As light moves from air (n 1.00) to amber it deviates 18o from its 45o angle of
incidence. Which way does it bend? What is the speed of light in amber?
Light entering a denser medium refracts towards the normal. Thus the angle of refraction is θt = 45 - 18 = 27o
. Using Snell's Law we have nt = 1.56
The speed in amber is given by v = c/n = 3.0×108/1.56 1.92×108
m/s or 0.64c
A transparent fiber of index of refraction 1.6 is surrounded (cladded) by a less dense plastic of index
1.5. At what angle must a light ray in the fiber approach the interface so as to remain within the fiber?
This problem involves total internal reflection. The critical angle for staying within the fiber is given by:
sinθc = = 1.5/1.6 = 0.938
. Thus θc = 69.6o
. The ray must
approach the interface between the media at an angle of 69.6o
or greater to the normal.
A light ray in air approaches a water surface (n 1.33) such that its electric vector is parallel to the
plane of incidence. If θi = 53.06o, what is the relative amplitude of the reflected beam? What
about if the electric field is perpendicular to the plane of incidence?
We can apply the Fresnel Equations. In the first case we want the expression for r ||
Snell's Law we can deduce that sinθt = (ni/nt)sinθi
which implies θt = 36.94o
|r || = 0||
In the latter (perpendicular) case we have
|râä¥ = = - 0.278||
In the former case, no light is reflected -- this is called Brewster's angle as we shall see in the
section on polarization. For the perpendicular field the amplitude of the reflected wave is
as large as the incident wave. That is the reflected ray is about (0.278)2 0.08
, or about
8% as bright as the incident ray (irradiance is proportional to the square of the amplitude).
By what angle do blue light (λb = 460 nm) and red light (λr = 680 nm) disperse upon entering
(from vacuum) a medium with N = 7×1038, ε = 1.94, and σ0 = 5.4×1015 Hz at
an incident angle of 20o (the electron charge is 1.6×10-19 Coulombs and its mass is 9.11×10-31 kilograms)?
First we must calculate the index of refraction for both light frequencies. The angular frequency
of the blue light is σb = 4.10×1015
Hz and for the red light σr = 2.77×1015
Thus we have:
|nr2 = 1 + = 1 + = 1 + 0.472||
Thus nr = 1.213
. Similarly for the blue:
|nb2 = 1 + = 1 + = 1 + 0.821||
Thus nb = 1.349
. We can then calculate the angles of refraction of the two beams as they enter the
medium from Snell's Law. For the red: 1.213 sinθr = sinθi
. This gives θr = sin-1(sin(20o)/1.213) = 16.38o
. For the blue: 1.349 sinθb = sinθi
Giving: θb = 14.69o
. The difference between these two angles is 1.69o
, which is
the amount by which the different colored rays disperse.
What is the rate of change of the speed of light with angular frequency in a dielectric medium?
. But v = c/n
. So since c
is a constant, we can say = c
Now we must take the derivative of this with respect to σ
treating everything else as a constant. This gives:
The required derivative is just c