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Questions on black-body radiation and spectral classes
A star radiates approximately as a black body, so Wien's displacement law turns the peak wavelength of its spectrum into a surface temperature. Stefan's law P = σAT⁴ then converts that temperature and the star's surface area into a power output, and with the power known the two laws together give the radius. Absorption lines sort stars into the classes O to M.
19 original questions · 57 marks · the black-body radiation and spectral classes notes · Astrophysics
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State Stefan's law and Wien's displacement law, defining each symbol and giving the unit of Wien's constant.
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Stefan: P = σAT4, with A the surface area and T the surface temperature in kelvin (1). Wien: λmaxT = 2.9 × 10−3 m K, the constant carrying the product unit metre kelvin (1).Write the spectral classes in order from hottest to coolest, and state the class of the Sun.
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O B A F G K M, hottest to coolest (1). The Sun, at about 5800 K, is a class G star (1).State the two assumptions made when a star's temperature, power and radius are deduced from its measured spectrum.
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The star radiates as a black body (1), and the light travels to the telescope without absorption on the way, by dust or by atmosphere (1).State what is meant by a black body.
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A body that absorbs all the electromagnetic radiation incident on it (1). It is therefore also the best possible emitter, radiating a spectrum that depends only on its temperature (1).State the colour of a class O star and of a class M star, and name the molecule prominent in class M absorption spectra.
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Class O stars are blue; class M stars are red (1). Class M spectra show molecular absorption by titanium oxide, TiO (1).A star's surface temperature rises. Describe two changes to its black-body radiation curve.
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The peak moves to a shorter wavelength (Wien's law) (1), and the curve rises at every wavelength, so the total power radiated (the area under the curve) increases (1).Calculate the peak wavelength of the radiation from a star with a surface temperature of 10 000 K, and state the region of the spectrum in which it lies.
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λmax = 2.9 × 10−3/10 000 (1)
λmax = 2.9 × 10−7 m (1)
In the ultraviolet, so the star looks blue-white (1)A star's spectrum peaks at 9.7 × 10−7 m. Calculate its surface temperature and suggest its spectral class.
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T = 2.9 × 10−3/(9.7 × 10−7) (1)
T = 2990 K (1)
Just below 3500 K, so a red class M star (1)A star has twice the Sun's radius (take the Sun's radius as 6.96 × 108 m) and a surface temperature of 9000 K. Calculate its power output.
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A = 4πr2 = 4π × (1.39 × 109)2 (1)
A = 2.43 × 1019 m2 (1)
P = σAT4 = 5.67 × 10−8 × 2.43 × 1019 × 90004 (1)
P = 9.1 × 1027 W (1)Explain why the hydrogen Balmer absorption lines are strongest in class A stars, weaker in cooler stars, and weak again in the hottest stars.
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Balmer absorption needs hydrogen atoms already excited to the n = 2 level (1). In cool stars almost all atoms sit in the ground state, so the lines are weak; in the hottest stars the hydrogen is ionised, so no bound electrons remain to absorb (1). Class A, 7500 to 11 000 K, is the productive middle (1).A star's surface temperature triples while its radius stays the same. State the factor by which its power output increases.
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P ∝ T4 at fixed area (1), so the power rises by a factor of 34 = 81 (1).Two stars have equal radii. One has its spectral peak at 400 nm, the other at 800 nm. Calculate the ratio of their power outputs.
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λmaxT is constant, so the 400 nm star is twice as hot as the 800 nm star (1). With equal areas P ∝ T4 (1), so the ratio is 24 = 16, the hotter star radiating 16 times the power (1).A white dwarf of radius 7.0 × 106 m radiates a total power of 1.1 × 1024 W. Calculate its surface temperature. σ = 5.67 × 10−8 W m−2 K−4.
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A = 4πr2 = 4π × (7.0 × 106)2 = 6.2 × 1014 m2 (1). T4 = P/σA (1) = 1.1 × 1024/(5.67 × 10−8 × 6.2 × 1014) (1), so T = 1.3 × 104 K (about 13 000 K) (1).Calculate the power radiated by each square metre of the Sun's surface, taking the surface temperature as 5800 K and σ = 5.67 × 10−8 W m−2 K−4.
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Power per unit area = σT4 = 5.67 × 10−8 × 58004 (1) = 6.4 × 107 W m−2 (1).A red giant radiates 3.9 × 1028 W, one hundred times the Sun's output, from a surface at 3480 K. Calculate its radius, and express it in solar radii (Sun's radius 6.96 × 108 m).
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A = P/σT4 = 3.9 × 1028/(5.67 × 10−8 × 34804) (1)
A = 4.7 × 1021 m2 (1)
r = √(A/4π) (1)
r = 1.9 × 1010 m (1)
≈ 28 solar radii (1)Two stars have the same radius. Star X is class M and star Y is class A. Compare, with reasons, their colours and their power outputs.
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X, below 3500 K, peaks towards the infrared and looks red (1); Y, between 7500 and 11 000 K, peaks towards the ultraviolet and looks blue-white (1). With equal areas, P ∝ T4, so Y out-radiates X by a factor of between about 20 and a few hundred (1).A student says a star's colour tells you its temperature. State what measurement makes this precise, and the law that converts it.
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Measure the wavelength at which the star's black-body spectrum peaks (1); Wien's law λmaxT = 2.9 × 10−3 m K then gives the surface temperature directly (1).An astronomer must decide which of two stars is the larger. Star J radiates 4.6 × 1026 W with its spectral peak at 690 nm; star K radiates 1.5 × 1027 W with its peak at 230 nm. Deduce which star has the larger radius. σ = 5.67 × 10−8 W m−2 K−4; Wien constant 2.9 × 10−3 m K.
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Wien: TJ = 2.9 × 10−3/(6.9 × 10−7) = 4.2 × 103 K and TK = 1.3 × 104 K (1). A = P/σT4 and r = √(A/4π) (1). rJ = 1.4 × 109 m (1); rK = 2.9 × 108 m (1). Star J is about 5 times larger in radius, despite its smaller power output: its low temperature must be offset by area (1).Describe fully how astronomers determine the radius of a distant star from its spectrum and its measured brightness, naming each law used and stating the assumptions involved.
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Measure the wavelength at which the star's spectrum peaks; Wien's law λmaxT = 2.9 × 10−3 m K gives the surface temperature (1). Measure the radiant flux at Earth and, knowing the star's distance, use the inverse square law to find the total power radiated (1). Stefan's law P = σAT4 then gives the surface area (1), and A = 4πr2 converts area to radius (1). This assumes the star radiates as a black body (1) and that no light is absorbed between the star and the telescope, by dust or atmosphere (1).
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