Polarisation
Key idea: Explain what polarisation is, why it only occurs for transverse waves, and how polarisers affect intensity (A Level Physics).
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The core idea
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Learning objectives
- Explain polarisation and apply Malus’ law to amplitude and intensity.
1. Definitions (Must Know)
A. Polarisation
Polarisation is the restriction of a wave’s oscillations to one plane.
B. Plane-polarised wave
A plane-polarised wave is a transverse wave whose oscillations are in a single plane.
C. Unpolarised wave
An unpolarised wave has oscillations in many planes (randomly distributed).
For light, “unpolarised” means the electric field direction varies rapidly and randomly.
D. Polariser / analyser (transmission axis)
A polariser (or analyser) has a transmission axis. It only transmits the component of a transverse wave along that axis.
2. Key Ideas (What Earns Marks)
- Polarisation is a phenomenon associated with transverse waves only.
- Showing that a wave can be polarised is evidence it is transverse.
- A polariser reduces transmitted intensity because it only passes one component of the oscillation.
- For unpolarised light passing through an ideal polariser: I = (1/2)I₀
- For plane-polarised light through a polariser at angle θ, use Malus’ law: I = I₀ cos² θ
Full calculation method: Malus’ Law.
3. Detailed Explanations
A. Why polarisation only applies to transverse waves
To “restrict oscillations to one plane”, the oscillation must be able to point in different directions perpendicular to the wave travel direction.
That is true for transverse waves.
For a longitudinal wave, oscillations are along the direction of travel, so there is no “plane of oscillation” to restrict.
B. How a polariser works (idea)
For light, the oscillation is the electric field vector E.
A polariser transmits only the component of vector E along its transmission axis. That reduces the amplitude and therefore the intensity.
C. How to test whether light is polarised
Place a second polariser (the analyser) after the first and rotate it.
- If the intensity changes with rotation, the light is polarised.
- If the intensity stays constant for all angles, the light is unpolarised (or the setup is not sensitive enough).
4. Common Mistakes
- Mixing up unpolarised with “weak” (unpolarised can still be intense).
- Saying “all laser light is perfectly plane-polarised” (some lasers are strongly polarised, but it depends on the laser and optics).
- Claiming longitudinal waves can be polarised.
5. Exam Tips
- Use the exact phrase: “polarisation is a phenomenon associated with transverse waves”.
- If the question gives angles between polarisers, it is usually a Malus’ law question.
- If the question is qualitative, focus on “component along the transmission axis”.
6. Worked Examples
Modelled example 1
Why polarisation implies a transverse wave
Problem
Study the worked solution
State what polarisation does
Method
Polarisation restricts oscillations to one plane.Reason
A selectable plane requires more than one possible oscillation direction.Working
many transverse directions → one planeConnect to transverse waves
Method
A transverse oscillation is perpendicular to propagation and can have different orientations in that perpendicular plane.Reason
A polariser can therefore select one component.Working
oscillation ⊥ propagationExclude longitudinal waves
Method
A longitudinal wave cannot be polarised in this way.Reason
Its oscillation is fixed along the propagation direction, leaving no transverse plane to select.Working
longitudinal: oscillation ∥ propagation
Guided practice 2
Unpolarised light through one polariser
Problem
Try this before viewing the solution
Hints
Hint 1: distinguish unpolarised input
View solution step by step
Average over input directions
Method
The ideal polariser transmits half the incident intensity.Reason
Unpolarised light has rapidly varying transverse directions whose mean squared projection on any fixed axis is one half.Working
I = (1/2)I₀State the output state
Method
The transmitted light is plane-polarised along the transmission axis.Reason
Only that field component passes.Working
output direction = polariser axis
Common misconception 3
Two polarisers at 90°
Learner claim
Try this before viewing the solution
View solution step by step
Reject repeated averaging
Method
The half-intensity rule is not applied again to plane-polarised light.Reason
The second analyser sees a definite polarisation direction, not random directions.Working
known direction → Malus’ lawUse the relative angle
Method
The analyser axis is 90° from the incident polarisation.Reason
Crossed axes have no transmitted field component along the second axis.Working
cos 90° = 0Find intensity
Method
The ideal final intensity is zero.Reason
Intensity follows the squared field projection.Working
I = I₀ cos² 90° = 0
Examiner practice 4
Unpolarised light through two polarisers
Examination question
Try this before viewing the solution
View solution step by step
Treat the unpolarised input
1 markMethod
The first polariser transmits I₁ = I₀/2.Reason
It averages the squared projections of random input directions.Working
I₁ = (1/2)I₀Set the analyser angle
1 markMethod
The plane-polarised input to the analyser is at 60° to its axis.Reason
Angles for Malus’ law are measured between polarisation and transmission directions.Working
θ = 60°Apply Malus' law
1 markMethod
I₂ = I₁ cos² 60°.Reason
Intensity is proportional to the square of the transmitted field component.Working
I₂ = (I₀/2)(0.50)²Simplify
1 markMethod
The final intensity is I₀/8.Reason
One half multiplied by one quarter is one eighth.Working
I₂ = (1/8)I₀
Self-mark with the mark scheme
Compare your response with each mark point. Select a point only when your response contains that evidence.
Self-mark the half rule, relative angle, Malus relation and final fraction.
Challenge 5
Three polarisers (step-by-step)
Independent transfer
Try this before viewing the solution
Hints
Hint 1: use successive relative angles
View solution step by step
Pass the first polariser
Method
I₁ = I₀/2.Reason
The incident light is unpolarised.Working
I₁ = (1/2)I₀Pass the second polariser
Method
I₂ = 3I₀/8.Reason
The second axis is 30° from the current polarisation direction.Working
I₂ = (I₀/2) cos² 30° = (3/8)I₀Use the final relative angle
Method
The last angle is 60°, giving I₃ = 3I₀/32.Reason
After the second polariser, the light is polarised at 30°, so compare 90° with that direction.Working
I₃ = (3I₀/8) cos² 60° = (3/32)I₀
7. Mind Stretchers
Mind stretcher 1: Adding a third polariserExtension
Two polarisers are crossed (90° apart), so no light is transmitted.
Explain qualitatively why inserting a third polariser at 45° between them allows some light through.
Show Answer
The middle polariser changes the polarisation direction step-by-step: the first polariser sets one direction, the middle one transmits the component along 45°, and the final one transmits the component of that along its axis. Because the “rotation” happens in two stages, the final transmitted intensity is not zero.
Mind stretcher 2: Combining the “half” rule with Malus’ lawExtension
Show that unpolarised light of intensity I₀ passing through a polariser, then an analyser at angle θ, has final intensity I = 1/2 I₀ cos² θ.
Show Answer
After the first polariser, unpolarised light transmits with half intensity: I₁ = 1/2 I₀ After the analyser at angle θ: I = I₁ cos² θ = (1/2 I₀) cos² θ
Mind stretcher 3: Optional (Enrichment)Extension
A. Polarisation by reflection (glare)
Reflected light from a surface can be partially polarised, which is why some sunglasses reduce glare. This typically goes beyond what most exam questions require unless explicitly mentioned.
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Course and syllabus information
- Course
- GCE A-Level H2 Physics
- Edition
- GCE A-Level H2 Physics 2027