Charged Sphere with off-center cavity Electric field

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SUMMARY

The discussion focuses on calculating the total charge and dipole moment of a uniformly charged sphere with an off-center cavity. The total charge is determined to be (4/3)πρ(a³ - b³), where ρ is the charge density, a is the radius of the sphere, and b is the radius of the cavity. The dipole moment is calculated as p = (4/3)πρb³d, where d is the distance between the centers of the sphere and the cavity. The superposition principle is applied to find the electric field inside the cavity, which combines the fields from both the large sphere and the small cavity. The discussion also emphasizes the importance of coordinate systems in these calculations.

PREREQUISITES
  • Understanding of electrostatics and charge distributions
  • Familiarity with the superposition principle in electric fields
  • Knowledge of dipole moments and their calculations
  • Proficiency in using spherical coordinates for electric field calculations
NEXT STEPS
  • Study the concept of electric fields due to spherical charge distributions
  • Learn about the superposition principle in electrostatics
  • Explore dipole moments and their effects on electric fields
  • Investigate coordinate systems in electrostatics for complex geometries
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This discussion is beneficial for physics students, particularly those studying electrostatics, as well as educators looking for examples of charge distribution problems and their solutions.

EnderTheGreat
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Homework Statement


Consider a sphere uniformly charged over volume, apart from a spherical
off-center cavity. The charge density is ρ, radius of the sphere is a, radius of the cavity is
b, and the distance between the centers is d, d < a-b. (a) Find the total charge and the
dipole moment (with respect to the center of the large sphere) of this configuration. (b) Use
superposition principle to find the electric field inside the cavity. (c) Show that far from the
sphere the field is that of a charge plus dipole correction. Check that the charge and the
dipole moment correspond to that of part (a).


Homework Equations


ρ=Q/V
p=Ʃq_i(r_i-r)
E_sphere=Qr/4piεR^2 for r<R
superposition principle


The Attempt at a Solution


total charge I'm fairly certain is (4/3)piρ(a^3-b^3) just the large sphere minus the cavity.
The dipole moment i attempted to use a sum p=q_a(0-0)+q_b(d-0) and got

p=(4/3)pi*ρ*b^3*d (from the center of the cavity towards the center of the large sphere)

for b) I tried to find the Electric field due to the large sphere ((4/3)piρa^3)*(r/4piεa^2) and the field from the small sphere ((4/3)piρb^3)*(r/4piεb^2) but I am not sure what coordinate system i should be using, nor how to superimpose/sum the fields correctly.

c) We were not taught nor can i find anything in the book about a dipole correction, so I'm lost for this part.

(I wasnt sure if this should go in Advanced or Introductory physics, so it is in both, I will remove the other as soon as one is replied too, sorry)
 
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You can consider the hollow sphere as a full one + a small sphere with opposite charge, so you get zero charge inside the cavity. You can direct your system of coordinates any way, choose the most convenient: the centres of the spheres line up along one coordinate axis.
According to this model, the dipole moment is the same as that of a point charge q at distance d from the centre of the big sphere. Take care with the sign: The dipole moment points from the negative charge to the positive one.
The electric field of the hollow sphere is the sum of the full sphere + the small oppositely charged sphere at the place of the cavity. Check your work: The electric field at distance r depends on the charge enclosed in the sphere of radius r. If r<b the enclosed charge is less than the total charge of the sphere.

ehild
 

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