Line Spectra

Key idea: Distinguish emission and absorption line spectra, explain why spectra are discrete, and use ΔE = hf = hc/λ for transitions (A Level Physics).

  • GCE A-Level H2 Physics 2027
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Learning objectives

  • Analyse atomic energy levels and emission or absorption spectra.

1. Definitions (Must Know)

A. Emission line spectrum

An emission line spectrum is a set of discrete bright lines on a dark background, produced when excited atoms emit photons as electrons drop to lower energy levels.

B. Absorption line spectrum

An absorption line spectrum is a continuous spectrum with discrete dark lines removed, produced when atoms absorb photons of specific energies that match allowed transitions.

C. Transition energy

Photon energy in a transition is:

Δ E = hf = hc/λ

2. Key Ideas (What Earns Marks)

Photon absorption and emission between atomic energy levelsDiscrete atomic energy levels show an upward absorption transition and a downward emission transition, each labelled with photon energy equal to the level difference.EnergyE₁E₂E₃absorptionhf = E₃ − E₁emissionhf = E₃ − E₂
Scroll diagram horizontally to read all labels.
Absorption raises an electron only when the photon energy matches an allowed gap. Emission releases a photon whose energy equals the downward energy-level difference.
  • Line spectra exist because atomic energy levels are discrete.
  • Emission: photon energies correspond to downward transitions.
  • Absorption: only photons with exactly the right energies are absorbed (matching energy gaps).
  • Emission and absorption line positions match for the same gas (same energy gaps).
Syllabus link (9478)

This lesson targets learning outcomes 19k–19m: discrete levels, emission vs absorption spectra, and photon energies in transitions.

3. Detailed Explanations

A. Emission spectra (how they form)

If a low-pressure gas is excited (e.g. in a discharge tube), electrons in atoms can move to higher energy levels.

When they return to lower levels, they emit photons with energies equal to the differences between levels. Because only certain energy differences exist, only certain photon frequencies/wavelengths appear.

Hydrogen and iron emission spectra compared with absorptionHydrogen has four prominent visible Balmer lines at about 410, 434, 486 and 656 nanometres. Iron has many discrete emission lines in an illustrative dense pattern. An absorption spectrum is continuous colour crossed by dark lines at absorbed wavelengths.Hydrogen emission: four prominent visible Balmer lines410 nm434 nm486 nm656 nmIron emission: many discrete lines (illustrative, not a wavelength scale)Absorption: continuous spectrum with selected wavelengths removed
Hydrogen's prominent visible Balmer lines are labelled with approximate wavelengths. Iron illustrates a much denser element-specific line pattern; absorption removes selected wavelengths from a continuous spectrum.
Hydrogen line data used in the figure
Approximate wavelengthVisible colour region
410.2 nmviolet
434.0 nmviolet-blue
486.1 nmblue-green
656.3 nmred

B. Absorption spectra (how they form)

If white light passes through a cooler gas, atoms absorb photons whose energies match allowed upward transitions.

Those wavelengths are missing from the transmitted light, so dark lines appear.

The bottom row of the comparison figure shows the corresponding absorption idea: dark lines appear where photons are absorbed for upward transitions.

C. Emission vs absorption (comparison)

FeatureEmission spectrumAbsorption spectrum
Backgrounddarkcontinuous
Linesbrightdark
Processelectron drops and emits photonelectron absorbs photon and rises
Photon energiesequal to energy gapsequal to the same energy gaps

4. Common Mistakes

  • Saying “any photon can be absorbed” (only photons matching energy gaps are absorbed).
  • Mixing up emission and absorption diagrams (remember: bright vs dark lines).
  • Forgetting Δ E = hf applies to each transition.

5. Exam Tips

  • If asked “why lines are discrete”, say: “energy levels are discrete so only certain ΔE exist”.
  • If asked for a photon wavelength, use: λ = hc/(Δ E) and keep units consistent.

6. Worked Examples

Modelled example 1

Emission vs absorption identification

Core

Problem

A spectrum shows a continuous rainbow background crossed by thin dark lines. Identify the spectrum and explain how it forms.
Study the worked solution
  1. Read the visual evidence

    Method

    It is an absorption line spectrum.

    Reason

    A continuous background with selected dark wavelengths is the defining appearance of absorption.

    Working

    continuous background + dark lines → absorption
  2. Explain the missing wavelengths

    Method

    Atoms absorb photons whose energies match allowed upward transitions.

    Reason

    Discrete atomic energy levels permit only particular energy gaps.

    Working

    Δ E = hf = hc/λ

Guided practice 2

Photon wavelength from energy gap

About 4 min

Problem

An atomic transition has energy difference Δ E = 2.0 eV. Estimate the photon wavelength using hc = 1240 eV nm.

Try this before viewing the solution

Unit: nm

Hints

Hint 1: match the units
Because both Δ E and hc use eV-based units, use λ = hc/Δ E directly in nanometres.
View solution step by step
  1. Match photon and transition energy

    Method

    Δ E = hc/λ.

    Reason

    An allowed transition emits or absorbs one photon with the matching energy.

    Working

    λ = hc/(Δ E)
  2. Evaluate

    Method

    λ = 620 nm.

    Reason

    The supplied hc unit returns wavelength in nanometres.

    Working

    λ = 1240/2.0 nm = 620 nm

Common misconception 3

Photon energy from wavelength (SI units)

Find and correct the mistake

Learner claim

Hydrogen emits a red line of wavelength 656 nm. A learner substitutes 656 directly into Δ E = hc/λ while using SI values of h and c. Diagnose the error and find the photon energy. Take h = 6.63 × 10⁻³⁴ J s and c = 3.00 × 10⁸ m s⁻¹.

Try this before viewing the solution

Unit: J

View solution step by step
  1. Repair the wavelength unit

    Method

    656 nm = 656 × 10⁻⁹ m.

    Reason

    SI values for h and c require wavelength in metres.

    Working

    λ = 6.56 × 10⁻⁷ m
  2. Calculate photon energy

    Method

    Δ E = 3.03 × 10⁻¹⁹ J.

    Reason

    The energy of the emitted photon equals the downward level difference.

    Working

    Δ E = ((6.63 × 10⁻³⁴)(3.00 × 10⁸))/(656 × 10⁻⁹) = 3.03 × 10⁻¹⁹ J

Examiner practice 4

Frequency from transition energy

2 marks

Examination question

An atom emits a photon of energy Δ E = 3.0 × 10⁻¹⁹ J. Find the photon frequency. Take h = 6.63 × 10⁻³⁴ J s. [2 marks]

Try this before viewing the solution

View solution step by step
  1. Use photon energy

    1 mark

    Method

    f = Δ E/h.

    Reason

    The emitted photon carries the transition energy.

    Working

    f = (3.0 × 10⁻¹⁹)/(6.63 × 10⁻³⁴)
  2. Evaluate

    1 mark

    Method

    f = 4.5 × 10¹⁴ Hz.

    Reason

    Energy divided by J s gives s⁻¹.

    Working

    f = 4.5 × 10¹⁴ Hz

Challenge 5

Which photons can be absorbed? (energy levels)

Minimal support

Independent transfer

An atom has energy levels at 0 eV, 2.0 eV and 3.5 eV. The atom is initially in the ground state. Determine which photon wavelengths it can absorb. Use hc = 1240 eV nm.

Try this before viewing the solution

Hints

Hint 1: start from the occupied level
Only upward transitions beginning at the stated initial level are available.
View solution step by step
  1. Select allowed gaps

    Method

    The available upward gaps are 2.0 eV and 3.5 eV.

    Reason

    The atom begins at 0 eV; the 2.0 → 3.5 eV gap is not initially accessible.

    Working

    0 → 2.0 eV and 0 → 3.5 eV
  2. Convert the first gap

    Method

    The 2.0 eV gap absorbs 620 nm photons.

    Reason

    Photon energy must match the gap exactly in the idealised isolated-atom model.

    Working

    λ = 1240/2.0 = 620 nm
  3. Convert the second gap

    Method

    The 3.5 eV gap absorbs 354 nm photons.

    Reason

    The larger energy gap corresponds to the shorter wavelength.

    Working

    λ = 1240/3.5 = 354 nm

7. Mind Stretchers

Mind stretcher 1: Why low pressure helps line spectraExtension

Suggest why low-pressure gases give sharper line spectra than high-pressure gases.

Show Answer

At low pressure, atoms collide less often, so emitted/absorbed photons are less disturbed and lines are sharper.

At higher pressure, frequent collisions broaden and smear the lines.

Mind stretcher 2: Why do emission and absorption lines “match”?Extension

Explain why the wavelengths of emission lines for a gas match the wavelengths of the dark absorption lines for the same gas.

Show Answer

Both processes involve the same discrete energy gaps between atomic levels.

Emission occurs when electrons drop and emit photons of energy Δ E, while absorption occurs when electrons rise by absorbing photons of the same Δ E, so the same photon wavelengths appear.

Continue with the next resource in this course.

Course and syllabus information
Course
GCE A-Level H2 Physics
Edition
GCE A-Level H2 Physics 2027