Finding Constant A for Independent Electric Field between Two Spheres

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SUMMARY

The discussion focuses on determining the constant A for an electric field that remains independent of radius r between two spheres, with the inner sphere having radius a and the outer sphere radius b. The problem involves a charge density of A/r and a central charge Q. The solution requires using Gauss' law to calculate the electric field and setting the electric fields at the boundaries (r = a and r = b) equal to each other to solve for A. A critical point made is the necessity of correctly evaluating the volume integral for the charge distribution.

PREREQUISITES
  • Understanding of Gauss' law in electrostatics
  • Familiarity with spherical coordinates and volume integrals
  • Knowledge of electric field concepts and calculations
  • Ability to solve equations involving electric fields and charge distributions
NEXT STEPS
  • Review the application of Gauss' law in electrostatics
  • Study spherical coordinates and their use in volume integrals
  • Learn how to derive electric fields from charge distributions
  • Practice solving for constants in electric field equations
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Students studying electromagnetism, physicists working with electrostatic problems, and educators teaching concepts related to electric fields and charge distributions.

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Homework Statement


We have a sphere with radius b, within that sphere there's another sphere with radius a. Between the two spheres we have an electric charge with density A/r. Also, we have a charge Q in the center. We need to find the constant A so that the field between a and b is independent of r (meaning, it's constant for a<=r<=b).


Homework Equations


Gauss' law.



The Attempt at a Solution


I added the scanned pages I've written, it should be understandable. As I said, I used Gauss' law to calculate the field, using a sphere with radius r (a<=r<=b) to calculate the electric flux. After finding the electric field as a function of r, I calculated d(E(r))/dr and demanded that it would be=0, but I can't seem to get a solution for A that's independent of r.
 

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In your work, you had

[tex]Qin = \frac{A}{r} \left[ \frac{4}{3}\pi r^3 - \frac{4}{3}\pi a^3 \right] + Q[/tex]

That's not right. You're going to need to re-evaluate the volume integral. The [tex](4/3)\pi r^3[/tex] terms only makes sense if the charge distribution is uniformly distributed about the sphere. You can't just multiply them by A/r. It doesn't work that way. You'll have to re-do the volume integral, integrating A/r' from r' = a to r in spherical coordinates (be careful to use the correct volume differential when performing the integral -- it's not simply dr') .

Once you have an expression for the electric field, E, don't worry about taking the derivative. Instead, find the electric field at r = a, and call that Ea. Then find Eb, the electric field at r = b. Set Ea and Eb equal to each other and solve for A.
 
collinsmark said:
In your work, you had

[tex]Qin = \frac{A}{r} \left[ \frac{4}{3}\pi r^3 - \frac{4}{3}\pi a^3 \right] + Q[/tex]

That's not right. You're going to need to re-evaluate the volume integral. The [tex](4/3)\pi r^3[/tex] terms only makes sense if the charge distribution is uniformly distributed about the sphere. You can't just multiply them by A/r. It doesn't work that way. You'll have to re-do the volume integral, integrating A/r' from r' = a to r in spherical coordinates (be careful to use the correct volume differential when performing the integral -- it's not simply dr') .

Once you have an expression for the electric field, E, don't worry about taking the derivative. Instead, find the electric field at r = a, and call that Ea. Then find Eb, the electric field at r = b. Set Ea and Eb equal to each other and solve for A.

How did I not notice that..thanks, that solved it.
 

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