00:01
So a few words about the photoelectric effect, which is an effect that demonstrates that light behaves like little quanta of packets of energy.
00:13
And the explanation of this phenomena can only be made if light behaves as quanta of energy.
00:23
But the idea is, or the experiment involves the interaction of photons with either a metal surface or, a metal oxide.
00:34
A photon comes in and it must have enough energy so that it pulls the electron inside the surface out of the surface and perhaps gives the electron a little bit of energy once it leaves the surface.
00:50
So here is kind of a more energy level picture of what's going on.
00:54
The electron is in a potential well.
00:58
The depth of that well is known as the work function so when the photon gets absorbed, here's the electron, in comes the photon.
01:17
If it has enough energy to pull the electron out, the electron will come up to a potential energy of zero and leave the well with kinetic energy.
01:31
So the energy of the incoming photon goes to two things.
01:35
It goes into the potential energy, which, depending on the units of the work function, it could just be equal to the work function in electron volts.
01:48
Sometimes the work function is just given in volts, but the potential energy is the work function in electron volts.
01:58
And so the energy of the photon gets absorbed and brings the electron up to potential, equals to zero and then adds to the kinetic energy of the electron.
02:18
Meanwhile the photon disappears, gets totally absorbed.
02:23
Conservation of energy.
02:25
So let's take a look at an example.
02:27
We're going to take a nickel, clean nickel surface, so not a nickel oxide.
02:34
We can look up the work function.
02:36
It is 5 .1 electron bolts.
02:39
The energy of the photon coming in can be determined from hc over the wavelength, and we'll take the wavelength as a short ultraviolet to 106 nanometers...