Revision Notes
A Level Physics: Quantum Physics — Revision Notes
Condensed recall notes on the photoelectric effect, photon energy, wave-particle duality and energy levels for Cambridge AS & A Level Physics 9702.
- Subject
- Physics
- Level
- A LEVEL
- Topic
- Quantum physics
- Author
- Iftikhar Azeemi
- Updated
- Reviewed by
- Hassan (what this means)
Aligned to Cambridge A Level Physics (9702), 2025-2027. Official specification .
Syllabus page (what it covers and how it is assessed): Cambridge A Level Physics.
Syllabus points this page covers
9702 (A Level)
- 22.1 Energy and momentum of a photon
- 22.2 Photoelectric effect
- 22.3 Wave-particle duality
- 22.4 Energy levels in atoms and line spectra
Found an error? Report a correction.
Need help with this topic? Request a free trial class for A Level Physics (9702).
Condensed for the final weeks. For the full explanation, use the Quantum Physics study guide.
Photon energy
E = h f = h c / lambda h = 6.63 x 10^-34 J s
1 eV = 1.60 x 10^-19 J
The electron-volt is a convenient unit at the atomic scale: it is defined as the energy gained by an electron accelerated through a potential difference of 1 V.
The photoelectric effect
h f = Phi + KE_max
Phi = h f_0 (work function = threshold frequency x h)
KE_max = h f - Phi
Work function Φ — the minimum energy needed to remove an electron from the metal surface. Threshold frequency f₀ — below it, no emission occurs however intense the light.
The four observations, and what each one proves
| Observation | What it rules out |
|---|---|
| No emission below f₀, whatever the intensity | Wave theory — a wave could deliver enough energy eventually |
| Emission is instantaneous above f₀ | Wave theory — energy would need time to accumulate |
| KE_max depends on frequency, not intensity | Wave theory — brighter light should give faster electrons |
| Intensity affects the rate of emission only | Confirms one photon → one electron |
The one-to-one interaction is the whole argument. One photon transfers all its energy to one electron. If that quantum is smaller than Φ, nothing happens — and waiting does not help, because the energy is not accumulated.
Worked example
A metal has a work function of 2.0 eV. Light of frequency 8.0 × 10¹⁴ Hz shines on it. Find the maximum kinetic energy of emitted electrons, in eV.
E = hf = 6.63 x 10^-34 x 8.0 x 10^14 = 5.30 x 10^-19 J = 3.31 eV
KE_max = hf - Phi = 3.31 - 2.0 = 1.31 eV
Working directly in eV avoids an unnecessary unit conversion once the photon energy has been found.
Wave-particle duality
The photoelectric effect is strong evidence that light behaves as particles; interference and diffraction are equally strong evidence that light behaves as a wave. Both are true — this is wave-particle duality, and it applies in reverse to particles like electrons too.
de Broglie: lambda = h / p = h / (m v)
Electrons accelerated through a p.d. V gain energy eV = ½mv², giving λ = h/√(2meV).
Evidence: electron diffraction through a thin graphite film produces rings — diffraction is a wave property, yet electrons are particles. Conversely the photoelectric effect shows light, a wave, behaving as particles.
Because h is tiny, everyday objects have wavelengths far too small to observe — a macroscopic object’s de Broglie wavelength is many orders of magnitude smaller than any aperture it could pass through, so no diffraction is ever seen. An electron at a few hundred eV has a wavelength comparable to atomic spacing, which is why it diffracts from a crystal lattice.
Energy levels and spectra
Electron energy levels are discrete and negative (zero is defined at infinite separation — a bound electron has less energy than a free one).
h f = E_1 - E_2
| Spectrum | Cause |
|---|---|
| Emission line | Electron falls from higher to lower level, emitting a photon of exactly ΔE |
| Absorption line | Photon of exactly ΔE is absorbed, lifting an electron to a higher level |
Line spectra are discrete precisely because energy levels are discrete — this is the direct experimental evidence for quantisation, and each element’s pattern is unique, which is how stellar composition is determined from the absorption lines in starlight.
Exam traps
- Saying more intense light gives faster photoelectrons. It gives more of them.
- Using average energy rather than one-photon-one-electron.
- Forgetting to convert eV to J before substituting.
- Omitting the minus sign on energy levels.
- Using λ = h/mv with a speed found from a non-relativistic formula where it isn’t valid.
- Saying an electron “is” a wave or “is” a particle rather than exhibiting both behaviours depending on the experiment.
Self-test
- State the photoelectric equation and define the work function.
- Why does intense red light fail to eject electrons when faint blue light succeeds?
- What single feature of photon–electron interaction explains the threshold frequency?
- State de Broglie’s relation and the evidence for it.
- Why are line spectra discrete?
- A metal has a work function of 2.0 eV. Light of frequency 8.0 × 10¹⁴ Hz shines on it. Find KE_max in eV.
Answers: 1. hf = Φ + KE_max; Φ is the minimum energy required to remove an electron from the metal surface. 2. Red photons individually carry less energy than Φ; intensity only increases the number of photons, and energy is not accumulated because one photon interacts with one electron. 3. The one-to-one interaction — a single photon transfers all its energy to a single electron, so if hf < Φ no emission occurs at any intensity. 4. λ = h/p; electron diffraction rings from a thin graphite film. 5. Because electron energy levels are discrete, so only photons of energy exactly equal to a difference between two levels can be emitted or absorbed. 6. E = hf = 6.63×10⁻³⁴ × 8.0×10¹⁴ = 5.30×10⁻¹⁹ J ≈ 3.31 eV; KE_max = 3.31 − 2.0 = 1.31 eV.
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