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Light from an aquarium goes from water (n=43)through a plane of glass (n=32)into the air (n=1). Assuming its a monochromatic plane wave and that it strikes the glass at normal incidence, find the minimum and maximum transmission coefficients (Eq. 9.199). You can see the fish clearly; how well can it see you?

Short Answer

Expert verified

The minimum and maximum transmisssion coefficients are Tmin=0.93455andTmax=0.987959 respectively, and it is clearly seen that fish sees you just as well as you see it.

Step by step solution

01

Given information:

Given data:

The refractive index of water isn1=43.

The refractive index of glass isn2=32.

The refractive index of air isn3=1.

02

Determine the minimum and maximum transmission coefficients

Write the expression for the inversion of the transmission coefficient.

T-1=14n1n3[n1+n32+n12-n22n32-n22n22sin2n2ωdC]

Substitute n1=43, n2=32and n3=1in the above expression.

T-1=14431432+1+432-322r2-322322sin23ωd2CT-1=316499+1736×54×49sin23ωd2CT-1=4948+854836sin23ωd2C........(1)

For transmission coefficient to be minimum data-custom-editor="chemistry" sin23ωd2C=1.

Substitute data-custom-editor="chemistry" sin23ωd2C=1in equation (1).

data-custom-editor="chemistry" Tmin=4849+8536Tmin=0.93455

For transmission coefficient to be maximumdata-custom-editor="chemistry" sin23ωd2C=0.

Substitute data-custom-editor="chemistry" sin23ωd2C=0in equation (1).

Tmax=4849Tmax=0.987959

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Most popular questions from this chapter

(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 of1010Hz. 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" 1MHz. Compare the corresponding values in air (or vacuum).

(a) Show directly that Eqs. 9.197 satisfy Maxwell’s equations (Eq. 9.177) and the boundary conditions (Eq. 9.175).

(b) Find the charge density, λ(z,t), and the current, I(z,t), on the inner conductor.

Suppose you send an incident wave of specified shape, g1(z-v1t), down string number 1. It gives rise to a reflected wave, hR(z+v1t), and a transmitted wave, gT(z+v2t). By imposing the boundary conditions 9.26 and 9.27, find hRand gT.

[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 traveling through vacuum in the z direction encounters a perfect conductor occupying the region z0, and reflects back:

E(z,t)=E0[cos(kz-ωt)-cos(kz+ωt)]x^,(z>0),

(a) Find the accompanying magnetic field (in the region role="math" localid="1657454664985" (z>0).

(b) Assuming inside the conductor, find the current K on the surface z=0, by invoking the appropriate boundary condition.

(c) Find the magnetic force per unit area on the surface, and compare its time average with the expected radiation pressure (Eq. 9.64).

Question: Obtain Eq. 9.20 directly from the wave equation by separation of variables.

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