PHYS 1112
Chapter 24 Problems
Selected Solutions
- In order to get the light to be strongly reflected by this layer,
we need for the wave to come back (traverse the fluid twice) to the
interface in phase with the light that is reflected from the interface.
Since the index of refraction for glass is less than n = 1.756, we know
that the light that is reflected from the interface from the glass side
will experience a 180o phase shift. If the light is
reflected from the other side, it will experience no phase shift. This
means that the light that traverses the liquid and returns must travel
a distance equal to 1/2 wavelength of the light in the liquid in order
to be in of phase with the light. We can write this as
2t = l'/2
where l' = l/n
= 600 nm/1.756 = 342 nm. If we plug this into the equation, we get
t = l'/4 = 342 nm/4 = 85.4 nm
Of course, other possible thicknesses of this liquid layer that would
also give a strong reflection would be odd integer multiples of this.
- In oder to find out how many dark bands that there will be, we
need to find out how many wavelengths will "fit" in the air gap at the
paper end of the system, i.e. we need to find out m where m is given by
2t = ml
m = 2t/l = 2(4.00 x 10-5
m)/(5.461 x 10-7 m) = 146.5
Therefore, if we include the first dark band, there will be a total of
147 dark bands.
- Since we are at the polarizing angle (Brewster's angle), we know
that the sum of the angle of reflection and the angle of refraction
must equal a right angle, i.e.
qreflected + qrefracted = 90o
These angles must also be consistent with Snell's Law. This means that
sin qincident = sin qreflected = n sin qrefracted
= (1.65) sin qrefracted
sin (90o - qrefracted
) = cos qrefracted = (1.65) sin qrefracted
cot qrefracted = 1.65
qrefracted = cot-1(1.65)
= 31.2o
- This problem is really asking "How many bright fringes
appear in the first 1 cm away from the primary maximum that occurs
at q = 0o ?" Mathematically,
it is asking for the value of m that solves the equation
d sin q1= ml
where q1 is the angle that
subtends the first 1 cm on the screen. Since 1 cm << 2 m, we can
approximate sin q1 by
sin q1 = (.01 m)/(2 m) = .005
m = d (.005)/l = (.001 m)(.005)/(6 x 10-7
m) = 8.3
If you find an error in these, or just have a comment, send an
e-mail message
to jpratte@kennesaw.edu