"I am convinced that He [God] does not
play dice"
Albert Einstein
Photo-electric Effect:
Perhaps the most famous demonstration of the particle
properties of electromagnetic waves is the
photo-electric effect . The surface of a metal is illuminated with
UV light leading to the emission of electrons. In 1905 Einstein
explained this phenomenon by assigning particle properties to the
incident UV light. It was this explanation which, in 1921, earned
Einstein the
Nobel Prize - not his theory of Relativity !
UV light is incident on the metal. The
metallic surface is included as part
of a circuit, so that the emitted electrons will create a current,
measured by the ammeter.
Einstein assumed that the incident UV light was comprised of a "
stream" of photons (particles of light). Each photon
carries an energy,
E = hf
where f is the frequency of the
UV light and h = 6.63 x 10 -34 J.s,
known as Planck's constant (Planck had
previously proposed this expression for the energy of a photon, when
attempting to explain
black-body radiation ). Upon interaction with the metallic surface,
the photon is absorbed by an atom (of the metal) and an electron is
emitted. Energy conservation for this single photon process leads
to
hf = KE of emitted electron + energy
necessary to release electron from metallic surface,
or
hf = (KE)e- +
where is called the "work function"
of the metal. Each metal has a characteristic work function.
Note that the photoelectric effect is not
observed for insulators. In metals each atom has at least one
electron which is "loosely" bound to the atom; an UV photon
provides enough energy to release these electrons. In an
insulator all electrons are "tightly" bound; the energy
of an UV photon
is insufficient to release the electron from the atom.
PE effect - Classical and Quantum Predictions:
What makes the photoelectric effect so important in the
development of quantum mechanics is the fact that it could not be
explained by the existing classical laws of physics.
In fact classical physics lead to contrary predictions.
There are three critical properties in which the classical
predictions could not be reconciled with the quantum results.
Cut-off frequency:
Experimentally it is observed that if the frequency of the
incident light is less than a particular (cut-off) frequency, fc,
then no electrons are emitted, independent of the intensity of
the source.
Quantum explanation:
If the energy of each incident photons is less than then
electrons cannot be released from the surface of the metal; the cut-off
frequency is given by,
hfc =
Classical prediction:
There should be no cut-off frequency. The energy of a wave
depends on the intensity (not the frequency). Sooner or later, even a
very low intensity light source will deposit enough energy to release
an electron.
Time delay:
Experimentally it is observed that for f > fc
electrons appear
immediately upon illumination of the surface, no matter how low
the intensity of the source.
Quantum explanation:
The process of electron emission is a particle
process. Even a single photon can emit an electron.
Classical prediction:
There should be a "time delay" between the source being
illuminated and the emission of the first electron. The energy of a
wave is "spread out" meaning that, for a weak source, it could
take some significant time to accumulate enough energy at the location
of a single atom to release an electron.
Electron kinetic energy:
Experimentally it is observed that for a given source frequency
(f > f
c ) the kinetic energy of the emitted electrons is independent of
source intensity.
Quantum explanation:
The kinetic energy of the electrons depends on the frequency of
the source. Increasing the intensity of the source increases the
number of photons which in turn will increase the number of emitted
electrons, but each electron will have the same kinetic energy.
Classical prediction:
Electron kinetic energy should increase with source intensity.
Greater wave intensity implies more energy deposited at the
location of each atom. This additioinal energy appears as
increased kinetic energy.
Electromagnetic
waves have both wave and particle properties
Wave properties dominate at low energy (E = hf), equivalent to
long wavelength and small frequency, e.g. radio waves.
Particle properties dominate at high energy, equivalent to short
wavelength and high frequency, e.g.X-rays.
However, at any wavelength
(frequency) it is possible to observe both aspects - but
not simultaneously .
Electron-Volts
The energies involved in atomic processes such as the
photo-electric effect are extremely small by everyday standards.
In order to avoid having to keep track of large negative powers
of ten when dealing with
energy (mass and momentum) a new unit of energy is introduced - the
electron
volt (eV).
Definition:
The electron-volt is the energy given to an electron
when accelerated through a potential difference of 1 volt