Chapter 9: 9.33P (page 432)
The "inversion theorem" for Fourier transforms states that
Use this to determine , in Eq. 9.20, in terms of and
Short Answer
The expression for is
Chapter 9: 9.33P (page 432)
The "inversion theorem" for Fourier transforms states that
Use this to determine , in Eq. 9.20, in terms of and
The expression for is
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Get started for freeIn writing Eqs. 9.76 and 9.77, I tacitly assumed that the reflected and transmitted waves have the same polarization as the incident wave—along the x direction. Prove that this must be so. [Hint: Let the polarization vectors of the transmitted and reflected waves be
prove from the boundary conditions that .]
Question:The index of refraction of diamond is 2.42. Construct the graph analogous to Fig. 9.16 for the air/diamond interface. (Assume .) In particular, calculate (a) the amplitudes at normal incidence, (b) Brewster's angle, and (c) the "crossover" angle, at which the reflected and transmitted amplitudes are equal.
Find the width of the anomalous dispersion region for the case of a single resonance at frequency . Assume . Show that the index of refraction assumes its maximum and minimum values at points where the absorption coefficient is at half-maximum.
Consider the resonant cavity produced by closing off the two ends of a rectangular wave guide, at and at , making a perfectly conducting empty box. Show that the resonant frequencies for both TE and TM modes are given by
(9.204)
For integers l, m, and n. Find the associated electric and magneticfields.
Consider a particle of charge q and mass m, free to move in the plane in response to an electromagnetic wave propagating in the z direction (Eq. 9.48—might as well set ).
(a) Ignoring the magnetic force, find the velocity of the particle, as a function of time. (Assume the average velocity is zero.)
(b) Now calculate the resulting magnetic force on the particle.
(c) Show that the (time) average magnetic force is zero.
The problem with this naive model for the pressure of light is that the velocity is out of phase with the fields. For energy to be absorbed there’s got to be some resistance to the motion of the charges. Suppose we include a force of the form , for some damping constant .
(d) Repeat part (a) (ignore the exponentially damped transient). Repeat part (b), and find the average magnetic force on the particle.
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