Chapter 9: Q9.3P (page 388)
Question: Use Eq. 9.19 to determineandin terms ofrole="math" localid="1653473428327" ,,, and.
Short Answer
The value of is role="math" localid="1653473609796" , and the value of is
Chapter 9: Q9.3P (page 388)
Question: Use Eq. 9.19 to determineandin terms ofrole="math" localid="1653473428327" ,,, and.
The value of is role="math" localid="1653473609796" , and the value of is
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(This is, incidentally, the simplest possible spherical wave. For notational convenience, let role="math" localid="1658817164296" in your calculations.)
(a) Show that obeys all four of Maxwell's equations, in vacuum, and find the associated magnetic field.
(b) Calculate the Poynting vector. Average over a full cycle to get the intensity vector . (Does it point in the expected direction? Does it fall off like, as it should?)
(c) Integrate role="math" localid="1658817283737" over a spherical surface to determine the total power radiated. [Answer: ]
(a) Show that the skin depth in a poor conductor is (independent of frequency). Find the skin depth (in meters) for (pure) water. (Use the static values of and ; your answers will be valid, then, only at relatively low frequencies.)
(b) Show that the skin depth in a good conductor is (where λ is the wavelength in the conductor). Find the skin depth (in nanometers) for a typical metal in the visible range , assuming and . Why are metals opaque?
(c) Show that in a good conductor the magnetic field lags the electric field by , and find the ratio of their amplitudes. For a numerical example, use the “typical metal” in part (b).
Question:Equation 9.36 describes the most general linearly polarized wave on a string. Linear (or "plane") polarization (so called because the displacement is parallel to a fixed vector n) results from the combination of horizontally and vertically polarized waves of the same phase (Eq. 9.39). If the two components are of equal amplitude, but out of phase by (say,,), the result is a circularly polarized wave. In that case:
(a) At a fixed point, show that the string moves in a circle about the axis. Does it go clockwise or counter clockwise, as you look down the axis toward the origin? How would you construct a wave circling the other way? (In optics, the clockwise case is called right circular polarization, and the counter clockwise, left circular polarization.)
(b) Sketch the string at time t =0.
(c) How would you shake the string in order to produce a circularly polarized wave?
(a) Suppose you imbedded some free charge in a piece of glass. About how long would it take for the charge to flow to the surface?
(b) Silver is an excellent conductor, but it’s expensive. Suppose you were designing a microwave experiment to operate at a frequency of. How thick would you make the silver coatings?
(c) Find the wavelength and propagation speed in copper for radio waves at role="math" localid="1655716459863" . Compare the corresponding values in air (or vacuum).
The "inversion theorem" for Fourier transforms states that
Use this to determine , in Eq. 9.20, in terms of and
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