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
All the tools & learning materials you need for study success - in one app.
Get started for freeA microwave antenna radiating at 10GHz is to be protected from the environment by a plastic shield of dielectric constant 2.5. What is the minimum thickness of this shielding that will allow perfect transmission (assuming normal incidence)? [Hint: Use Eq. 9. 199.]
Question: Show that the standing wave satisfies the wave equation, and express it as the sum of a wave traveling to the left and a wave traveling to the right (Eq. 9.6).
(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 intensity of sunlight hitting the earth is about . If sunlight strikes a perfect absorber, what pressure does it exert? How about a perfect reflector? What fraction of atmospheric pressure does this amount to?
[The naive explanation for the pressure of light offered in section 9.2.3 has its flaws, as you discovered if you worked Problem 9.11. Here's another account, due originally to Planck.] A plane wave travelling through vaccum in the z direction encounters a perfect conductor occupying the region , and reflects back:
What do you think about this solution?
We value your feedback to improve our textbook solutions.