Medical physics and astronomy (A Level)
25. Astronomy and Cosmology
5 min read 9 parts Lesson 22 of 22 Unit quiz
Lesson summary
25. Astronomy and Cosmology — Cambridge AS & A Level Physics 9702 — CAMBRIDGE AS & A LEVEL PHYSICS 9702 — COMPLETE NOTES notes: Use luminosity, standard candles, Wien's and Stefan–Boltzmann laws, redshift and Hubble's law to find distances, temperatures, radii and the age of the …
- Luminosity L
- Radiant flux F
- Difference
- Spreading of light
- Assumptions
- Use of distance
Section 1 of 9Luminosity and radiant flux
- Luminosity L = the total power radiated by a star, in watts.
- Radiant flux F = the power per unit area received normally at the observer, in W m−2.
- Difference
- luminosity is the whole output at the star, while the radiant flux is the small fraction reaching a unit area on Earth after spreading out.
Section 2 of 9Inverse square law of flux
- Spreading of light
- the star's radiation spreads evenly over a sphere of surface area 4πd2, where d is the distance to the star.
- Equation
- F = L/(4πd2).
- A star twice as far away gives one quarter of the flux.
- A larger measured F means the star is closer.
- Assumptions
- uniform radiation and no absorption between the star and Earth.
- Use of distance
- d is the distance to the star, not the star's radius.
Section 3 of 9Standard candles and stellar distances
- Standard candle = an astronomical object whose luminosity is known because of a characteristic property of its class.
- Cepheid variable stars
- pulsating stars whose brightness varies periodically, with a period related to their luminosity.
- Type 1a supernovae
- explosions of a white dwarf in a binary pair that always reach the same peak luminosity.
- Method
- measure the flux F received, use the known L and calculate d from the inverse square law.
- Distance ladder
- parallax works only for nearby stars, so overlapping standard-candle methods, each covering a range, build the scale out to distant galaxies.
- Comparison
- type 1a supernovae are far more luminous than Cepheids, so they are visible and usable in the most distant galaxies.
Section 4 of 9Wien's displacement law
- Black body = an object that absorbs all radiation falling on it, reflecting and transmitting none, and is a good emitter.
- Stars are the best approximation, and the spectrum depends only on temperature.
- Wien's law
- the peak wavelength is inversely proportional to the surface temperature, λmaxT = 2.9 × 10−3 m K.
- A hotter body has a shorter peak wavelength and a greater intensity at every wavelength.
- Temperature must be in kelvin.
- Colour and temperature
- hotter stars are blue or white and cooler stars are yellow or red, such as Betelgeuse in Orion.
| Colour | Temperature / K |
|---|---|
| Blue | above 33 000 |
| Blue-white | 10 000 – 30 000 |
| White | 7500 – 10 000 |
| Yellow-white | 6000 – 7500 |
| Yellow | 5000 – 6000 |
| Orange | 3500 – 5000 |
| Red | below 3500 |
Section 5 of 9Stefan–Boltzmann law and stellar radii
- Stefan–Boltzmann law = the total energy emitted per unit area per second by a black body is proportional to the fourth power of its absolute temperature.
- Luminosity
- L = 4πr2σT4, where r is the star's radius and σ = 5.67 × 10−8 W m−2 K−4.
- Luminosity depends on both surface temperature and radius, so a cool star can be very luminous if it is huge.
- Finding a radius:
- Use Wien's law to find the surface temperature from the peak wavelength.
- Find the luminosity, from the inverse square law if flux and distance are given.
- Rearrange to r √[L/(4πσT4)].
Section 6 of 9Spectra of stars and galaxies
- Information
- astronomers study space only through the radiation arriving from it, including emission and absorption spectra.
- Absorption lines
- hydrogen and helium in a star absorb particular wavelengths, giving characteristic lines.
- Distant galaxies
- the same pattern of lines appears but shifted to longer wavelengths towards the red end.
- The pattern identifies the element and the shift gives the speed.
Section 7 of 9Doppler redshift
- Doppler effect = the apparent change in wavelength or frequency of radiation caused by relative motion of source and observer.
- Redshift
- the source is receding, so the wavelength increases and the frequency decreases.
- Blueshift
- the source is approaching.
- Equation (non-relativistic)
- Δλ/λ ≈ Δf/f ≈ v/c.
- Wording
- the wavelengths of spectral lines increase towards the red end, and the lines do not literally "become red".
Section 8 of 9The expanding universe and Hubble's law
- Expansion
- nearly all galaxies are receding, which suggests the space between them is expanding.
- The expansion stretches light waves on their way to us, producing the redshift.
- The more redshifted the light, the faster the galaxy recedes.
- Balloon analogy
- dots on an inflating balloon move apart because the rubber stretches, as galaxies are carried apart by stretching space and not by moving through it.
- Hubble's law = the recession speed of a galaxy is proportional to its distance from Earth, v = H0d.What the symbols mean: v = recession speed of the galaxy (km s−1) · H0 = Hubble constant (km s−1 Mpc−1) · d = distance (Mpc)
- Hubble found speeds from redshift and distances from standard candles.
- H0 is the Hubble constant (the expansion rate, in s−1), the gradient of a v–d graph.
- Further galaxies recede faster.
Section 9 of 9Big Bang and the age of the universe
- Big Bang theory
- running the expansion backwards, all matter was at the same point in the past, in a hot, dense singular point that began expanding very quickly.
- Redshift and expansion are key evidence.
- Age of the universe
- assuming a constant expansion rate, t0 = 1/H0.
- Estimates
- current estimates are 13 to 14 billion years, and obtaining an accurate H0 is a high priority for cosmologists.
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