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Astronomy and Cosmology

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  Cambridge International AS & A Level Physics (9702)

Astronomy and Cosmology

The big idea: Starlight tells us how far, how hot and how big. Standard candles give distance, Wien and Stefan–Boltzmann give temperature and radius, and redshift plus Hubble’s law point back to a Big Bang.

Summary — What This Chapter Covers
  • Luminosity L: total power of radiation emitted by a star. Radiant flux intensity F = L/(4πd2).
  • A standard candle is an object of known luminosity; measuring F then gives d.
  • Wien's law λmax ∝ 1/T; Stefan–Boltzmann L = 4πσr2T4; together they give stellar radii.
  • Redshift Δλ/λ ≈ Δf/f ≈ v/c; distant galaxies are receding.
  • Hubble's law v ≈ H0d implies an expanding Universe that began in a Big Bang.
1. Standard Candles
25.1

Known luminosity, measured flux

The luminosity L of a star is the total power of radiation it emits (W). The radiation spreads over a sphere of area 4πd2, so the radiant flux intensity F (power per unit area received, W m−2) falls with the inverse square of distance.

A standard candle is an object whose luminosity is known. Measure F from Earth, and d follows from the inverse square law. Cepheid variable stars (whose luminosity is linked to their pulsation period) work for nearby galaxies; type Ia supernovae, which all peak at about the same luminosity and are extremely bright, reach far more distant galaxies.

Inverse square law F = L/(4πd2)    d = √(L/(4πF))
Worked Example

A Cepheid in a distant galaxy has luminosity 3.0 × 1030 W and a measured radiant flux intensity of 2.5 × 10−12 W m−2. Find the distance to the galaxy.

Practice Question

The Sun’s luminosity is 3.83 × 1026 W and it is 1.50 × 1011 m away. Find the radiant flux intensity at Earth.

2. Stellar Radii
25.2

Wien and Stefan–Boltzmann

A star radiates approximately like a black body. Wien’s displacement law: the wavelength at which the emitted intensity peaks is inversely proportional to the thermodynamic surface temperature, λmax ∝ 1/T (λmaxT = constant, about 2.9 × 10−3 m K; questions give the constant or a reference star). Hotter stars peak at shorter wavelengths and look bluer.

The Stefan–Boltzmann law gives the luminosity from the surface area and temperature, L = 4πσr2T4, with σ = 5.67 × 10−8 W m−2 K−4. Find T from the spectrum (Wien), L from a standard-candle or distance measurement, then solve for r.

Black-body laws λmax ∝ 1/T    L = 4πσr2T4
Worked Example

A star’s spectrum peaks at 290 nm and its luminosity is 4.0 × 1028 W. Take λmaxT = 2.9 × 10−3 m K. Find its surface temperature and radius.

Practice Question

Star X has the same surface temperature as star Y but four times its luminosity. Compare their radii.

3. Hubble's Law and the Big Bang Theory
25.3

Redshift and expansion

longer wavelengths redshifted

Hubble’s law 0 Big Bang 0 0 −1

Redshift and Hubble Δλ/λ ≈ Δf/f ≈ v/c    v ≈ H0d    age ≈ 1/H0
Worked Example

0 −18 −1

Practice Question

Estimate the age of the Universe from H0 = 2.2 × 10−18 s−1.

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