A point charge qis at the center of an uncharged spherical conducting

shell, of inner radius aand outer radius b. Question:How much work would it take to move the charge out to infinity (through a tiny hole drilled in the shell)?

Short Answer

Expert verified

The work done to movea point charge qat the center of an uncharged spherical conducting shell of inner radius aand outer radius bto infinity is q28πε01a-1b.

Step by step solution

01

Given data

A point charge qis at the center of an uncharged spherical conducting

shell, of inner radius aand outer radius b.

02

Work done to spread charge  -q on a sphere of radius  r with another charge q  at the center

W=-18ττε0q2r.......(1)

Here, ε0is the permittivity of free space.

03

Work done to remove center charge

A point charge qinduces -q charge at the inner surface and +q charge on the outer surface of the conducting spherical shell.

Work done to bring the point charge with nothing else nearby is

W1=0

From equation (1), work done to bring the inner spherical shell with -qand radius a is

role="math" localid="1657520476370" W2=-18πε0q2a

From equation (1), work done to bring the inner spherical shell with -qand radiusb is
W3=-18πε0q2b

Thus, the net initial charge is

Wi=W1+W2+W3

Substitute the values in the above equation and get

Wi=0-18πε0q2a+18πε0q2b=q28πε01a-1b

This is the initial energy of the configuration. After the point charge is removed, the spherical shell becomes neutral and thus the final energy of the configuration is zero. Hence, the work done to remove the charge is

W=0-Wi

=q28πε01a-1b

Thus, the work done to remove the point charge is =q28πε01a-1b.

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Most popular questions from this chapter

A long coaxial cable (Fig. 2.26) carries a uniform volume charge density pon the inner cylinder (radius a ), and a uniform surface charge density on the outer cylindrical shell (radius b ). Thissurface charge is negative and is of just the right magnitude that the cable as a whole is electrically neutral. Find the electric field in each of the three regions: (i) inside the inner cylinder(s<a),(ii) between the cylinders(a<s<b)(iii) outside the cable(s>b)Plot lEI as a function of s.

Find the potential on the rim of a uniformly charged disk (radius R002C

charge density u).

We know that the charge on a conductor goes to the surface, but just

how it distributes itself there is not easy to determine. One famous example in which the surface charge density can be calculated explicitly is the ellipsoid:

x2a2+y2b2+z2c2=1

In this case15

σ=Q4πabc(x2a4+y2b4+z2c4)-1/2

(2.57) where Q is the total charge. By choosing appropriate values for a , b and c. obtain (from Eq. 2.57):

(a) the net (both sides) surface charge density a(r) on a circular disk of radius R; (b) the net surface charge density a(x) on an infinite conducting "ribbon" in the xy plane, which straddles they axis from x = - a to x = a (let A be the total charge per unit length of ribbon);

(c) the net charge per unit length λ(x)on a conducting "needle," running from x = - a to x = a. In each case, sketch the graph of your result.

Suppose the electric field in some region is found to beE=Kr3r^

in spherical coordinates (kis some constant).

(a) Find the charge density role="math" localid="1654330395426" P

(b) Find the total charge contained in a sphere of radius Rcentered at the origin.(Do it two different ways.)

Calculate×Edirectly from Eq. 2.8, by the method of Sect. 2.2.2. Refer to Prob. 1.63 if you get stuck.

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