Electromagnetic radiation had a particular nature - it was tiny packets of energy, rather than a continuous wave
The energy of each photon is directly proportional to its frequency
E = hf where E is the energy of the photon in J, f is the frequency of the electromagnetic radiation in Hz, and h is the Planck's constant (6.63 x 10^-34)
E = hc / lambda
The energy of a photon is inversely proportional to its wavelength
Short wavelength photons, like x-rays, have much more energy than long wavelength radio waves
Electronvolts (eV) --> The energy of 1eV is defined as the energy transferred to or from an electron when it moves through a potential difference of 1V
W = QV = eV
LEDs & Planck's constant:
LEDs convert electrical energy into light energy
The emit visible photons when the pd across them is above a critical value (the threshold pd)
When the pd reaches the threshold pd the LED lights up & starts emitting photons of a specific wavelength
At this pd the work done is given by W=QV
This energy is about the same as the energy of the emitted photon.
We can use the voltmeter to measure the minimum pd that is required to turn on the LED.
A black tube placed over the LED helps to show exactly where the LED lights up.
At the threshold pd, the energy transferred by an electron in the LED is approximately equal to the energy of the single photon it emits
threshold pd x charge on electron = energy of emitted photon
Ve = hf
Ev = hc/ f
Photoelectric effect —> the ejection of electrons from the surface of a metal when it is exposed to electromagnetic radiation of sufficiently high frequency (or short wavelength)
Laws of photoelectric effect:
Increasing the intensity of the radiation incident on a metal surface increases the number of electrons emitted per second
If the incident radiation frequency(f) is a certain threshold frequency(f0), no electrons are emitted, no matter how intense the radiation is
Different meals have different (f0) & (lambda 0) values
The photoelectrons are emitted from a given metal with a range of kinetic energies , from zero up to a maximum value
The maximum kinetic energy (KE max) of the emitted electrons increases with the frequency of the incident radiation and it is independent of the intensity of the radiation
threshold frequency —> the minimum frequency of electromagnetic radiation which will cause photoelectric emission
threshold wavelength —> the maximum wavelength of electromagnetic radiation which will cause photoelectric emission
Kinetic energy gained by electron = energy of incident photon
1/2mv^2 = hf
Work function —> the minimum energy needed by an electron in order to escape from the metal surface
Photoelectric equation:
When a photon of energy (hf) causes photoemission from a metal surface, some of the photon energy is used to overcome the work function, while the remainder appears as kinetic energy of the emitted electron.
hf = work function + KE max
incident photon energy hf0= work function
Observations of the gold leaf experiment:
placing the UV light source closer to the metal plate causes the gold leaf to fall more quickly
Using a higher frequency light source doesn’t change how quickly the gold leaf falls
using a filament lamp source causes no change in the gold leafs position
using a positively charged plate causes no change in the gold leaf’s position
Emission of photoelectrons happen as soon as the radiation is incident on the surface of the metal
Interaction between a photon and surface electron
Each surface electron can only interact with a single photon
Wave - particle duality --> A model used to describe how all matter has both wave & particle properties
Electron diffraction:
Electrons have a mass & charge so they can be accelerated & deflected by electric & magneticfields
Under certain conditions electrons can diffract. They spread out like waves as they pass through a tiny gap, and can form diffraction patterns in the same way as light
For diffraction to occur the size of the gap through which the electrons pass must be similar to their wavelength
Wave - particle duality:
The wavelength of a particle is inversely proportional to its momentum