Electricity and magnetism (Gauss' law)

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SUMMARY

The discussion centers on applying Gauss' Law to calculate the electric field and potential of two spherical shells with radii r1 and r2, where r2 > r1. The inner shell carries a uniform charge Q1, while the outer shell has charge Q2. The electric field E is derived as E = KQ1 r1 / r2^3, and the potential V is expressed as V = (9 x 10^9 Nm^2/c^2)(Q1/r1 + Q2/r2). Participants emphasize the need to consider different domains for the electric field and correct the initial misunderstanding regarding the "volume ratio" concept.

PREREQUISITES
  • Understanding of Gauss' Law and its application to spherical symmetry.
  • Familiarity with electric fields and potentials in electrostatics.
  • Knowledge of charge distributions and their effects on electric fields.
  • Basic algebra and calculus for manipulating equations involving electric fields and potentials.
NEXT STEPS
  • Study the derivation of electric fields using Gauss' Law in different geometries.
  • Explore the concept of electric potential and its calculation for various charge distributions.
  • Learn about the implications of charge density and its effect on electric fields.
  • Investigate the differences in electric field behavior in regions inside and outside charged conductors.
USEFUL FOR

Students preparing for exams in electromagnetism, physics educators, and anyone interested in mastering the concepts of electric fields and potentials in electrostatics.

Silentwhale
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Homework Statement


Given two things spherical shells radii r1 and r2 with r2 > r1.
The inner she'll is charged uniformly with a total charge Q1, while the outer shell with Q2.

A) use gauss law to computer the electric field everywhere
B) Use any method to calculate the potential everywhere.

Homework Equations

The Attempt at a Solution


I will be attempting this problem soon just wanted to post the question so I wouldn't waste time it is for my midterm practice. Thank you. I will post my trial solution when I am done trying this problem. Thank you
 
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OK so here is my attempt to the problem:

A) EA = (Qin/ε) (volume ratio)

E (
4(pi)r1^2) = (Q1/ ε) ((4/3 pi r1^3)/(4/3 pi r2^3))

E (
4 pi r1^2) = Q1 r1^3 / ε r2^2

E=
Q1 r1^3 / ε r2^3 4pi r1^2

E
= Q1 r1 / 4pi ε r2^3

E
= KQ1 r1 / r2^3 final answer for a

B)
v= kQ1/r1 + kQ2/r2

V
= (9 x 10^9 Nm^2/ c^2)(Q1/r1 + Q2/r2) answer part b
 
Silentwhale said:
A) EA = (Qin/ε) (volume ratio)

Volume ratio? You have a typo in your post, but I believe what you intended to type was “thin shell”. Your “volume ratio” suggests you are considering these to be uniform charge densities. Also, even if that were the case, the electric field will have different functional forms over different domains of radius. You have to find a separate answer for each domain.
 
I do not understand where A) came from. What is this volume ratio? As pointed out in post #3, you are asked to find the electric field everywhere, so first take the case where you want the electric field somewhere inside the inner sphere. Write down the law of physics that you are going to use to solve the problem and aply that law.
 

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