Electric field of a point charge inside a sphere

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SUMMARY

The discussion focuses on calculating the electric field of a point charge located inside a sphere with a non-uniform charge density defined by ρ(r) = ρ0(r4/R4). The first part involves determining the charge Q(r) within a radius r < R using Gauss's law, leading to the derivation of the radial electric field Er(r). The second part addresses the addition of a point charge Q at position vector R0 = (1, 1, 1) and calculating the resultant electric field E(r) at point P = (1, 2, 1) by applying the superposition principle.

PREREQUISITES
  • Understanding of Gauss's law in both integral and differential forms.
  • Familiarity with electric field calculations for point charges and continuous charge distributions.
  • Knowledge of vector calculus, particularly divergence and gradient operations.
  • Basic principles of electrostatics, including charge density and electric field superposition.
NEXT STEPS
  • Study the application of Gauss's law for various charge distributions.
  • Learn about electric field calculations using the superposition principle in electrostatics.
  • Explore vector calculus techniques relevant to electromagnetism, particularly divergence.
  • Investigate the effects of non-uniform charge distributions on electric fields.
USEFUL FOR

Students and professionals in physics, particularly those focusing on electromagnetism, electrostatics, and vector calculus applications in electric field analysis.

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Homework Statement



(a)Consider a charged sphere of radius R centred at the origin with the spherically symmetric charge density ρ(r) = ρ0(r4/R4) where ρ0 is a constant and r is the radial coordinate.
Find the charge dQ0 contained in a spherical shell of radius r0 < R and infinitesimal thickness dr0.
Hence find the charge Q(r) contained inside the sphere as a function of
r < R.
Using Gauss’s law in integral form, determine the magnitude of the radial electric field Er(r) inside the sphere as a function of r < R.
Using the fact that \underline{∇}\cdotE(r) = \frac{1}{r^2}\frac{∂}{∂r}(r2Er(r)) in this case, verify Gauss’s law in
differential form at a general point inside the sphere.

(b) A positive point charge Q is added to a point P0 with position vector R0 with components (1, 1, 1) inside a sphere with the same charge density as in part
(a) apart from the charge Q. Calculate the vector electric field E(r) at a point
P with position vector r with components (1, 2, 1) inside the sphere in terms
of the unit vectors \widehat{x}, \widehat{y}, \widehat{z} and Q and Er (considered in part (a)).

Homework Equations





The Attempt at a Solution


i have done part b of the question already. i am just not quite sure how to deal with a point charge inside a sphere with charge density. Do i just add up the two field?
 
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Superposition principle.
 

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