[试题] 108-1 朱国瑞 古典电力学一 期末考

楼主: TunaVentw (dB9)   2020-09-26 14:25:37
课程名称︰古典电力学一
课程性质︰物理系系定选修
课程教师︰朱国瑞
开课学院:理学院
开课系所︰物理学系
考试日期(年月日)︰2020年01月06日
考试时限(分钟):110分钟
是否需发放奖励金:是
(如未明确表示,则不予发放
试题 :
Electrodynamics (I), Final Exam (6 problems) 1/6/2020
Note:(1) You may use Jackson. Any other materials (such as lecture notes, dic-
tionary, calculator, cell phone, and insertions of any kind) are NOT
allowed.
(2) You may use any eq. in Jackson without derivation unless you are
asked to derive it.
(3) Notationsm equation no, and page no follow Jackson.
1. Answer the following questions about Faraday's law:
∮\vec{E}‧d\vec{l}=-∫_s(∂\vec{B}/∂t)‧\vec{n}da
(a) If loop C is a closed wire with σ=∞ (hence \vec{E}=0 in the wire).
Then, ∮\vec{E}‧d\vec{l}=0 at all times even if a time-varying magnetic
flux is applied through the loop. Explain how this is possible. (4%)
(b) Consider a σ=∞ wire with a gap with end points a and b (see figure).
Let \vec{B}(\vec{x},t) be a known external field. What is the value of
∫^b_a\vec{E}‧d\vec{l}? (4%) ∫^b_a\vec{E}‧d\vec{l} depeneds on the
path from a to b. Why? (4%_
(c) Consider Case (b) again. If a point charge q (with negligible self fiels
) moves from a to b along the same path as in Case (b), the work done by
E on q is not equal to q times the ∫^b_a\vec{E}‧d\vec{l} in case (b).
Why? (4%)
╭──────────╮b
│\vec{B}(\vec{x},t)

╰──────────╯a
2. Inside a linear and uniform dielectric medium of permiitivity ε, there are
static free charge density [ρ_free(\vec{x})] and polarization charge dens-
ity [ρ_pol(\vec{x})].
(a) Show ρ_net/ε_0 = ρ_free/ε, where ρ_net = ρ_free + ρ_pol and ε_0
is the permittivity of free space. (4%)
(b) If ρ_free is a point charge given by ρ_free = qδ(\vec{x}-\vec{x_0}),
find ρ_pol. (4%)
(c) Discuss the physical implication of the result in (b) if ε>ε_0. (4%)
3. (a) Assume \vec{J}(t) = Re[\vec{J}_0e^{-iωt}] and \vec{E}(t) = Re[\vec{E}_0
e^{-iωt} ], where \vec{J}_0 and \vec{E}_0 are complex constants and ω
is a real constant. Show that the time-averaged value of \vec{J}(t)‧
\vec{E}(t) over one period is given by 1/2Re[\vec{J}_0\vec{E}^*_0]. (6%)
(b) Assume ε=ε'+iε'' is a complex number. Show Re√ε‧Im√ε = 1/2ε''.
(6%)
[Hint: Let ε(a+ib)^2]
4. A conducting surface has a static surface charge density σ. For simplicity,
assume that tje surface is flat. Use the Maxwell stress tensor [Jackson Eqs
(6.120) and (6.122)] to show that the force per unit area on the conducting
surface is σ^2/(2ε_0). (20%)
5. It's algebraically clear from observing (7.51) that we may neglect collisi-
ons and binding forces under the conditions ω>>γ_j and ω>>ω_j. As in the
lecture notes, do some simple calculations starting from (7.49) to find the
physical interpretations of these algebraic observations. (20%)
6. A plane wave of frequency ω and propagation constant k is propagating in
the +z direction in a uniform conducting medium characterized by a real
permeability μ and a complex permittivity: ε = ε_b + iσ/ω. Assume ε_b,
σ, and ω are all real.
(a) Write down the dispersion relation of the plane wave in terms of μ, ε,
k, and ω. (4%)
(b) Under what criterion is the medium a good conductor? Write it in terms
of ε_b, σ, and ω? (4%)
(c) Derive the skin depth (δ) of a good conductor in terms of σ, μ,and
ω. (4%)
(d) If E(z=0)=E_0, what is E(z) in terms of E_0, z, and δ? (4%)
(e) Calculate the Ohmic power/unit volume deposited into the medium by the
plane wave in terms of |E_0|, z, σ, and δ. (4%)

Links booklink

Contact Us: admin [ a t ] ucptt.com