Interference and Diffraction
Interference and Diffraction — American System Physics Revision Notes & Topical Questions
5 min read 6 parts Lesson 1 of 5 1 quiz
Interference and Diffraction of Light — AMERICAN SYSTEM PHYSICS notes: Explain superposition, double-slit, thin-film, single-slit and grating patterns and use the related equations and the Rayleigh criterion.By the principle of superposition, overlapping waves add.
- Coherent sources
- fringe spacing
- Huygens' principle
- Worked example 1
- Worked example 2
- Worked example 3
Part 1 of 4Superposition and double-slit interference
By the principle of superposition, overlapping waves add. Coherent sources emit waves of the same frequency and wavelength with a constant phase difference, needed for a stable pattern; lasers provide coherent light.
| Feature | Constructive | Destructive |
|---|---|---|
| Phase relation | in phase (0°, 360° ...) | antiphase (180°) |
| Path difference | 0, λ, 2λ ... = mλ | ½λ, 1½λ ... = (m + ½)λ |
| Resultant amplitude | sum (maximum) | difference (zero if equal) |
| Light | bright fringe | dark fringe |
| Sound | loud | quiet |
Thin film
- when the film index is higher than its surroundings, reflection is bright when 2t = (m + ½)λfilm, where λfilm = λ/n;
- there is a phase change of ½λ on reflection from a higher-index medium.
- Holograms rely on interference.
Part 2 of 4Diffraction at a single slit and resolution
Diffraction is the spreading of waves as they pass through a gap (aperture, width w) or around an edge; dust on lenses can produce diffraction patterns, and diffraction shows light is a wave. Huygens' principle: every point on a wavefront is a source of secondary wavelets, and the new wavefront is the surface tangent to all of them.
Diffraction limits resolution. By the Rayleigh criterion, two point sources are just resolved when the central maximum of one pattern falls on the first minimum of the other; for a circular aperture of diameter D, θ = 1.22λ/D. Resolving power is the ability to distinguish two close objects. A ripple tank can demonstrate wave diffraction.
Part 3 of 4Diffraction gratings
A grating works like many slits at once.
- giving the condition d sin θ = mλ and very sharp, bright maxima.
Part 4 of 4Worked examples
Laser light passes through two slits 0.20 mm apart. Fringes on a screen 3.0 m away are 9.5 mm apart. Calculate the wavelength. [3]3 marks
λ = xd/L = (9.5 × 10−3 × 0.20 × 10−3)/3.0 = 6.3 × 10−7 m (633 nm, red).
Green light (λ = 5.4 × 10−7 m) passes through slits 0.30 mm apart. Find the fringe spacing on a screen 2.5 m away. [3]3 marks
x = λL/d = (5.4 × 10−7 × 2.5)/(0.30 × 10−3) = 4.5 × 10−3 m (4.5 mm).
Two coherent speakers emit sound of wavelength 0.68 m. At P the path difference is 1.02 m. Is P loud or quiet? [2]2 marks
1.02/0.68 = 1.5 wavelengths, an odd number of half-wavelengths, so destructive interference: P is quiet.
A single slit (w = 0.12 mm) is lit with 600 nm light and the screen is 2.0 m away. How wide is the central maximum? [3]3 marks
x1 = λL/w = 600 × 10−9 × 2.0/0.12 × 10−3 = 1.0 × 10−2 m. Width = 2x1 = 2.0 cm.
A telescope has aperture 0.10 m. Find the smallest angle it resolves for 550 nm light. [2]2 marks
θ = 1.22λ/D = 1.22 × 550 × 10−9/0.10 = 6.7 × 10−6 rad.
A grating has 400 lines per mm. Find its spacing d. For a grating with d = 2.0 × 10−6 m and λ = 6.0 × 10−7 m, what is the highest visible order? [3]3 marks
N = 4.0 × 105 m−1, so d = 1/N = 2.5 × 10−6 m. For the second grating d/λ = 3.33, so the highest order is 3.
Key terms
| Term | Meaning |
|---|---|
| Coherent sources | Sources with the same frequency and a constant phase difference. |
| Fringe spacing | Distance between centres of adjacent bright (or dark) fringes. |
| Huygens' principle | Every point on a wavefront is a source of secondary wavelets; the new wavefront is tangent to them. |
| Rayleigh criterion | Two sources are just resolved when one central maximum falls on the other's first minimum; θ = 1.22λ/D. |
| Grating spacing (d) | Distance between adjacent slits, d = 1/(lines per metre). |
| Emission line spectrum | Bright lines at specific wavelengths from a hot, low-pressure gas, characteristic of the element. |
| Polarization | Restriction of a transverse wave's vibrations to one plane. |
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