J2 all space (a) Positive charge Q is distributed uniformly over the surface of a thin spherical shell of radius i. ii. Find the electric field in all regions of space. Calculate the total potential energy of this charge distribution using the integral ab (b) Positive charge Q is distributed uniformly throughout the volume of a solid sphere of radiu: Find the electric field in all regions of space. i. ii. Calculate the total potential energy of this charge distribution using the integral ab (Note: "all regions of space" really does mean all regions. In both cases, you need to integrate the volumes inside and outside the sphere.)

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4. In Lecture 9 we saw that the energy density of an electric field is u = EE²/2. This "electric-field
energy" is not a new kind of energy; it is simply a different way of interpreting electric potential
energy. In particular, we can compute the total potential energy of a charge distribution from the
energy density. Previously we had calculated the total potential energy for a collection of point
charges (see slide 13 in Lecture 6), but now we can calculate it for continuous charge distributions.
The total potential energy of a charge distribution is the volume integral of the energy density over
all regions of space:
U =
s
2 €0E² dv
all
space
(a) Positive charge Q is distributed uniformly over the surface of a thin spherical shell of radius R.
Find the electric field in all regions of space.
i.
ii.
Calculate the total potential energy of this charge distribution using the integral above.
(b) Positive charge Q is distributed uniformly throughout the volume of a solid sphere of radius R.
Find the electric field in all regions of space.
i.
ii.
Calculate the total potential energy of this charge distribution using the integral above.
(Note: "all regions of space" really does mean all regions. In both cases, you need to integrate over
the volumes inside and outside the sphere.)
Transcribed Image Text:4. In Lecture 9 we saw that the energy density of an electric field is u = EE²/2. This "electric-field energy" is not a new kind of energy; it is simply a different way of interpreting electric potential energy. In particular, we can compute the total potential energy of a charge distribution from the energy density. Previously we had calculated the total potential energy for a collection of point charges (see slide 13 in Lecture 6), but now we can calculate it for continuous charge distributions. The total potential energy of a charge distribution is the volume integral of the energy density over all regions of space: U = s 2 €0E² dv all space (a) Positive charge Q is distributed uniformly over the surface of a thin spherical shell of radius R. Find the electric field in all regions of space. i. ii. Calculate the total potential energy of this charge distribution using the integral above. (b) Positive charge Q is distributed uniformly throughout the volume of a solid sphere of radius R. Find the electric field in all regions of space. i. ii. Calculate the total potential energy of this charge distribution using the integral above. (Note: "all regions of space" really does mean all regions. In both cases, you need to integrate over the volumes inside and outside the sphere.)
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