Superposition & Interference
- Apply the principle of superposition to overlapping waves
- Use path difference to distinguish constructive from destructive interference
- Relate the double-slit condition to bright and dark fringes
Superposition and interference
When two waves overlap, their displacements simply add — the principle of superposition. Where two crests meet, they reinforce into a bigger crest: constructive interference. Where a crest meets a trough, they cancel: destructive interference. For a stable pattern the waves must be coherent (same frequency and a fixed phase relationship). Interference is the signature behavior of waves — particles do not add and cancel this way, so an interference pattern is proof you are dealing with a wave.
Path difference decides the outcome
What determines constructive versus destructive interference at a point is the path difference — how much farther one wave traveled than the other to reach it. If the path difference is a whole number of wavelengths (0, λ, 2λ, …), the waves arrive in phase and interfere constructively (bright/loud). If it is a half-integer number of wavelengths (½λ, 1½λ, …), they arrive out of phase and interfere destructively (dark/silent). In Young’s double-slit experiment, this produces alternating bright and dark fringes on a screen.
In a double-slit experiment, the slit separation is d = 0.10 mm and light of wavelength λ = 500 nm is used. Find sinθ for the first-order (m = 1) bright fringe.
- 1.Bright-fringe condition: d sinθ = mλ, so sinθ = mλ/d.
- 2.Convert units: d = 0.10 mm = 1.0 × 10⁻⁴ m, λ = 500 nm = 5.0 × 10⁻⁷ m.
- 3.Substitute (m = 1): sinθ = (5.0 × 10⁻⁷) / (1.0 × 10⁻⁴).
- 4.Divide: sinθ = 5.0 × 10⁻³ = 0.0050.
Two coherent waves arrive at a point with a path difference of exactly one full wavelength. The interference there is:
Translate path difference into wavelengths: whole numbers (0, 1λ, 2λ) give bright/constructive, half-numbers (½λ, 1½λ) give dark/destructive. Counting in units of λ is faster and less error-prone than working in meters.
In a double-slit experiment, d = 0.10 mm and λ = 500 nm. For the first-order bright fringe (m = 1), what is sinθ?
Convert everything to meters before using d sinθ = mλ: millimeters are 10⁻³ and nanometers are 10⁻⁹. A power-of-ten error here is the most common way to lose the double-slit point.
Answer the 2 checkpoints as you read.
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