29 September
Making Light From Matter

Things are not what they seem

Phaedrus, Fables

Assignment:

Reading: Explorations, pp. 147-160.

Sign up for a time slot for Observing Lab #2.

Problem Set #4 is due Thursday at 1:00 pm

In Class:

Question to Ponder

A beam of blue light has a wavelegnth of 400 nm, while a beam of infrared light has a wavelength of 2000nm. What can you say about the speed of the light waves in the two beams?
  • a) The speed of the blue light is five times greater than the speed of the infrared light.
  • b) The speed of the blue light is the same as the speed of the infrared light.
  • c) The speed of the blue light is five times less than the speed of the infrared light.
  • d) You can't say anything about the speeds of these light beams without knowing the frequencies of the light waves.


Einstein Mucks Things Up

  • Until Einstein comes along, everyone's happy with light as a wave of electromagnetic energy.
  • He worries about the Photo-electric Effect.
  • Shine light onto a piece of metal.



  • When blue light is shined on the metal, electrons are knocked off the metal.
  • When red light is shined on the metal, nothing happens, even if you use a really high intensity beam.
  • It's the color (or more precisely the wavelength) of the light that matters.
  • Einstein concludes that light is composed of particles after all (he calls them "photons").
  • Blue light is able to knock the elecrons off the metal because blue light particles have more energy per particle.
  • Red light is made of photons of lower energy, each of which doesn't have enough power to knock off and electron.
  • A brighter red light just means more of those low energy photons, but even in this case each individual photon doesn't have the energy to knock an electron off.
  • Einstein finds that the energy of a photon of light is related to the wavelength as follows:
    Energy of the photon = Eph = hc/lambda
    where h is Planck's constant = 6.626 x 10-34 J s,
    c is the speed of light = 3.00 x 108 m/s, and
    lambda is the wavelength in units of m.


Wave-Particle Duality

  • So in the end, we find that light seems to act like a wave sometimes, and other times like a particle.
  • In flight, light appears to behave very much like a wave. Young's experiment on the diffraction and interference of light has been repeated many times in many ways, and it's very clear that light does things that plain old particles shouldn't do.
  • But Einstein's experiment has also been repeated in a lot of different ways, and it's also true that light interacts with matter in a "quantized" way, delivering its energy in discrete packets whose size depends on wavelength.
  • The real problem here is with our insistence that light should act like either a wave of a particle in the first place. Light just acts like light. The fact that we don't have a good analogy for it probably says more about the limitations of our imagination rather than the quirky nature of light.


Making Light From Matter

  • Light has to be generated somewhere, and most of the light we see comes from matter.
  • Light is nothing but a traveling packet of energy, so in order to emit light, a material must give up some energy.
  • Therefore, to be an emitter, a material must have "extra" energy to give away, and a way to emit it as light.
  • There are two general ways to do this (see below).


Thermal Emission: Making Light from Hot Stuff

  • If you heat a dense material enough, it'll start to glow.
  • It's not burning, but it is giving off light.
  • The material is hotter than its surroundings, and it's cooling off by shedding energy.
  • Called "thermal," or "blackbody" emission, the light from a heated object consists of a photons of a wide and continuous range of wavelengths, e.g., its spectrum is a smooth, rainbow-like blur.
  • The hotter the object gets, the more light is emitted.
  • Also, the hotter the object gets, the more blue the emitted light becomes; that is, the spectrum shifts to shorter wavelengths.
  • This makes sense, since a hotter object will have more energy available, and therefore can make more of the high energy (and short wavelength) photons.
  • Wien's Law describes how the peak of the spectrum (i.e., the wavelength at which the emission is brightest) shifts with temperature (see your book for a quantitative discussion).
  • This is a remarkable result, because it allows us to determine the temperature of an object simply by measuring the emission it produces.


Spectral Line Emission: Photons from Individual Atoms

  • Thermal blackbody emission comes mainly from dense objects, where the individual atoms are either well-linked to one another, or they're so close together that they're always bumping into one another.
  • In constrast, spectral line emission occurs when the density is very low, and atoms are more-or-less free to roam about without bumping into one another very often.
  • In this case, emission occurs when an atom chages from a high energy state to a low energy state.
  • This can be visualized reasonably accurately with a simple atomic model containing a small central nucleus containing neutrons and protons surrounded by a cloud of orbiting electrons.
  • Remarkably, the electrons can't fit into the atom is just any old way; that is, there are only a few specific configurations that are stable.
  • You can think of the different configurations as electron orbits that are closer to or farther from the nuclues (though this is a gross simplification of real atomic structure).
  • Each state of the atom has a certain specified energy, so when an atom makes a change from one state to another lower energy state, it needs to get rid of an amount of energy equal to the difference between the energies of the two states.
  • It gets rid of this "extra" energy by liberating a photon.
  • Only photons whose energies are equal to the difference in energy between two atomic states can be produced, so only a small set of specific wavelength photons can be emitted by a particular atom.
  • The result is a "line" spectrum consisting of emission only at a few specific wavelengths, and no emission at other wavelengths.
  • This means that the spectrum from each different kind of atom will produce a different pattern of emission lines, and therefore produce a kind of light "fingerprint" which is unique for each atomic species.
  • That means we can identify what elements are in stars or other celestial objects just by looking at the pattern of emission in their spectra.

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