Title: Chapter 33. Electromagnetic Waves
1Chapter 33. Electromagnetic Waves
- 33.1. What is Physics?
- 33.2. Maxwell's Rainbow
- 33.3. The Traveling Electromagnetic Wave,
Qualitatively - 33.4. The Traveling Electromagnetic Wave,
Quantitatively - 33.5. Energy Transport and the Poynting
Vector - 33.7. Polarization
- 33.8. Reflection and Refraction
- 33.9. Total Internal Reflection
- 33.10. Polarization by Reflection
2What is Physics?
3Maxwell's Rainbow
4Sensitivity of the average human eye
5Electromagnetic Waves
- It consists of mutually perpendicular and
oscillating electric and magnetic fields. The
fields always vary sinusoidally. Moreover, the
fields vary with the same frequency and in phase
(in step) with each other. - The wave is a transverse wave, both electric and
magnetic fields are oscillating perpendicular to
the direction in which the wave travels. The
cross product always gives the direction
in which the wave travels. - Electromagnetic waves can travel through a vacuum
or a material substance. - All electromagnetic waves move through a vacuum
at the same speed, and the symbol c is used to
denote its value. This speed is called the speed
of light in a vacuum and is - The magnitudes of the fields at every instant and
at any point are related by
6Properties of the Wave
- Wavelength ? is the horizontal distance between
any two successive equivalent points on the wave. - Amplitude A is the highest point on the wave
pattern. - Period T is the time required for the wave to
travel a distance of one wavelength. Unit is
second. - Frequency f f1/T. The frequency is measured in
cycles per second or hertz (Hz). - Speed of wave is v?/T ?f
7The Speed of Light
- All electromagnetic waves travel through a vacuum
at the same speed, which is known as the speed of
light c3.00108 m/s. - All electromagnetic waves travel through a
material substance with the speeds less than the
speed of light in vacuum c3.00108 m/s. The
waves with different wave lengths may have
different speeds in a material substance. - In 1865, Maxwell determined theoretically that
electromagnetic waves propagate through a vacuum
at a speed given by
(m/s)
8The Energy Carried by Electromagnetic Waves
9Poynting Vector
- The rate of energy transport per unit area in EM
wave is described by a vector, called the
Poynting vector
- The direction of the Poynting vector of an
electromagnetic wave at any point gives the
wave's direction of travel and the direction of
energy transport at that point.
10Intensity of EM Wave
the root-mean-square value of the electric field,
as
- The time-averaged value of S is called the
intensity I of the wave
The root-mean-square value of the electric field,
as
- The energy associated with the electric field
exactly equals to the energy associated with the
magnetic field.
11Variation of Intensity with Distance
12Polarization
- A linearly polarized electromagnetic wave is one
in which the oscillation of the electric field
occurs only along one direction, which is taken
to be the direction of polarization.
- Polarized randomly, or unpolarized wave is one
in which the direction of polarization does not
remain fixed, but fluctuates randomly in time.
13Polarizing Sheet
- An electric field component parallel to the
polarizing direction is passed (transmitted) by a
polarizing sheet a component perpendicular to it
is absorbed. - one-half rule an unpolarized light pass through
a polarizing sheet, the intensity I of the
emerging polarized light is
14MALUS LAW
15Example
16Example
17Example
- What value of ? should be used in Figure, so
the average intensity of the polarized light
reaching the photocell is one-tenth the average
intensity of the unpolarized light?
18Geometrical Optics
- Wave fronts the surfaces through all points of
the wave that are in the same phase of motion are
called wave fronts. - Rays the radial lines pointing outward from the
source and perpendicular to the wave fronts are
called rays. The rays point in the direction of
the velocity of the wave.
- Although a light wave spreads as it moves away
from its source, we can often approximate its
travel as being in a straight line. The study of
the properties of light waves under that
approximation is called geometrical optics
19Reflection and Refraction
20The Reflection of Light
- Why are we able to see ourselves from mirror?
21LAW OF REFLECTION
- The incident ray, the reflected ray, and the
normal to the surface all lie in the same plane,
and the angle of reflection ?r equals the angle
of incidence ?i
22Example
- Two plane mirrors are separated by 120, as the
drawing illustrates. If a ray strikes mirror M1,
at a 65 angle of incidence, at what angle ? does
it leave mirror M2?
23Law of refraction
- A refracted ray lies in the plane of incidence
and has an angle ?2 of refraction that is
related to the angle of incidence ?1 by
the symbols n1 and n2 are dimensionless
constant, called the index of refraction
24Dispersion
- The index of refraction n encountered by
light in any medium except vacuum depends on the
wavelength of the light. The dependence of n on
wavelength implies that when a light beam
consists of rays of different wavelengths, the
rays will be refracted at different angles by a
surface that is, the light will be spread out by
the refraction. This spreading of light is called
chromatic dispersion,
- The index of refraction n in the different
materials is different for the same wave length
of lights. - The index of refraction n in the same materials
is different for different wave length of lights.
25Dispersion
26Total Internal Reflection
27Polarization by Reflection
- A ray of unpolarized light incident on a glass
surface. The electric field vectors of the light
has two components. The perpendicular components
are perpendicular to the plane of incidence The
parallel components are parallel to the plane of
incidence. Because the light is unpolarized,
these two components are of equal magnitude. - The reflected light also has both components but
with unequal magnitudes. - When the light is incident at a particular
incident angle, called the Brewster angle , the
reflected light has only perpendicular
components,