Two-point source interference
The set-up
- Two-point source interference happens when two sources send out waves that overlap.
- For a steady, observable pattern the two sources must be coherent:
- the same frequency (and therefore the same wavelength),
- a constant phase relationship — usually "in phase", meaning they produce crests at the same instant.
- In the laboratory this is done with two dippers driven by the same motor in a ripple tank, or two loudspeakers driven by one signal generator.
Constructive and destructive interference
The pattern is just superposition applied continuously at every point:
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Constructive interference — the two waves arrive in phase (crest meets crest, or trough meets trough).
- The displacements add, giving a large amplitude.
- For water: large waves. For sound: loud. For light: bright.
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Destructive interference — the two waves arrive completely out of phase (crest meets trough).
- The displacements subtract, giving a small or zero amplitude.
- For water: flat water. For sound: quiet. For light: dark.
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Which happens at a point depends on the path difference — how much further one wave has travelled than the other:
- paths differing by a whole number of wavelengths → the waves are back in step → constructive,
- paths differing by a half number of wavelengths (, , …) → the waves are exactly out of step → destructive.
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At Level 2 you explain this qualitatively — you are not asked to calculate fringe spacings.
The pattern that results
- The regions of constructive and destructive interference are not scattered — they form lines radiating outward from between the two sources.
- Antinodal lines — lines of constructive interference (large amplitude).
- Nodal lines — lines of destructive interference (little or no amplitude).
- They alternate: antinodal, nodal, antinodal, and so on out to each side.
- The central line, exactly midway between the two sources, is always antinodal.
- Every point on it is equidistant from both sources, so the path difference is zero — the waves always arrive in phase there.
Move the two sources and change the wavelength below, and watch the nodal and antinodal lines shift:
Path difference = 0.53 λ → destructive (dark)
Drag the detector.
How the pattern changes
Two changes are examined repeatedly:
- Increasing the wavelength (equivalently, lowering the frequency):
- the lines spread further apart,
- fewer lines fit into the same region.
- Increasing the separation of the sources:
- the lines are squeezed closer together,
- more lines fit into the same region.
- Stated as one rule: the spacing of the pattern grows with wavelength and shrinks with source separation.
- Changing the amplitude of the sources changes how strong the effect is, but not where the nodal and antinodal lines lie.
What interference is not
- It is not waves cancelling energy out of existence. Energy is redistributed — removed from the nodal lines and concentrated on the antinodal lines. Total energy is unchanged.
- It is not the same as diffraction, though the two often appear together. Diffraction is one wave spreading through a gap; interference is two waves overlapping.
Worked ExampleExplaining a point on a nodal line
Two loudspeakers, driven by the same signal generator at a single frequency, face an open field. A student walks across the field in front of them and finds alternating loud and quiet positions. At one quiet point, the distance to one speaker is m and to the other is m. The sound has a wavelength of m. Explain why this point is quiet.
Step 1 — Find the path difference
Step 2 — Compare it with the wavelength
The path difference is two and a half wavelengths.
Step 3 — Interpret
A path difference of a half number of wavelengths means one wave has travelled exactly half a cycle further than the other, so a crest from one speaker arrives at the same moment as a trough from the other. The waves are completely out of phase.
By the principle of superposition their displacements subtract, and since the two speakers are identical the amplitudes are nearly equal, so they almost completely cancel. The point lies on a nodal line and the sound is quiet.