Chapter revision
Revision summary
Key ideas, equations and common mistakes. Open any topic below for the full explanation.
Identify the evidence and the quantity being predicted. A photon energy, a probability density, a momentum spread and an atomic energy gap require different calculations.
Choose the model before the equation
| Task | Keep this distinction |
|---|---|
| Light evidence | Threshold frequency supports quantised energy exchange; interference and diffraction support wave behaviour. Frequency changes energy per photon, while intensity at fixed frequency changes photon rate. |
| Momentum and wavelength | A photon has p = E/c = h/λ despite zero rest mass. A non-relativistic electron uses p = mv and λ = h/p. Do not use E = pc for its kinetic energy. |
| Position probability | Amplitude can be signed; density |ψ|2 is nonnegative. An interval probability is density area, not density alone or the square of amplitude area. |
| Coherent alternatives | Add amplitudes before squaring. Relative signs or phases affect interference. A global sign reversal of one complete real state does not change its density. |
| Localisation | A narrower position distribution needs a broader momentum distribution. The width relation concerns spread, not a required mean momentum or apparatus error. |
| Confinement | Boundary conditions select standing shapes and quantised energies. A wavefunction plot is not a particle trajectory, and the box's level sequence is not an atom's exact sequence. |
| Spectral lines | Use an allowed gap from the actual occupied level. Photon energy is the magnitude of the energy change, not the absolute value of one level. |
Photon and matter-wave calculations
Threshold: Φwork = hf0
Matter wave: λ = h/p
Non-relativistic massive particle: p = mv
For the 6.00 × 1014 Hz photon, λ = 500 nm, E ≈ 2.49 eV and p ≈ 1.33 × 10-27 kg m/s. The 1.50 × 106 m/s electron instead has λ ≈ 0.485 nm. Doubling its speed halves wavelength while quadrupling kinetic energy.
Normalisation and area
For a profile that vanishes outside 0 < x < L:
C2L = 1, so C = 1/√L
Sine profile ψ = C sin(πx/L):
C2L/2 = 1, so C = √(2/L)
Choose a global sign without changing probabilities. At L = 4.00 nm, the positive coefficients are 0.500 and 0.707107 nm-1/2. The square profile gives probability 0.375 over 1.00-2.50 nm. The sine profile's central 1.00-3.00 nm probability is about 0.818310; a coarse trapezium estimate need not equal that smooth-model area.
The coordinate and density units must match: nm-1 times nm gives a dimensionless probability. For coherent real contributions, (a + b)2 includes 2ab. Do not replace it with a2 + b2. Detection-bin frequencies estimate finite-interval probabilities and do not establish a classical path or exact point probability.
Width scales, box states and atomic gaps
Infinite well: ψn = √(2/L) sin(nπx/L)
λn = 2L/n
En = h2n2/(8mL2)
The width relation is an order-of-magnitude convention, not an exact equality. Infinite-well states have n = 1, 2, 3, ... and n - 1 interior nodes. Their first energies are in the ratio 1:4:9. Doubling width quarters energies at fixed n and mass; n = 2 at width 2L has the same energy as n = 1 at width L.
In the supplied atom, levels -6, -3 and -1 eV give permitted gaps of 3, 2 and 5 eV. The emitted wavelengths are about 414, 622 and 249 nm. A ground-state absorber can use the 3 and 5 eV upward gaps; the 2 eV absorption requires the -3 eV state to be occupied. The 249 nm line is ultraviolet.
Quantities and units
| Quantity and symbol | Unit | Meaning |
|---|---|---|
| Energy E, En | J or eV | 1 eV = 1.60 × 10-19 J. |
| Work function Φwork | J | Minimum surface-removal energy, distinct from magnetic flux. |
| Planck constant h | J s | 6.63 × 10-34 J s in these examples. |
| Momentum p | kg m/s = N s | Photon and massive-particle relations have different conditions. |
| Frequency f | Hz | Sets energy per photon. |
| Vacuum light speed c | m/s | 3.00 × 108 m/s. |
| Wavelength λ; width L; position x | m or nm | 1 nm = 10-9 m. Match density units to the position coordinate. |
| Mass m, me | kg | me = 9.11 × 10-31 kg. |
| Elementary charge e | C | 1.60 × 10-19 C; eV itself is an energy unit. |
| One-dimensional amplitude ψ | m-1/2 or nm-1/2 | Its modulus squared is the corresponding inverse-length density. |
| Probability; quantum number n | No unit | Probability is between 0 and 1. Here n labels a box state, not amount of substance. |
| Box potential energy V | J or eV | The local symbol V here does not mean electric potential. |
A three-dimensional electron cloud instead uses probability per volume, with SI density unit m-3. Always identify what the graph's vertical axis represents before reading a height or calculating an area.
Review a topic
- Evidence for photons
- Matter waves and detections
- Wavefunctions and probability
- Adding probability amplitudes
- Localisation and momentum spread
- A particle in a box
- Atomic transitions and spectra