Chapter 4: Q4.7P (page 172)
Show that the energy of an ideal dipole p in an electric field E isgiven by
Short Answer
Thepotential energy for the dipole moment is .
Chapter 4: Q4.7P (page 172)
Show that the energy of an ideal dipole p in an electric field E isgiven by
Thepotential energy for the dipole moment is .
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Get started for freeAccording to quantum mechanics, the electron cloud for a hydrogen
atom in the ground state has a charge density
where qis the charge of the electron and ais the Bohr radius. Find the atomic
polarizability of such an atom. [Hint:First calculate the electric field of the electron cloud, then expand the exponential, assuming .
For the bar electret of Prob. 4.11, make three careful sketches: one
of P, one of E, and one of D. Assume L is about 2a. [Hint: E lines terminate on
charges; D lines terminate on free charges.]
A very long cylinder, of radius a, carries a uniform polarization P perpendicular to its axis. Find the electric field inside the cylinder. Show that the field outside the cylinder can be expressed in the form
[Careful: I said "uniform," not "radial"!]
Find the field inside a sphere of linear dielectric material in an otherwise uniform electric field (Ex. 4.7) by the following method of successive approximations: First pretend the field inside is just , and use Eq. 4.30 to write down the resulting polarization . This polarization generates a field of its own, (Ex. 4.2), which in turn modifies the polarization by an amount . which further changes the field by an amount , and so on. The resulting field is . Sum the series, and compare your answer with Eq. 4.49.
A conducting sphere of radius a, at potential , is surrounded by a
thin concentric spherical shell of radius b,over which someone has glued a surface charge
,
where k is a constant and is the usual spherical coordinate.
a) Find the potential in each region: (i) r>b, and (ii) a<r<b.
b) Find the induced surface charge on the conductor.
c) What is the total charge of this system? Check that your answer is consistent with the behavior of V at large.
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