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Why do atoms emit and absorb light only at specific wavelengths, and how does the Bohr model explain this?

Explain atomic emission and absorption spectra using the Bohr model and the relationship between photon energy and energy-level differences.

How discrete atomic energy levels in the Bohr model produce line emission and absorption spectra, and the link between photon energy and the difference between energy levels.

Reviewed by: AI editorial process; not yet individually human-reviewed

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  1. What this dot point is asking
  2. The Bohr model
  3. Why spectra are lines, not continuous
  4. Reading energy-level diagrams
  5. How SACE assesses this

What this dot point is asking

You need to explain emission and absorption line spectra using the Bohr model and the relationship between photon energy and the difference between atomic energy levels.

The Bohr model

Bohr proposed that electrons can only exist in certain allowed orbits, each with a fixed energy - the atom's energy levels. The lowest level is the ground state; higher levels are excited states. An electron cannot have an energy between the allowed levels.

A photon whose energy does not match a level difference is simply not absorbed.

Why spectra are lines, not continuous

Because the energy levels are discrete, only certain transitions - and therefore only certain photon energies and wavelengths - are possible. Each element has its own unique set of levels, so it produces a unique pattern of spectral lines, like a fingerprint. If the levels were continuous, every transition energy would be possible and the spectrum would be an unbroken band; the existence of sharp lines is direct evidence for quantised energy levels.

This is how astronomers identify the elements in stars: dark absorption lines in starlight reveal which elements are present in the star's atmosphere.

Reading energy-level diagrams

Energy levels are usually drawn as horizontal lines, with the ground state at the bottom (most negative energy) and the ionisation level at 00 eV. The energy is negative because the electron is bound; raising it to 00 eV frees it (ionisation). Larger downward jumps emit higher-energy, shorter-wavelength photons.

How SACE assesses this

SACE Stage 2 questions give a set of energy levels (in eV) and ask for the frequency or wavelength of the photon emitted in a stated transition, or work backwards from a measured photon to find an unknown level. The dependable method is: take the difference between the two levels, E=EhigherElowerE = E_\text{higher} - E_\text{lower}, convert from eV to joules using 1 eV=1.60×1019 J1\ \text{eV} = 1.60\times10^{-19}\ \text{J}, then apply E=hfE = hf or E=hcλE = \dfrac{hc}{\lambda}. Sign handling is where most marks are lost, because the levels are negative, so a drop from 0.85-0.85 to 13.6-13.6 eV releases 12.7512.75 eV. A common explanation part asks why discrete spectral lines are evidence for quantised levels; the answer is that each line corresponds to one fixed energy gap, which is only possible if the electron can occupy only certain discrete energies.

Exam-style practice questions

Practice questions written in the style of SACE Board exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

SACE 20244 marksA hydrogen atom has electron energy levels n=1n=1 at 13.6 eV-13.6\ \text{eV}, n=2n=2 at 3.40 eV-3.40\ \text{eV}, n=3n=3 at 1.51 eV-1.51\ \text{eV} and n=4n=4 at 0.85 eV-0.85\ \text{eV}. An electron transitions from n=4n=4 to n=1n=1. Calculate the frequency of the emitted photon. Use h=6.63×1034 J sh = 6.63\times10^{-34}\ \text{J s} and 1 eV=1.60×1019 J1\ \text{eV} = 1.60\times10^{-19}\ \text{J}.
Show worked answer →

The photon energy equals the difference between the levels:

E=E4E1=(0.85)(13.6)=12.75 eV.E = E_4 - E_1 = (-0.85) - (-13.6) = 12.75\ \text{eV}.

Convert to joules: E=12.75×1.60×1019=2.04×1018 JE = 12.75\times1.60\times10^{-19} = 2.04\times10^{-18}\ \text{J}.
Use E=hfE = hf:
f=Eh=2.04×10186.63×1034=3.08×1015 Hz.f = \dfrac{E}{h} = \dfrac{2.04\times10^{-18}}{6.63\times10^{-34}} = 3.08\times10^{15}\ \text{Hz}.

1 mark for the energy difference in eV, 1 mark for the sign handling, 1 mark for converting to joules, 1 mark for using E=hfE = hf to reach about 3.08×1015 Hz3.08\times10^{15}\ \text{Hz} (ultraviolet).

SACE 20234 marksAn electron transitions from n=3n=3 (at 8.0 eV-8.0\ \text{eV}) to n=2n=2, emitting a photon of frequency 8.45×1014 Hz8.45\times10^{14}\ \text{Hz}. Determine the energy of the n=2n=2 level in eV.
Show worked answer →

Photon energy: E=hf=(6.63×1034)(8.45×1014)=5.60×1019 JE = hf = (6.63\times10^{-34})(8.45\times10^{14}) = 5.60\times10^{-19}\ \text{J}.

Convert to eV: E=5.60×10191.60×1019=3.50 eVE = \dfrac{5.60\times10^{-19}}{1.60\times10^{-19}} = 3.50\ \text{eV}.

This equals the gap, E=E3E2E = E_3 - E_2, so E2=E3E=(8.0)3.50=11.5 eVE_2 = E_3 - E = (-8.0) - 3.50 = -11.5\ \text{eV}.
1 mark for the photon energy in joules, 1 mark for converting to eV, 1 mark for E2=E3EE_2 = E_3 - E, 1 mark for the answer of 11.5 eV-11.5\ \text{eV}. The n=2n=2 level is lower (more negative) than n=3n=3, as expected.

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