Chapter 11 Quantum Physics Flashcards
The Photon
- Photons are fundamental particles which make up all forms of electromagnetic radiation
- A photon is a massless “packet” or a “quantum” of electromagnetic energy
- Energy is not transferred continuously, but as discrete packets of energy
- each photon carries a specific amount of energy, and transfers this energy all in one go
Calculating Photon Energy
- The energy of a photon can be calculated using the formula:
E = hf
- Using the wave equation, energy can also be equal to:
- Where:
- E = energy of the photon (J)
- h = Planck’s constant (J s)
- c = the speed of light (m s-1)
- f = frequency in Hertz (Hz)
- λ = wavelength (m)
This equation tells us what:
- The higher the frequency of EM radiation, the higher the energy of the photon
- The energy of a photon is inversely proportional to the wavelength
- A long-wavelength photon of light has a lower energy than a shorter-wavelength photon
Photon Momentum
- a photon travelling in a vacuum has momentum, despite it having no mass
- The momentum (p) of a photon is related to its energy (E) by the equation and Where c is the speed of light:
The Electronvolt is derived from?
- the definition of potential difference:
- When an electron travels through a potential difference, energy is transferred between two points in a circuit, or electric field
electronvolt is defined as:
The energy gained by an electron travelling through a potential difference of one volt
1 eV = 1.6 × 10-19 J
(relation to kinetic energy) When a charged particle is accelerated through a potential difference, it
- gains kinetic energy
- If an electron accelerates from rest, an electronvolt is equal to the kinetic energy gained:
eV = ½ mv2
- Rearranging the equation gives the speed of the electron:
- To convert between eV and J:
- eV → J: multiply by 1.6 × 10-19
- J → eV: divide by 1.6 × 10-19
The photoelectric effect is the
- phenomena in which electrons are emitted from the surface of a metal upon the absorption of electromagnetic radiation
- Electrons removed from a metal known as photoelectrons
The photoelectric effect provides important evidence that light is
quantised, or carried in discrete packets
- This is shown by the fact each electron can absorb only a single photon
- This means only the frequencies of light above a threshold frequency will emit a photoelectron
The photoelectric effect can be observed on a
- gold leaf electroscope
- A plate of metal, usually zinc, is attached to a gold leaf, which initially has a negative charge, causing it to be repelled by a central negatively charged rod
- This causes negative charge, or electrons, to build up on the zinc plate
- UV light is shone onto the metal plate, leading to the emission of photoelectrons
- This causes the extra electrons on the central rod and gold leaf to be removed, the gold leaf begins to fall back towards the central rod
- they become less negatively charged, and hence repel less
Some notable observations of photoelectric effect can be observed on a gold leaf electroscope
- Placing the UV light source closer to the metal plate causes the gold leaf to fall more quickly
- Using a higher frequency light source does not change the how quickly the gold leaf falls
- Using a filament light source causes no change in the gold leaf’s position
- Using a positively charged plate also causes no change in the gold leaf’s position
- The threshold frequency is defined as:
The minimum frequency of incident electromagnetic radiation required to remove a photoelectron from the surface of a metal
The threshold wavelength, related to
- threshold frequency by the wave equation, is defined as:
The longest wavelength of incident electromagnetic radiation that would remove a photoelectron from the surface of a metal
- Threshold frequency and wavelength are properties of a material, and vary from metal to metal
The Photoelectric Equation
E = hf = Φ + ½mv2max
- Symbols:
- h = Planck’s constant (J s)
- f = the frequency of the incident radiation (Hz)
- Φ = the work function of the material (J)
- ½mv2max= the maximum kinetic energy of the photoelectrons (J)
- Since energy is always conserved, the energy of an incident photon is equal to:
The threshold energy + the kinetic energy of the photoelectron
- The energy within a photon is equal to hf
- This energy is transferred to the electron to release it from a material (the work function) and gives the emitted photoelectron the remaining amount as kinetic energy
(E = hf = Φ + ½mv2max )This equation demonstrates
- If the incident photons do not have a high enough frequency (f) and energy to overcome the work function (Φ)
- >no electrons will be emitted
- When hf0 = Φ, where f0 = threshold frequency, photoelectric emission only just occurs
- Ekmax depends only on the frequency of the incident photon, and not the intensity of the radiation
- The majority of photoelectrons will have kinetic energies less than Ekmax
Graphical Representation of Work Function
- The photoelectric equation can be rearranged into the straight line equation:
- y = mx + c
- Comparing this to the photoelectric equation:
- Ekmax = hf - Φ
- A graph of maximum kinetic energy Ekmax against frequency f can be obtained
The key elements of the graph:
- The work function Φ is the y-intercept
- The threshold frequency f0 is the x-intercept
- The gradient is equal to Planck’s constant h
- There are no electrons emitted below the threshold frequency f0
- The work function Φ, or threshold energy, of a material is defined as:
The minimum energy required to release a photoelectron from the surface of a material
an electron can only escape the surface of the metal if
it absorbs a photon which has an energy equal to Φ or higher because the electrons in a metal as trapped inside an ‘energy well’ where the energy between the surface and the top of the well is equal to the work function Φ
A single electron absorbs one photon
- Different metals have different threshold frequencies, and hence different work functions
- Using the well analogy:
- A more tightly bound electron requires more energy to reach the top of the well
- A less tightly bound electron requires less energy to reach the top of the well
Alkali metals have threshold frequencies in the
- such as sodium and potassium, have threshold frequencies in the visible light region
- This is because the attractive forces between the surface electrons and positive metal ions are relatively weak
Alkali metals have threshold frequencies in the
- such as sodium and potassium, have threshold frequencies in the visible light region
- This is because the attractive forces between the surface electrons and positive metal ions are relatively weak