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Light Fundamentals

Light is classified as a transverse wave even though no "particles" move in a light wave. Only transverse waves can be polarized. Since light can be polarized, it is classified as a transverse wave.

Light is also classified as an electromagnetic wave since it can pass through a vacuum. Light consists of an electric field and a magnetic field oscillating through space perpendicular to one another. Here are two representations of light as an electromagnetic wave.
                 

Characteristics of light as electromagnetic radiation:

  1. it travels through a vacuum
  2. its speed in a vacuum is 3 x 108 m/s
  3. visible light ranges from 700 nm for red light to 400 nm for violet (blue) light where
    1 nanometer = 1 x 10-9 m

Theories of light:

  1. Newton's corpuscular theory: Newton predicted that light behaved like a particle, called a corpuscle. Newton's theory supports reflection.
  2. Wave theory (Maxwell): light is an electromagnetic wave. The wave theory supports reflection, refraction, interference, and diffraction. Proof that light has a wave nature -- only a wave can interfere and diffract.
  3. Modern theory: dual nature of light. Light acts like a particle when it transfers or absorbs energy; light acts like a wave when it moves through space. Einstein described the particle nature of light. In his equation, E = hf, he describes the energy E of a particle and the corresponding frequency f of the wave. Proof that light has a particle nature -- photoelectric effect, Compton effect, pair production, and emission spectra.

Pulling Things Together
(not asked on APB)

Maxwell's Equations Maxwell showed that light is a traveling configuation of electric and magnetic fields. He formulated differential equations that proved that electromagntic fields spread in the form of polarized waves and at the speed of light. The speed of light is related to purely electric and magnetic quantities.

speed of light formula
Where mo and eo are the permeability of free space(mo = 4p x 10-7 T m/A) and permittivity of free space (eo = 8.85 x 10-12 C2/N m2)

Maxwell's four equations include a generalized form of Coulomb's law called Gauss' law for electricity (describes charge and the electric field), a similar law for the magnetism (describes magnetic field), Faraday's law (describes the electric field produced by a changing magnetic field), and Ampere-Maxwell law (describes a magnetic field produced by a changing electric field, by a current, or by both).

luminous body
produces light
illuminated body
reflects light
luminous flux (symbol is P, SI unit is lumen, lm)
measures the rate at which light is emitted from a source
illumination (symbol is E, SI unit is lux or lumens/m2)
refers to the amount of light falling on a surface

illumination formula

intensity (symbol is I, non-SI unit is candela, cd)
- measures how bright or intense the light is striking a surface. The intensity (or brightness) of light is the amount of energy it carries per unit time.

intensity formula

In our lab, we will be using a Joly photometer to measure the intensity of an unknown light bulb. The photometer is a device that measures the relative intensity of light. It is moved back and forth until both of its sides are equally illuminated.

How this is asked on the AP B exam:  KNOW the inverse square law! Be able to convert power in Watts to intensity in W/ms. This is given by
I = P/(4 p r2)

Light and Matter

Light terms:

color

the color of an opaque object is due to the color that it reflects.
A black object absorbs all color and a white object reflects all color.
The color of a transparent object is due to the combining of transmitted light colors.

Primary colors of transmitted light

red, green, and blue combine to form white light

Secondary colors

produced by combining two primary colors
yellow - formed when green and red are combined
cyan - formed when blue and green are combined
magenta - formed when red and blue are combined

Complementary colors

produced by combining a primary color and a secondary color to form white light

An applet that allows you to mix colors and pigments. Color

The colors of a thin film result from the interference of light reflected from the front and the back surfaces of the thin film. When the film thickness equals ¼ l, that color of light will be constructively interfered with as it reflects from the two surfaces of the film. All others will be destructively interfered with.

Polarized light waves are either vertical or horizontal. They are produced by passing light through a polarizer.

Diffraction

Huygen's Principle Huygen's Principle predicts the future position of a wave when its earlier position is known. "Every point on a wave front can be considered as a source of tiny wavelets that spread out in the forward direction at the speed of the wave itself. The new wave front is the envelope of all the wavelets - that is, tangent to them."

Huygen's principle explains what happens when a wave hits an obstacle and the wave fronts are partially obstructed. It predicts that waves bend behind an obstacle, or diffract. Since diffraction only occurs for waves, not for particles, it verifies the wave nature of light.

Huygen's principle can also be applied to refraction. It predicts, for example, that the speed of light is less in water than in air. Foucault experimentally determined the speed of light in water in 1850, verifying the wave-theory prediction.

Diffraction
spreading of light around the edges of a barrier
Monochromatic light
light of one color. Red light of wavelength of 700 nm is an example of monochromatic light.
Coherent light
light that is totally in-phase. Light produced by a laser is an example of coherent light. The light that exists the laser is totally in-phase.

When light interferes, the light waves produce alternating bright and dark bands of colors (interference fringes); nodal lines appear as dark bands and antinodal lines appear as bright bands. Violet light (with the shortest wavelength) is the least diffracted and red light (with the longest wavelength)is the most diffracted.

Angstrom: 1 A = 1 x 10-10 m

    Spectrum types:
  1. Continuous
    • produced by white light
    • contains all the colors in the rainbow
    • red light is diffracted the most and blue (violet) light is diffracted the least
  2. Absorption (dark line)
    • consists of dark lines on a continuous spectrum background
    • energy is absorbed at characteristic frequencies
  3. Emission (bright line)
  4. energy is emitted at characteristic frequencies

Spectrum types: The top one is a continuous spectrum; the middle is an emission spectrum; and the bottom is an absorption spectrum.

An excellent applet that shows the emission (bright line) spectra of multiple elements. This is a wonderful resource that students can use when working with gas discharge tubes in the laboratory.

Another good resource showing elemental spectra.

Scroll to the bottom of the page to view other spectra.

Diffraction is used experimentally to determine the wavelength of light:

n l = d sin q

Double Slit Diffraction

In 1801, Thomas Young experimentally determined the wavelengths of visible light, obtaining experimental proof for the wave nature of light. In his experiment, light from a single source falls on two closely spaced slits. If light behaved as a particle, we would expect to see two spots on a screen. Instead, Young saw a series of bright lines which he explained as a wave-interference phenomenon.

When the light falls on the two slits, it diffracts, spreading out. The diffracted waves from each slit constructively and destructively interfere. If the waves from the two slits travel the same distance, they are in phase, and produce a bright spot in the center of the screen. Constructive interference also occurs when one wave travels an extra distance that is a whole number multiple of a wavelength of the wave, producing bright lines on the screen. Destructive interference occurs when one wave travels a distance of one-half wavelength (or 3/2, 5/2, etc.) more than the other, producing dark lines on the screen. One sees a bright central spot on the screen, with alternating dark and bright lines (or fringes) on either side.

Since the distance d between the slits is very small compared to the distance to the screen, you can assume that the light rays emerging from each slit are essentially parallel. The light rays make an angle of q with the horizontal. The extra distance that one light ray goes is equal to d sinq.

Constructive interference for a given wavelength of light l occurs when

d sinq = nl
the value of n (1, 2, 3, etc.) is called the order of the interference fringes. The first order fringes (n=1) occur on either side of the central bright spot; the second order fringes (n=2) occur on either side of the first order fringes, etc.

Destructive interference for a given wavelength of light l occurs when

d sinq = (m + 1/2)l where m can have the values of m = 0, 1, 2, ...

In double slit diffraction, the intensity of the bright lines (or fringes) is greatest for the central bright spot and decreases for the higher orders. Except for the central bright spot, the position of the fringe depends upon the wavelength of light. As Young found, the central bright spot apppears as the original, undiffracted light. The higher order fringes, contain a spectrum of the light colors comprising the original light. Their position depends upon their wavelength. Young proved that one color of light is distinguished from another color by wavelength.


The image above shows how intensity varies with position (on the screen) for a double slit diffraction pattern.

The image above shows two waves of light that each pass through a slit of width d and travel the same distance before they arrive at the screen. They constructively interfere because both go the same distance and arrive in-phase.

The image above shows two waves of light that each pass through a slit of width d and travel to a screen. The wave on the bottom travels a distance of 1/2l farther than the top wave. The waves destructively interfere because they arrive at the screen out-of-phase by 1/2 l.

The image shows two waves of light that each pass through a slit of width d and travel to a screen. The wave on the bottom travels a distance of l farther than the top wave. The waves constructively interfere because they arrive at the screen in-phase.

The location of constructive interference fringes can be predicted using:

nl = d sin q where q is the angle that would be formed by wave and a line drawn perpendicular to the screen. We will measure q as shown below.

A 2 source interference applet.

A ripple tank applet. Another ripple tank applet.

A very good Double Slit Diffraction applet

Another diffraction applet

Good applet that relates ripple tank to dirraction pattern on a screen.

Single Slit Diffraction

Single Slit Diffraction Applet

Another single slit applet which lets you vary slit width and slit to screen distance and determine how that affects the diffraction pattern.

Very good applet that shows both single and double slit diffraction

Light passes through a small slit and falls on a screen so far away that the light rays emerging from the slit are considered to be parallel. Light rays that pass straight through are all in phase and produce a central bright spot of undiffracted light.

Consider rays at angle q such that the ray at traveling through the top of the slit travels exactly one wavelength longer than that emerging from the bottom of the slit. The light ray traveling through the center of the slit will travel 1/2 wavelength more than that of one emerging from the top of the slit. This ray will destructively interfere with that passing through the top of the slit. Each ray passing through the bottom half of the slit will cancel with a corresponding ray passing through the top half. The rays destructively interfere in pairs. Thus, no light reaches the screen.

This occurs at angles given by

D sinq = nl
where D is the slit width and n=1,2,3,etc.

Broad bands (areas of light) occur at angles given by

D sinq = (m + 1/2)l
where D is the slit width and m=0,1,2,3,etc. Single slit diffraction differs from double slit in that patterns have a wide central band and dark bands are produced. D sinq = n l locates the position of minima for n=1,2,3,etc. When n=0, the strongest maxima (the central bright spot) occurs. Between the minima, smaller intensity maxima occur. (Notice - the minima for a single slit diffraction pattern satisfy the criteria for a maxima for a double slit pattern.)

The image below shows a graph of intensity vs position for a single slit diffraction pattern. Notice the wide central band and the much less intense secondary bands.

Single slit diffraction applet

diffraction gratingconsists of multiples of single slits that each act as a single slit, producing a much brighter pattern. Gratings are produced by machining very fine parallel lines. If a grating consists of 10,000 lines per cm, the spacing between the lines (D) can be found by first converting cm to m (yielding lines per m) and then taking the reciprocal of this number.

D = meters/line

Thin Film Interference

At the boundary between two different media, light is partially reflected and partially transmitted. If the incident medium is less dense than the transmitted medium, the reflected ray is inverted (it changes phase by 1/2 wavelength). If the incident medium is more dense than the transmitted medium, the reflected ray's orientation is unchanged.

Thin film interference is used to control reflection &/or transmission of light or heat at optical surfaces.

Thin Film Interference Applet To work thin film interference problems, you must realize that a formula is not enough. You must also determine if a phase change occurred at the boundary:

  1. Calculate the wavelength of the light in the medium.
    n lmed = lvac
    where n is the index of refraction in the medium
  2. Determine whether a phase change occurs in the reflected wave or not. Determine the orientation of the reflected wave knowing that the reflected wave is inverted when going from a less to a more dense medium and that the reflected wave's orientation remains the same when going from a more to a less dense medium.
  3. If a phase change occurs, a 1/2lmed shift occurs.
  4. The reflected wave goes an extra distance of 2t, where t is the thickness of the film.
  5. Constructive interference occurs at whole number multiples of wavelengths, or lmed, 2 lmed, etc. (or, mlmed)
  6. If the film is on a less dense surface, there is a net phase change of 1/2 lmed. The condition for constructive interference must be
    2t + 1/2lmed = mlmed, or 2t = mlmed/2
  7. If the film is on a more dense surface, there is no net phase change. The condition for constructive interference must be
    2t = m lmed
  8. Destructive interference occurs at odd multiples of half-wavelengths, or 1/2 lmed, 3/2 lmed, etc. (or, m + 1/2lmed)
  9. If a film is on a less dense surface, there is a net phase change of 1/2 lmed. The condition for destructive interference must be
    2t + 1/2lmed = (m + 1/2)lmed, or 2t = mlmed
  10. If the film is on a more dense surface, there is no net phase change. The condition for destructive interference must be
    2t = (m + 1/2)lmed
Newton's Rings  When a curved glass surface is placed in contact with a flat glass surface, a series of concentric rings is seen when illuminated from above by monochromatic light. These are called Newton's Rings. They are due to the interference between rays reflected by thetop and bottom surfaces of the very thin air gap between the two peices of glass (just like a thin film). Because the width of the air gap increases from the central contact point out to the edges, the extra path length for the lower ray varies, giving rise to a series of bright and dark lines.

Newton's rings

Polarized Light

Applet showing how polarized light is produced

Maxwell's theory of light predicts that light can be polarized since it is a transverse wave. The direction of polarization is taken as the direction of the electric field vector. Polarized light is said to be plane-polarized, or the oscillations are in a plane. In unpolarized light, the electric field vectors vibrate at all angles.

A polarizer produces plane-polarized light by transmitting only the component of light parallel to the axis. An analyzer determines if the light is polarized and what is the plane of polarization.

Light can also be partially polarized by reflection. If light traveling in air is reflected from a medium with index of refraction of n, the incident beam is completely polarized if the incident beam's angle is given by tanq = n.

AP Multiple Choice Questions:

  1. Be prepared to perform simple calculations using n l =d sin q. You can use this to predict the separation of two sources (d) in interference of waves.
  2. Be prepared to differentiate between the characteristics of single and double slit interference patterns.
  3. Be able to recognize the order of the electromagnetic spectrum.
AP Free Response Questions:
  1. Be able to use n l = d sin q in calculations.
  2. Be able to predict how a double slit interference pattern would change if produced in a medium other than air (of known index of refraction). This is based upon the speed of light in the medium.
  3. Be able to use v=lf to calculate the frequency of light and wavelength for media other than air. You would have to use the index of refraction to predict the speed of light in the medium (vmedium=(3 x 108)/nmedium)
  4. Be able to calculate the minimum thickness of a thin film that will result in minimum or maximum reflectance.
  5. Be able to graph intensity of light vs position for a single-slit interference pattern and for a double slit interference pattern.
  6. Be able to calculate the path difference for points of constructive and desctructive interference in double-slit diffraction patterns.
  7. Be able to predict changes in double-slit diffraction patterns if slit width is changed.

AP Objectives - Physical Optics

Light Sample Problems

Light Homework

AP Physical Optics Class Problems