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Superposition

A-Level Physics 9702 · Topic 8 revision notes · AS

What happens when waves meet: stationary waves, diffraction, two-source interference, the double slit and the diffraction grating.

18 definitions to learn word for word, 12 equations in their own column, 12 diagrams and graphs. Read it, cover it, test yourself.

  1. 8.1a Superposition and stationary waves
  2. 8.1b Stationary waves on strings, in air columns and with microwaves
  3. 8.2 Diffraction
  4. 8.3a Interference and coherence
  5. 8.3b The double-slit experiment
  6. 8.4 The diffraction grating
Definitions (mark-scheme wording)EquationsExam traps

8.1aSuperposition and stationary waves

Definitions

Principle of superposition
when two or more waves meet at a point, the resultant displacement is the sum of the displacements of the individual waves.
Stationary wave
the wave formed when two progressive waves of the same frequency (and similar amplitude) travelling in opposite directions superpose; no energy is transferred.
Node
a point on a stationary wave where the amplitude is always zero.
Antinode
a point on a stationary wave where the amplitude is a maximum.

Key points

  • Usually formed by a wave and its reflection travelling back along the same path.
  • Adjacent nodes (or antinodes) are λ/2 apart; node to adjacent antinode is λ/4.
  • All points between two adjacent nodes are in phase; points in adjacent loops are 180° out of phase.
  • Amplitude varies with position (zero at nodes); in a progressive wave every point has the same amplitude.
  • A stationary wave stores energy; a progressive wave transfers energy.
  • Wavelength of the stationary wave = wavelength of the two progressive waves that make it.
λ/2 NNN A A amplitude varies along the string
Stationary wave between fixed ends: solid and dashed shapes are half a period apart. Nodes N never move; antinodes A swing fully.
PQR nodes every λ/2 P and Q: in phase R: 180° out of phase with P
Phase in a stationary wave: P and Q (same loop) move in phase; R (next loop) is 180° out of phase with them.

Watch out!

  • Adjacent nodes are λ/2 apart, not λ. Three nodes on a string span one whole wavelength.
  • Points in the same loop are in phase even though their amplitudes differ.

8.1bStationary waves on strings, in air columns and with microwaves

Definitions

Fundamental (first harmonic)
the stationary wave of lowest frequency that can form on the string or in the air column.
Harmonic
a stationary wave mode whose frequency is a whole-number multiple of the fundamental frequency.
End correction
the small distance beyond the open end of a tube at which the antinode actually forms.

Key points

  • String fixed at both ends: nodes at both ends. Fundamental L = λ/2; then L = λ, 3λ/2 ...
  • String apparatus: vibration generator, string over a pulley, hanging masses; change f until loops appear.
  • Tube closed at one end: node at the closed end, antinode at the open end. Fundamental L = λ/4.
  • Tube open at both ends: antinodes at both ends. Fundamental L = λ/2.
  • Resonance tube: two successive resonance lengths differ by λ/2; subtracting cancels the end correction.
  • Microwaves: transmitter faces a metal plate; move a probe along the line. Adjacent minima (nodes) are λ/2 apart.
  • Measure across many nodes and divide, to reduce the percentage uncertainty.
vibrationgenerator masses pulley L = 3λ/2
Stationary waves on a string: the vibration generator sets f; the hanging masses set the tension. Here three loops, so L = 3λ/2.
NA closed: L = λ/4 ANA open: L = λ/2 fundamental modes
Air columns (displacement envelopes): closed end = node, open end = antinode.
T transmitter metal plate probe at a node move probe λ (two node gaps)
Microwaves reflected from a metal plate form a stationary wave; the probe finds nodes λ/2 apart.

Watch out!

  • A closed tube has only odd harmonics (L = λ/4, 3λ/4 ...); an open tube has all of them.
  • The first resonance length alone gives λ/4 plus the end correction; use the difference of two lengths.

8.2Diffraction

Definitions

Diffraction
the spreading of a wave as it passes through a gap or around the edge of an obstacle.

Key points

  • Spreading is greatest when the gap width is similar to the wavelength.
  • Gap much wider than λ: waves pass almost straight through, with slight spreading at the edges.
  • Wavelength, frequency and speed are unchanged by diffraction; only the direction of travel spreads.
  • Shown in a ripple tank: plane waves through a barrier gap become curved.
  • Sound (λ ~ 1 m) diffracts round doorways; light (λ ~ 5 × 10-7 m) needs a very narrow slit.
  • Diffraction at each slit is what lets waves from two slits overlap and interfere.
gap >> λ gap ≈ λ little spreading maximum spreading
Ripple tank: a wide gap barely spreads the waves; a gap about one wavelength wide spreads them into semicircles. Wavefront spacing (λ) is unchanged.

Watch out!

  • A narrower gap spreads the wave more, not less (down to a gap about λ wide).
  • Do not draw a change in wavefront spacing after the gap: λ stays the same.

8.3aInterference and coherence

Definitions

Interference
the superposition of waves from two (or more) coherent sources to give regions of maximum and minimum amplitude.
Coherent
having a constant phase difference (so the waves have the same frequency).
Path difference
the difference in the distances travelled by two waves from their sources to a point.
Constructive interference
waves arrive in phase and superpose to give maximum amplitude.
Destructive interference
waves arrive in antiphase (180° out of phase) and superpose to give minimum amplitude.

Key points

  • A steady, observable pattern needs coherent sources; similar amplitudes give clear minima.
  • For in-phase sources: maximum where path difference = nλ; minimum where it is (n + ½)λ.
  • Equivalent phase differences: 0, 360° ... for a maximum; 180°, 540° ... for a minimum.
  • Complete cancellation only if the two amplitudes at that point are equal.
  • Demonstrations: ripple tank with two dippers on one bar; two loudspeakers on one signal generator; microwaves through two slits.
  • Two separate lamps are not coherent (random phase changes); use one laser, or one source and a double slit.
S₁S₂ n = 0 n = 1 n = 1 max: nλ
Two coherent sources in a ripple tank: crests (arcs) cross along lines of maximum (red, n = 0, 1); minima lie between them.
constructive both waves (same) sum: 2A destructive antiphase waves sum: zero
In phase: amplitudes add (maximum). In antiphase with equal amplitude: they cancel (minimum).

Watch out!

  • Coherent means constant phase difference, not necessarily zero phase difference.
  • If the sources are in antiphase the conditions swap: nλ gives a minimum.

8.3bThe double-slit experiment

Definitions

Fringe separation (x)
the distance between the centres of adjacent bright (or adjacent dark) fringes.
Slit separation (a)
the distance between the centres of the two slits.

Key points

  • Monochromatic light (e.g. a laser) through two narrow, close slits gives equally spaced bright and dark fringes.
  • The slits act as coherent sources: both are lit by the same wavefront; diffraction makes their light overlap.
  • Bright fringe: path difference nλ. Dark fringe: path difference (n + ½)λ.
  • Fringe spacing x increases with λ and D, and decreases as a increases.
  • Valid when a << D (small angles). Typical: a ~ 0.5 mm, D ~ 1-2 m, x ~ a few mm.
  • Measure across many fringes and divide to reduce percentage uncertainty in x.
  • White light: central fringe white; others are coloured spectra with violet nearest the centre, red furthest.
double slit a screen x path diff. = nλ D
Double slit: light from the two slits reaches a bright fringe with path difference nλ; fringe spacing x = λD/a.
intensityposition x central max
Intensity across the screen: evenly spaced maxima, one fringe spacing x apart, fading slowly with distance from the centre.

Watch out!

  • x is the spacing between adjacent fringes: 10 fringe spacings measured together means divide by 10, not 11.
  • Keep units consistent: a and x often in mm, D in m. Convert all to metres.

8.4The diffraction grating

Definitions

Diffraction grating
a plate with a large number of parallel, equally spaced, very narrow slits (lines).
Grating spacing (d)
the distance between the centres of adjacent slits; d = 1/N, where N is the number of lines per metre.
Order (n)
the number of wavelengths of path difference between waves from adjacent slits at that maximum.

Key points

  • Many slits give maxima that are very sharp and bright, at large angles: more precise than the double slit.
  • Zero order (n = 0) goes straight through; orders appear symmetrically on either side.
  • Highest order: sin θ ≤ 1, so nmax = d/λ rounded down.
  • More lines per metre means smaller d, larger angles and fewer orders.
  • Measure the angle between the two order-n maxima on either side and halve it to get θ.
  • White light: zero order is white; each higher order is a spectrum, violet deviated least, red most; higher orders may overlap.
grating θ n = 0 n = 1n = 1 n = 2n = 2 laser
Grating orders: n = 0 straight through, symmetric orders either side at angles given by d sin θ = nλ.
θ d sin θ d to order n maximum when d sin θ = nλ
Why d sin θ = nλ: waves from adjacent slits at angle θ differ in path by d sin θ; a maximum needs this to be a whole number of wavelengths.

Watch out!

  • "500 lines per mm" means N = 5 × 105 m-1, so d = 2 × 10-6 m. Convert to per metre before inverting.
  • nmax is rounded down: d/λ = 3.8 means 3 orders each side (7 maxima in total).
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