Chapter 29: Problem 12
Electromagnetic waves don't readily penetrate metals. Why not?
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These are the key concepts you need to understand to accurately answer the question.
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Chapter 29: Problem 12
Electromagnetic waves don't readily penetrate metals. Why not?
These are the key concepts you need to understand to accurately answer the question.
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You're engineering a new cell phone, and you'd like to incorporate the antenna entirely within the phone, which is \(9 \mathrm{cm}\) long when closed. The antenna is to be a quarter-wavelength long-a common design for vertically oriented antennas. If the cell-phone frequency is \(2.4 \mathrm{GHz}\), will the antenna fit?
Lasers are classified according to the eye-damage danger they pose. Class 2 lasers, including many laser pointers, produce visible light with no greater than 1 mW total power. They're relatively safe because the eye's blink reflex limits exposure time to 250 ms. Find (a) the intensity of a 1 -m \(\mathrm{W}\) class 2 laser with beam diameter \(1.0 \mathrm{mm},\) (b) the total energy delivered before the blink reflex shuts the eye, and (c) the peak electric field in the laser beam.
You're an astronomer studying the origin of the solar system, and you're evaluating a hypothesis that sufficiently small particles were blown out of the solar system by the force of sunlight. To see how small such particles must be, compare the force of sunlight with the force of solar gravity, and solve for the particle radius at which the two are equal. Assume spherical particles with density \(2 \mathrm{g} / \mathrm{cm}^{3} .\) (Note: Distance from the Sun doesn't matter. Why not?)
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The fields of an electromagnetic wave are \(\vec{E}=E_{p} \sin (k z+\omega t) \hat{\jmath}\) and \(\vec{B}=B_{p} \sin (k z+\omega t) \hat{\imath} .\) Give a unit vector in the wave's propagation direction.
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