Wave Properties
Frequency, wavelength, amplitude, phase, wave speed, transverse vs longitudinal waves, and the Doppler effect.
Wave mechanics, interference, diffraction, polarisation, and geometrical optics — from sound to light to quantum probability waves.
Waves are periodic disturbances that transport energy without transporting matter. They appear throughout physics: mechanical waves in strings and air, electromagnetic waves (light, radio, X-rays), seismic waves, and quantum probability waves. Optics applies wave principles specifically to light, covering both the wave (physical optics) and ray (geometrical optics) descriptions.
The one-dimensional wave equation ∂²y/∂t² = v²∂²y/∂x² has sinusoidal solutions y(x,t) = A sin(kx − ωt + φ), where k = 2π/λ is the wave number, ω = 2π/T is the angular frequency, and v = ω/k is the phase velocity. The same equation governs sound, light, and — in a modified form — quantum wavefunctions.
Waves obey the superposition principle: the total displacement is the sum of individual displacements. When two coherent waves overlap, they interfere: constructively when in phase (path difference = nλ) and destructively when out of phase (path difference = (n+½)λ). Young's double-slit experiment is the paradigmatic demonstration of wave interference.
Waves bend around obstacles and spread through apertures — diffraction. The single-slit pattern has a central maximum of width 2λL/a. Diffraction gratings with many slits produce sharp bright fringes and are used in spectroscopy. Fraunhofer diffraction describes the far-field pattern; Fresnel diffraction handles the near-field.
When two identical waves travel in opposite directions, they superpose to form a standing wave with fixed nodes and antinodes. A string fixed at both ends supports standing waves at f_n = nv/2L. Resonance occurs when a driving frequency matches a natural frequency — the basis of musical instruments, microwave cavities, and laser resonators.
When wavelengths are much shorter than obstacles, light travels in straight rays. Snell's law n₁ sin θ₁ = n₂ sin θ₂ governs refraction. Total internal reflection occurs when θ > θ_c = arcsin(n₂/n₁) — exploited in optical fibres. Lenses and mirrors focus light via thin-lens equations: 1/f = 1/d_o + 1/d_i.
Frequency, wavelength, amplitude, phase, wave speed, transverse vs longitudinal waves, and the Doppler effect.
Interference, diffraction, standing waves, resonance, polarisation, and geometrical optics.
Fourier analysis of waves, coherence and lasers, nonlinear optics, and wave-particle duality.
Sound and light frequency shifts due to relative motion — from sirens to redshift.
Read →Nodes, antinodes, harmonics, and why guitar strings sing.
Read →Far-field and near-field diffraction patterns and their practical applications.
Read →Perfect polarisation by reflection and its use in photography and optics.
Read →Decomposing any periodic signal into sinusoids — the most useful tool in wave physics.
Read →Mach cones, shock waves, and the physics of supersonic flight.
Read →∂²y/∂t² = v² ∂²y/∂x². Solutions are sinusoids propagating at speed v. The same form describes sound, light, and quantum wavefunctions.
Constructive: waves in phase add amplitudes (path difference = nλ). Destructive: waves out of phase cancel (path difference = (n+½)λ).
Thin-film interference: light from the front and back film surfaces travels slightly different paths, causing certain wavelengths to interfere constructively.
The orientation of a transverse wave's oscillation. Polarising filters transmit one orientation; used in LCDs, sunglasses, and optical communications.