A thin wire of radius b is used to form a circular wire loop of radius a (a
>> b) and total resistance R.
The loop is rotating about the z-axis with constant angular velocity ωk
in a region with constant magnetic field B = B0i.
At t = 0 the loop lies in the y-z plane and the points A and P cross the y-axis.
Find the potential difference between points A and P as a function of time.
A thin wire of radius b is used to form a circular wire loop of radius a (a
>> b) and total resistance R.
The loop is rotating about the z-axis with constant angular velocity ωk
in a region with constant magnetic field B = B0i.
At t = 0 the loop lies in the y-z plane and the point A at the center of the
wire crosses the y-axis.
Let the (θ/θ) direction be tangential to the loop and be equal to the
positive z direction at point A.
Let the (φ/φ) direction be tangential to the wire and be equal to the
direction indicated in the figure.
(a) Find the current flowing in the loop. Neglect the
self-inductance of the loop. What is current density J as a
function of time?
(b) Find the thermal energy generated per unit time, averaged over one
revolution.
(c) Write down an expression for the the Poynting vector
S on the
surface of the wire.
(d) Use S to find the field energy per unit time flowing into the
wire, averaged over one revolution.
(a) From Maxwell's equations, derive the conservation of energy
equation,
(∂u/∂t) + ∇∙S
= -E∙j,
where u is the energy density
and S is the Poynting vector. Rewrite this equation in integral form and
explain why it is a statement of energy conservation.
(b) A long, cylindrical conductor of radius a and conductivity
σ carries a constant current I. Find S at the
surface of the cylinder and interpret your result in terms of conservation of
energy.
Show that a radially oscillating spherically symmetric charge distribution does
not radiate.
Assume a harmonic time variation of frequency ω
and use the complex formalism,
namely ρ(r,t) = Re[ρ(r)exp(-iωt)], D(r,t) = Re[D(r)exp(-iωt)], and so forth.
(a) First
write down
Maxwell's equations and the continuity equation using the complex formalism to eliminate
time derivatives.
(b) Note that one can write j(r) = rf(r). Compare
∇∙D and ∇∙j
to relate D and j.
(c) Show that ∫ρ(r) d3r = 0.
(d) What are D and B outside the source? (Hint: Consider
∇∙B and ∇×B.)
(e) What do you conclude concerning radial oscillations of a spherically symmetric
source with an arbitrary time variation?
(a) Write down the set of Maxwell's equations in the form that applies
to static fields.
(b) Use the continuity equation to adapt Maxwell's
∇×B equation to dynamic
fields. (This can be done by using a term that Maxwell referred to as
"displacement current".)
(c) Write down the dynamical form of Maxwell's equations.
(d) Introduce the vector and scalar potentials and show that this leads to
two wave equations in these potentials. (The Lorentz gauge may be used to
answer this part.)
(e) Define the Coulomb gauge and elaborate on some Coulomb gauge details.