setup in the integration to arrive at the correct expressions for charge density.

LumiKnight
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Homework Statement



A long, non conducting, solid cylinder of radius 4.2 cm has a nonuniform volume charge density ρ = Ar^2, a function of the radial distance r from the cylinder axis. A = 2.5 µC/m5.

(a) What is the magnitude of the electric field at a radial distance of 3.2 cm from the axis of the cylinder?

(b) What is the magnitude of the electric field at a radial distance of 5.2 cm from the axis of the cylinder?

Homework Equations



e0 Ø = charge enclosed ; e0 is the permittivity constant 8.85e-12 and Ø can be the flux

e0 E(2π r L) = λ L ; λ is the linear charge density

The Attempt at a Solution

I thought that I could just integrate Ar^2 twice, which would give me λ. Then I could multiply by the height of the cylinder, L. After I did all that I arrived at this:

E=(Ar^3) / (24e0) with e0 being the permittivity constant.
The correct form would have me do this though:

charge enclosed = ∫ 2π r L (Ar^2) dr ; from 0 to r

= 2π L A ∫ r^3 dr ; from 0 to r

If you integrate that and solve for E you get this:

E=(Ar^3) / (4e0) <----- This gives the correct answer.Can someone explain to me why the method I'm using wrong? Is there some constant I am missing in my method? Or is it just wrong? And this is also my first post here on Physics Forums? Please tell me if I am doing something wrong so I can correct it in any future post.
 
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LumiKnight said:
I thought that I could just integrate Ar^2 twice, which would give me λ.
This is what you should be doing. How exactly did you integrate?
 
I would do this:

∫ A r^2 dr = A ∫ r^2 dr

That would give me this:

(1/3)A r^3

Integrating again treating A as a constant would then give me this:

(1/3)A ∫ r^3 dr = (1/12)A r^4


I could then set λ = (1/12)A r^4 , and I could substitute λ into the equation: e0 E(2π r L) = λ L

E = (A r^3) / (2π*e0*12) I forgot to divide by 2π. But doing that just makes the denominator bigger. :frown:
 
Last edited:
The integration is not correct. Remember this rule? [itex]dxdy=r \ dr \ d \theta[/itex]
 
BruceW said:
The integration is not correct. Remember this rule? [itex]dxdy=r \ dr \ d \theta[/itex]

No. :rolleyes: I don't think I've ever seen that.
 
Last edited:
hmm. I don't think you can do this question without using that rule, so I'm surprised you haven't seen it before. It is essentially an area integral using the cylindrical coordinate system (where the area is perpendicular to the z axis). You could also directly integrate using dxdy, but it would be much more complicated.

Anyway, if you use that rule (remember that r is inside the integral, along with the function), then you should get the right answer for lambda.
 

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