1. What happens to peak wavelength when blackbody temperature doubles?
- It doubles.
- It remains fixed.
- It halves.
Check the answer and reasoning
It halves.
Wien’s law holds λmax T constant.
Physics / A2 level
Infer stellar properties and cosmic expansion from light.
Luminosity is total radiated power; observed flux is power per unit detector area. Distance changes flux without necessarily changing luminosity. A blackbody approximation connects stellar spectra and power to surface temperature and radius.
At sufficiently low cosmological redshift, recession speed is approximately proportional to distance. Cosmic microwave background radiation is further evidence for cosmic evolution. An age estimated from an expansion rate depends on assumptions about expansion history.
Luminosity is a star’s total radiated power; flux is received power per unit area. For an isotropic source without intervening absorption, F = L/(4πd²). Moving a detector twice as far away reduces flux to one quarter while luminosity is unchanged. A faint star can therefore be intrinsically faint, very distant or affected by absorption; brightness alone does not uniquely establish its distance.
A blackbody approximation gives λmax T = b and L = 4πR²σT⁴ for a spherical star. Hotter surfaces have shorter peak wavelengths. If temperature and luminosity are known, the second relation can estimate radius. The peak depends on which spectral representation is plotted, so the familiar wavelength-form Wien constant must match the graph used. Real stellar atmospheres introduce lines and deviations from a perfect blackbody.
Compare an identified spectral line with its reference wavelength: z = (λobserved − λemitted)/λemitted. At sufficiently low cosmological redshift, recession speed can be approximated by cz and related to distance through v ≈ H₀d. This local approximation must not be applied blindly at large redshift. Calibration and the methods used to infer distance matter when interpreting a graph of recession speed against distance.
The cosmic microwave background has a nearly thermal spectrum and arrives from essentially every direction. It is evidence for a hot early Universe that became transparent and whose radiation subsequently stretched during expansion. An estimate of expansion age from 1/H₀ assumes an oversimplified expansion history. Gravitationally bound systems such as the Solar System do not simply expand according to the same large-scale distance law; distinguish local dynamics from cosmological expansion.
Neglecting absorption, the fainter star is three times as distant because received flux varies inversely with distance squared. Equal luminosity is essential to this comparison.
Flux from an isotropic source with no absorption.
Wien’s displacement law.
Blackbody luminosity of a spherical star.
Low-redshift Hubble relationship.
Use H₀ = 70 km/s/Mpc. What recession speed is predicted for a galaxy 100 Mpc away?
v ≈ 70 × 100 = 7000 km/s.
Find peak wavelength at two blackbody temperatures and compare λmax T, keeping plotting conventions consistent.
Use the spectrum model for temperature and orbital models for bound motion. None directly simulates cosmic expansion, stellar evolution or the microwave background, so connect those topics to observations and explicit models.
It halves.
Wien’s law holds λmax T constant.
7000 km/s
v ≈ 70 × 100 = 7000 km/s.
It becomes one quarter.
Flux decreases with distance squared.