c = ν × λ
Higher frequency means a shorter vacuum wavelength.
Relation between the speed of electromagnetic radiation, its frequency and its wavelength.
- c
- speed of light in vacuum (m s^-1)
- ν
- frequency (s^-1)
- λ
- wavelength (m)
Use when — The radiation travels in vacuum.
Common trap — Mixing wavelength units, such as nanometres and metres, without converting.
E = h × ν = h × c / λ
Each photon carries energy proportional to its frequency.
Energy carried by a single photon of a given frequency or wavelength.
- h
- Planck constant (J s)
Use when — Referring to the energy of one photon of frequency ν.
Common trap — Using this photon energy directly as a molar energy without multiplying by the Avogadro constant.
K_max = h × ν - φ
Frequency, not intensity, controls whether photoelectrons are ejected and with how much energy.
Maximum kinetic energy of a photoelectron ejected by radiation above the material's threshold.
- K_max
- maximum photoelectron kinetic energy (J)
- φ
- work function of the material (J)
Use when — Photon energy exceeds the material work function.
Common trap — Assuming increasing light intensity alone can cross the threshold frequency.
E_n = -13.6 × Z^2 / n^2 eV
Greater nuclear charge binds the single electron more strongly at a given level.
Bohr energy of a hydrogen-like one-electron species at principal quantum number n.
- Z
- nuclear charge number
- n
- principal quantum number
Use when — Hydrogen or a hydrogen-like one-electron species, within the nonrelativistic Bohr model.
Common trap — Using this formula directly for multi-electron atoms, where it does not apply.
r_n = a0 × n^2 / Z
Higher levels are larger; higher nuclear charge contracts the orbit radius.
Bohr radius of a hydrogen-like one-electron orbit at level n.
- a0
- Bohr radius constant (m)
Use when — A one-electron species is described within the Bohr model.
Common trap — Omitting the nuclear charge Z when comparing radii across different one-electron species.
1/λ = R × Z^2 × (1/n_f^2 - 1/n_i^2)
A spectral photon carries the energy gap between the initial and final levels.
Emission wavenumber for a transition from a higher level n_i to a lower level n_f in a hydrogen-like species.
- R
- Rydberg constant (m^-1)
- n_i
- initial principal quantum number, with n_i greater than n_f
- n_f
- final principal quantum number
Use when — A hydrogen-like species undergoes an electronic transition.
Common trap — Reversing the initial and final levels and reporting a negative wavelength.
λ = h / p
Greater momentum means a shorter matter-wave wavelength.
Matter-wave wavelength associated with a particle of momentum p.
- p
- momentum of the particle (kg m s^-1)
Use when — Matter-wave behaviour is being considered; use the appropriate momentum expression for the given speed regime.
Common trap — Using p = m × v at relativistic speeds without the necessary correction.
Δx × Δp_x ≥ ħ / 2
Quantum states cannot have arbitrarily sharp position and momentum at the same time.
Fundamental lower bound on the product of position and momentum uncertainties for conjugate variables.
- Δx
- standard deviation in position (m)
- Δp_x
- standard deviation in momentum (kg m s^-1)
- ħ
- reduced Planck constant (J s)
Use when — Interpreting position and momentum as statistical standard deviations for conjugate variables.
Common trap — Describing the uncertainty principle as a limitation of measurement technique rather than a fundamental quantum limit.
Radial nodes = n - l - 1; Angular nodes = l
Quantum numbers determine how many radial and angular nodes an orbital must have.
Node counts for hydrogenic orbital forms in terms of quantum numbers.
- n
- principal quantum number
- l
- azimuthal quantum number
Use when — Standard hydrogenic quantum numbers are given for an orbital.
Common trap — Confusing radial probability density peaks with the nodes where the density is zero.