Chapter 3 Flashcards
Threshold frequency
The minimum frequency of light that can cause the photoelectric effect
The atom
The atom is formed of 3 constituents protons,neutrons and electrons.
Specific charge
The SP of a particle is the charge - mass ratio and is calculated by dividing a particles charge by its mass
Charge / mass
The photo electric affect
Is where photoelectrons are emitted for the surface of a metal after light above a certain frequency is shone on it. This certain frequency is different for different types of metals and is called the threshold frequency.
The threshold frequency
Couldn’t be explained by wave theory, as it suggest that any frequency of light should be able to cause the photoelectric emission as the energy absorbed by each electron will gradually increase with each incoming wave.
Threshold frequency explained with the photon model of light
Em waves travel in discrete packets called photons, which have an energy which is directly proportional to the frequency
Each electron can absorb a single photon therefore a photon electron is only emitted if the frequency is above the threshold frequency.
If the intensity of the light is increased if the frequency is above the threshold more photon electrons are emitted per second.
What is work function
Work function of a metal is the minimum energy required for electrons to be emitted from the surface of a metal and it is denoted by (circle with a line going straight down)
Stopping potential
Stopping potential is the potential difference you would need to apply across the metal to stop the photo electrons with the maximum kinetic energy. Measuring stopping potential allows you to find the maximum kinetic energy of the released photo electrons as EK (max) = eVs. Where Vs is the stopping potential and e is the charge of an electron.
This is derived using the fact that energy = charge x voltage.
PE equation
E = h x f = 0| + Ek (max)
Shows relationships between work function, maximum kinetic energy and the frequency of light.
Collisions of electrons and excitation
Electrons in atoms can only exist in discrete energy levels, these electrons can gain energy from Collisions with free electrons, which can cause them to move up in Energy levels this is known as excitation
They gain enough energy to be removed from the atom entirely this is called ionisation
If an electron becomes excited …
It will quickly return to its original energy level ( ground state) and therefore releases energy it gained in the form of the photon.
Fluorescent tube
An example of a practical use of excitation is in a fluorescent tube in order to produce light.
Fluorescent tubes are filled with mercury vapour, across which a high voltage is applied.
This voltage accelerates free electrons through the tube, which collide with the mercury
atoms causing them to become ionised, releasing more free electrons.
The free electrons collide with the mercury atoms, causing them to become excited. When they de-excite they release photons, most of which are in the UV range.
The (phosphorous) fluorescent coating on the inside of the tube, absorbs these UV photons and therefore electrons in the atoms of the coating become excited and de-excite releasing photons of visible light.
describing the energy difference between energy levels,
When describing the energy difference between energy levels, the values of energy are very small, therefore the unit, electron volts (eV) is used instead of joules (J).
An electron volt is defined as the energy gained by one electron when passing through a potential difference of 1 volt.
Energy levels and photon emission
By passing the light from a fluorescent tube through a diffraction grating or prism, you get a line spectrum.
Each line in the spectrum will represent a different wavelength of light emitted by the tube.
As this spectrum is not continuous but rather contains only discrete
values of wavelength, the only photon energies emitted will correspond to these
wavelengths, therefore this is evidence to show that electrons in atoms can only transition between discrete energy levels,
line absorption spectrum
which looks like a continuous spectrum of all possible wavelengths of light, with black lines at certain wavelengths.
These lines represent the possible differences in energy levels as the atoms in the gas can only absorb photons of an energy equal to the exact difference between two energy levels.