Chapter 3: Q14P (page 140)
For the infinite slot (Ex. 3.3), determine the charge density on
the strip at , assuming it is a conductor at constant potential .
Short Answer
Answer
The equation for the charge density on the strip at is .
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Chapter 3: Q14P (page 140)
For the infinite slot (Ex. 3.3), determine the charge density on
the strip at , assuming it is a conductor at constant potential .
Answer
The equation for the charge density on the strip at is .
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Buckminsterfullerine is a molecule of 60 carbon atoms arranged
like the stitching on a soccer-ball. It may be approximated as a conducting spherical shell of radius . A nearby electron would be attracted, according to Prob. 3.9, so it is not surprising that the ion exists. (Imagine that the electron on average-smears itself out uniformly over the surface.) But how about a second electron? At large distances it would be repelled by the ion, obviously, but at a certain distance r (from the center), the net force is zero, and closer than this it would be attracted. So an electron with enough energy to get in that close should bind.
(a) Find r, in . [You'll have to do it numerically.]
(b) How much energy (in electron volts) would it take to push an electron in (from
infinity) to the point r? [Incidentally, the ion has been observed.]
A spherical shell of radius R carries a uniform surface charge on the "northern" hemisphere and a uniform surface charge on the "southern "hemisphere. Find the potential inside and outside the sphere, calculating the coefficients explicitly up to and .
A uniform line charge is placed on an infinite straight wire, a distanced above a grounded conducting plane. (Let's say the wire runs parallel to the x-axis and directly above it, and the conducting plane is the plane.)
Find the force on the charge in Fig. 3.14. (The plane is a grounded conductor.)

In Section 3.1.4, I proved that the electrostatic potential at any point
in a charge-free region is equal to its average value over any spherical surface
(radius R )centered at .Here's an alternative argument that does not rely on Coulomb's law, only on Laplace's equation. We might as well set the origin at P .Let be the average; first show that
(note that the in da cancels the out front, so the only dependence on R
is in itself). Now use the divergence theorem, and conclude that if Vsatisfies
Laplace's equation, then,.
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