The Doppler effect & redshift
Motion towards the observer compresses wavelengths (blue shift); away, it stretches them (red shift).
A source moving relative to an observer changes the observed wavelength: towards → shorter λ (blue shift); away → longer λ (red shift). Only valid for v≪c.
Δλ = λ_lab − λ_obs Δf = f_lab − f_obs
Δf/f = −Δλ/λ = v/c = z
AQA's sign convention: both Δλ and Δf are calculated as (lab − observed), then linked by a minus sign — this keeps z>0 for receding objects and z<0 for approaching ones.
Worked example: the Sun's rotation
Comparing the wavelength shift on opposite limbs of the Sun gives its rotational speed via the Doppler equation; combining with ω=v/r and T=2π/ω then gives its rotational period.
Binary stars
As the stars orbit, spectral lines oscillate between red- and blue-shifted.
Two stars orbiting a common centre of mass. Radial velocity method: as one approaches (blue-shift) and the other recedes (red-shift), spectral lines split and oscillate — this is the only reliable way to measure stellar masses.
- Visual binaries: individually resolved by telescope.
- Spectroscopic binaries: too close to resolve — identified only via spectra/light curves.
- Transit (eclipsing) method: dips in total apparent magnitude as one star eclipses the other — a bigger dip occurs when the brighter star is eclipsed.
Exoplanets
Transit method: periodic dip in brightness as the planet crosses in front of the star.
- Transit method (~78% of discoveries): periodic brightness dip; the planet contributes no light of its own, so the curve shape differs slightly from an eclipsing binary. Best for short orbital periods; can detect Earth-sized planets.
- Radial velocity method: tiny periodic Doppler shift as the star wobbles under the planet's gravity — needs very sensitive spectrometers.
- Direct imaging: only feasible for large planets far from a bright parent star.