uncoupling the equations results in second order differential
equations for E and B that are identical to the wave equation
discussed earlier in the semester with a speed for the waves equal
to
The results can be summarized
The directions of oscillation of the electric and magnetic fields are perpendicular to the
direction of propagation of the wave. (EM waves are transverse waves)
The electric and magnetic field oscillate in perpendicular directions.
The vector product of the electric field and the magnetic field gives the direction of
propagation of the wave.
The electric and magnetic fields are sinusoidal.
These electric and magnetic field carry energy and momentum.
Poynting vector
vector representing the rate of energy transfer per unit area
The intensity, I, is defined as the time average of the Poynting vector and is
equal to
Radiation pressure
change in momentum for light
Young
double slit experiment (Chapter 36)
Speed of Light
Galileo
possibly infinite
Roemer
eclipsing moons of Jupiter
2.1 x 108 m/s
Fizeau
rotating wheel
3.1 x 108 m/s
Begin by treating light as a wave.
Huygen's Principle
wave front composed of wavelets
distance between wave fronts = d = c Dt
Ray Approximation
path of light is represented by arrows perpendicular to wave
front.
How does the incident angle compare to the reflected angle.
look at two rays
compare the two triangles indicated
If we can find a relationship between q1 and q1' then we also have a
relationship between qi and qr. That is q1 + qr = 90o and q1' + qi
= 90o
Law of Reflection: The angle of incidence equals the
angle
of reflection.
Refraction
Light passes into material
speed changes
v < c (always)
Index of Refraction (n)
n = c/v
n > 1 for any other material
Total Internal Reflection
We can solve Snell's Law to predict the angle of refraction for a particular boundary
If n2 > n1, (light moving from a material with a low index of refraction to a material
with a high index of refraction) we have no problems but
if n1 > n2,
it is possible that is greater than one and the arcsin is undefined for an
argument greater than one.
when light travels from a material with a high index of refraction to one with a
low index of refraction, there is a critical angle, such that if the incident angle
is greater than this critical angle, the light will not be refracted.
to find this critical angle
When the
angle of
incidence is
greater than
the critical angle, no light will be refracted. All of the incident light will be
reflected back into the material. This phenomena is called total internal
reflection. Total internal reflection is possible only when n2 < n1.
Dispersion
the index of refraction for a material varies with wavelength,
different colors of light are refracted by different amounts
Prism
small wavelengths are bent more than longer wavelengths