Interference

Section: Superposition  |  Syllabus: Cambridge AS Level Physics (9702)

What is Interference?

When two or more waves overlap in the same region of space, they combine according to the principle of superposition. The resulting pattern of reinforcement and cancellation is called interference.

Interference The phenomenon that occurs when two or more waves superpose to produce a resultant wave with a displacement that is the sum of the individual displacements.

Interference can result in:

Coherence

For a stable, observable interference pattern, the wave sources must be coherent.

Coherence Two wave sources are coherent if they have: (1) the same waveform, (2) the same frequency (or wavelength), and (3) a constant phase difference. For electromagnetic waves, they must also be polarised in the same plane. Why Coherence Matters

Non-coherent sources have randomly varying phase differences. The interference pattern shifts rapidly and averages out-no stable pattern is observed. Coherent sources maintain fixed positions of maxima and minima.

Achieving Coherent Light Sources

Exam Insight

Two independent light bulbs are NOT coherent-they emit light with random phase variations. Only sources derived from a single source, or laser light, can produce stable interference patterns.

Constructive and Destructive Interference

Constructive Interference

Constructive interference occurs when two waves arrive in phase at a point. The crests of one wave align with the crests of the other.

Conditions for Constructive Interference:

Path difference = nλ (where n = 0, 1, 2, 3, ...)

Phase difference = 0, 2π, 4π, ... (or 0°, 360°, 720°, ...)

Result: Maximum amplitude = sum of individual amplitudes

Destructive Interference

Destructive interference occurs when two waves arrive in antiphase at a point. The crests of one wave align with the troughs of the other.

Conditions for Destructive Interference:

Path difference = (n + (1/2))λ (where n = 0, 1, 2, 3, ...)

i.e., (λ/2), (3λ/2), (5λ/2), ...

Phase difference = π, 3π, 5π, ... (or 180°, 540°, 900°, ...)

Result: Minimum amplitude Complete Cancellation

Complete destructive interference (zero resultant amplitude) only occurs when the two interfering waves have identical amplitudes. If the amplitudes are different, the resultant will be the difference of the amplitudes.

Path Difference and Phase Difference

The path difference is the difference in distance travelled by two waves from their sources to a point. The phase difference at that point depends on the path difference.

Relationship:

Phase difference = (2π/λ) × path difference

or in degrees: Phase difference = (360°/λ) × path difference

Amplitude and Intensity

The intensity of a wave is proportional to the square of its amplitude.

I ∝ A^2

where I = intensity and A = amplitude

For two identical waves of amplitude A:

Conditions for Observable Interference Fringes

To observe a clear two-source interference pattern, the following conditions must be met:

  1. The sources must be coherent (same frequency, constant phase difference)
  2. The sources should have approximately equal amplitudes (for clear dark fringes)
  3. For transverse waves, the waves must be polarised in the same plane (or unpolarised)
  4. The sources must be close together relative to the distance to the screen (for resolvable fringes with light)

Two-Source Interference Experiments

1. Water Waves in a Ripple Tank

Two dippers oscillating in phase (driven by same motor) create circular waves that overlap.

FIG 8.15: Two-Source Interference in Ripple Tank

Show: two point sources (dippers) producing circular wavefronts. Mark: lines of constructive interference (where crests meet crests) radiating outward as solid lines, lines of destructive interference (where crests meet troughs) as dashed lines. Label maxima and minima regions. Show the characteristic pattern of alternating maximum and minimum amplitude lines.

Observations:

2. Sound Waves from Two Loudspeakers

Two loudspeakers connected with same polarity to same signal generator produce coherent sound waves.

Observations:

3. Microwaves

One transmitter with double slit creates two coherent secondary sources.

FIG 8.16: Microwave Double-Slit Interference

Show: microwave transmitter → double slit in metal barrier → two coherent sources → receiver/detector that can be moved perpendicular to the wave direction. Show regions of maxima and minima. Include connection to amplifier/loudspeaker for detection.

Observations:

4. Light: Young's Double-Slit Experiment

Crucial evidence for wave nature of light (Thomas Young, 1803).

FIG 8.17: Young's Double-Slit Setup

Show: monochromatic light source → single slit S (to create coherence) → double slits S₁ and S₂ (separation a) → screen at distance D. Show wavefronts from S₁ and S₂ overlapping. On screen, show alternating bright and dark fringes with fringe separation x marked. Include path difference illustration showing paths from S₁ and S₂ to a point on screen.

FIG 8.18: Double-Slit Fringe Pattern

Show intensity distribution: equally-spaced bright fringes with dark fringes between. Below, show intensity vs position graph with regular maxima and minima. Mark central maximum (path difference = 0), and label fringe separation x.

Observations:

Young's Double-Slit Equation

The fringe spacing relates to wavelength, slit separation, and screen distance.

FIG 8.19: Derivation of Young's Equation

Show geometry: two slits S₁ and S₂ separated by distance a, screen at distance D. Two paths from slits to point P on screen (at distance y from centre). Show similar triangles: path difference z relates to a and D, fringe spacing x relates to D. Derivation uses: z/a ≈ y/D and for adjacent bright fringes, z = λ, y = x, giving λ = ax/D.

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