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Atomic Spectra

Level 1 - Physics topic page in Matter Waves.

Principle

Atomic line spectra come from photons emitted or absorbed between discrete energy levels.

Notation

\(E_i,E_f\)
initial and final atomic energies
\(\mathrm{J}\)
\(\Delta E\)
energy difference
\(\mathrm{J}\)
\(f\)
photon frequency
\(\mathrm{Hz}\)
\(\lambda\)
photon wavelength
\(\mathrm{m}\)
\(h\)
Planck constant
\(\mathrm{J\,s}\)
\(c\)
speed of light
\(\mathrm{m\,s^{-1}}\)

Method

Derivation 1: Connect energy gaps to photons

An atom emits a photon when it moves from a higher energy level to a lower one.

Emission energy
\[hf=E_i-E_f\]
Photon wavelength
\[\lambda=\frac{c}{f}\]
Energy wavelength
\[E_i-E_f=\frac{hc}{\lambda}\]

Derivation 2: Absorb only allowed energies

Absorption occurs when the photon energy matches an available upward transition.

Absorption condition
\[hf=E_f-E_i\]

Derivation 3: Use spectra as fingerprints

Different atoms have different level spacings, so their line spectra identify the element.

Rules

Photon energy
\[E_\gamma=hf=\frac{hc}{\lambda}\]
Emission
\[E_\gamma=E_i-E_f\]
Absorption
\[E_\gamma=E_f-E_i\]
Electronvolt
\[1\,\mathrm{eV}=1.60\times10^{-19}\,\mathrm J\]

Examples

Question
A transition releases
\[3.00\,\mathrm{eV}\]
Find the photon wavelength using
\[hc=1240\,\mathrm{eV\,nm}\]
Answer
\[\lambda=\frac{hc}{E}=\frac{1240}{3.00}=413\,\mathrm{nm}\]

Checks

  • Emission: atom loses energy, photon carries the gap.
  • Absorption: atom gains energy, photon must match an allowed gap.
  • Shorter wavelength means larger photon energy.
  • Line spectra imply discrete atomic energies.