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Astronomy 161
Introduction to Solar System Astronomy
Prof. Paul Martini

Lecture 20: Light


Key Ideas:

Speed of Light
Light is Electromagnetic Radiation
Light can be thought of as
Electromagnetic Waves
Photons (particles)
Electromagnetic Spectrum
Sequence of photon energies
Inverse Square Law of Brightness


Speed of Light

Olaus Romer noticed that the timing of the eclipses of Jupiter's moons depended on the Earth-Jupiter distance
Eclipses occur 16.6 minutes later when Jupiter is at conjunction compared to opposition
2 AU is therefore equal to the distance light travels in 16.6 minutes


Fizeau-Foucault Method

In 1850 the French physicists Fizeau and Foucault measured the speed of light in their laboratory:
c = 299,792.458 km/s
In their experiment, the deflection angle increases if:
The mirror rotates faster
There is a larger path length through the experiment


Waves

A "Wave" is any periodic change in the properties of a medium that travels through it and carries energy
"periodic" = with a regularly repeating pattern
Examples:
Water Waves: periodic changes in the height of the water traveling across the surface
Sound Waves: periodic changes in air pressure (compression waves) traveling though the air


Measuring Waves

Waves are described by two numbers
Wavelength: (l)
Distance between successive wave crests
Frequency: (f)
Number of wave crests passing per second
The wave speed, c, is the product of these: c = l x f


Examples of Waves

Ocean Waves:
l = 100m, f = 0.1/second
wave speed: c = 10 m/s (36 km/hr)
Speed depends on water depth, salinity, etc.
Sound Waves: (A 440 cycles per second)
l = 0.73 m, f = 440/second or 440 Hertz (Hz)
wave speed: c = 320 m/s (1150 km/hr)
For sound, "frequency" = "pitch"
Sound waves are pressure changes


Light as a Wave

Can treat light as an Electromagnetic Wave
Periodic changes in the strengths of electric and magnetic fields
Travels through a vacuum at the speed of light
Doesn't need a medium to "wave" in
Speed of light is a constant for all light waves
c = 300,000 km/sec
Independent of wavelength or frequency


Visible Light Waves

Wavelengths:
400 - 700 nanometers (nm)
1 nm = 1 billionth of a meter
Frequencies:
7.5 x 1014 - 4.3 x 1014 waves/sec (or Hertz)
Visible Spectrum:
Red Orange Yellow Green Blue Indigo Violet


Light as a Particle

Can also treat light as particles or Photons
Photon:
Massless particle that carries energy at the speed of light
Photon Energy:
E = h f
f = frequency of light
h = Planck's constant


Photoelectric Effect

Demonstration of the particle nature of light
Light hitting a piece of metal (for example, Cesium) kicks out electrons.
Low-freequency light (e.g. red)
No electrons kicked out, no matter how bright
High-frequency light (e.g. blue)
Number of electrons kicked out is proportional to the brightness of the light
Electron energies are proportional to the frequency
Photons hitting the metal will knock out single electrons only if they have enough energy to break the electrons free of the metal.
Demonstration of this won Einstein the Nobel Prize


Electromagnetic Spectrum

Sequence of photon energies from low to high is called the Electromagnetic Spectrum
Low energy = low frequency = long wavelength
Examples are radio waves, microwaves, infrared
High energy = high frequency = short wavelength
Examples are ultraviolet, X-rays, Gamma Rays


How "Bright" is a Light Source?

We need to quantify how bright an object is
Wave picture of light:
Brightness is the amplitude of the wave (height of the wave crests)
Particle (photon) picture of light:
Brightness is the number of photons per second from the light source
The photon picture is the more useful one


Luminosity

Luminosity is the total energy emitted by an object
Measured in Power Units:
Energy per second emitted (e.g. Watts)
Independent of Distance
Measures the total energy output of an object (e.g. the Sun)


Apparent Brightness

Measures how bright an object appears to be to a distant observer
What we actually measure directly (observable)
Measured in Flux Units:
Energy per second per area from the source
Depends on the distance to the object


Inverse Square Law of Brightness

The Apparent Brightness of a source is inversely proportional to the square of its distance
2 times closer = 4 times brighter
2 times farther = 4 times fainter


See A Note about Graphics to learn why some of the graphics shown in the lectures are not reproduced with these notes.

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Updated: 2010 January 30
Copyright © Paul Martini All Rights Reserved.