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The directions and three problems from examination 3 of university of california, berkeley's physics 110b spring 2004 course. The problems cover topics such as complex fields, reflection amplitude ratio, jones matrix, state of polarization, electrostatic multipole moments, and radiation emission. Students are expected to use the given equations and boundary conditions to calculate answers and justify their work.
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University of California, Berkeley Physics 110B Spring 2004 (Strovink)
EXAMINATION 3
Directions: Do all three problems, which have unequal weight. This is a closed-book closed-note examexcept for Griffiths, Pedrotti, a copy of anything posted on the course web site, and anything in your own original handwriting (not Xeroxed). Calculators are not needed, but you may use one if you wish. Laptops and palmtops should be turned off. Use a bluebook. Do not use scratch paper – otherwise you risk losing part credit. Show all your work. Cross out rather than erase any work that you wish the grader to ignore. Justify what you do. Express your answer in terms of the quantities specified in the problem. Box or circle your answer.
Problem 1. (30 points) In a medium with (fixed) conductivity σ, the ratio of complex fields H/˜ E˜ is given by the complex admittance
μ
{[ √1 + β (^2) + 1 2
[ √1 + β (^2) − 1 2
where β ≡ (^) ωσ , and the (fixed) dielectric constant and the (fixed) magnetic permeability μ are due to the effects of bound electrons.
At normal incidence at the interface between two dissimilar materials 1 and 2, the (complex) electric field amplitude reflected back into ma- terial 1 is expressed as a (complex) ratio R˜ to the (complex) incident amplitude. By matching boundary conditions for the electric and mag- netic fields, R˜ is routinely found to be given by the standard result
Consider the case in which material 1 is an insu- lator (β = 0) and material 2 is a poor conductor (β 1), with
1 /μ 1 =
2 /μ 2. Calculate the
reflection amplitude ratio R˜ to lowest nonvan- ishing order in β.
Problem 2. (35 points) An ideal wave plate of thickness D with phase retardation difference
δ ≡ (ns − nf )
ωD c
having its slow (ns) axis along the direction (ˆx cos φ + ˆy sin φ), is represented by the Jones matrix
MW(φ) = ( cos δ 2 + i sin 2 δ cos 2φ i sin δ 2 sin 2φ i sin δ 2 sin 2φ cos δ 2 − i sin δ 2 cos 2φ
A beamof light traveling in the ˆz direction passes through a device that consists of the following ideal components:
(a.) (10 points) Calculate the Jones matrix that represents the effect of this device.
(b.) (15 points) Given that a beamis observed to emerge from this device, calculate its state of polarization.
(c.) (10 points) The Mueller matrix for this device is
1 2
Assume that the incident beam is natural light (100% unpolarized, 〈|Ex|^2 〉 = 〈|Ey |^2 〉). Calcu- late the fraction I′/I 0 of the incident irradiance that this device transmits.
Problem 3. (30 points) At t = 0, charge +e lies at (x, y, z) = (0, 0 , b/2) and charge −e lies at (x, y, z) = (0, 0 , −b/2).
(a.) (10 points) Identify the lowest-l nonvanishing electrostatic multipole moment(s) of the charge distribution (you don’t need to calculate its (their) magni- tude).
(b.) (5 points) The static charge distribution in (a.) now is set into oscillation: as time advances, the position vector of each charge is multiplied by the same factor 1 + cos ωt, where ω and 0 < 1 are real constants. Using the fact that a static elec- tric multipole corresponding to a given l and m, when caused to oscillate, yields E-type (TM) multipole radiation of the same l and m, what type(s) of lowest-l radiation (e.g. E2 1 ) is (are) emitted?
(c.) (15 points) For E-type (TM) radiation of type Elm, the mag-
netic field B˜ (⊥ rˆ) is proportional to the vector
spherical harmonic Xlm:
B˜ ∝ X lm(θ, φ)^ ≡^ L Ylm(θ, φ)^.
Also, in the far zone,
E^ ˜ ≈ cB˜ × ˆr.
Finally, in spherical polar coordinates,
iL ≡ r × ∇ = φ ˆ
∂θ
θˆ sin θ
∂φ
Write down a function f (θ, φ) such that the an- gular distribution of the radiated power P in the far zone b (^2) ωπc r is proportional to it:
dP dΩ
∝ f (θ, φ).