Stars - Sizes and types
Andrew Conway
Spectra of stars
Source: NASA Public Domain
Harvard spectral classification
- Spectral classification:
- From hottest to coolest: O B A F G K M
- Mnemonic: Oh, Be A Fine Guy (or Girl) Kiss Me
- Further subdivided: e.g. G0 is hottest in G and G9 is coolest
- Luminosity class uses a Roman numeral:
- 0 to IV are giants
- V is main sequence
- VI and VII are dwarfs
Solar values
The symbol ☉ is used to denote solar values.
- The Sun is a G2V star.
- The surface temperature is 5800 K.
- Radius: R☉ = 696,000 km
- Luminosity: L☉ = 3.85 × 1026 W
[Optional task: If you were to cover the surface of the Sun with enough 100 W light bulbs to match its luminosity, what size would each bulb need to be to all fit on the surface?]
Large numbers
To avoid writing out long numbers, we can use a short hand:
103 |
1000 |
3 |
104 |
10,000 |
4 |
105 |
100,000 |
5 |
106 |
1,000,000 |
6 |
Examples:
- 2 million = 2,000,000 = 2×106
- R☉ = 696,000 km = 6.96×105 km = 6.96×108 m
Classification table
O |
≥ 33,000 K |
blue |
≥ 30,000 L☉ |
~0.00003% |
B |
10,000–33,000 K |
blue white |
25–30,000 L☉ |
0.13% |
A |
7,500–10,000 K |
white |
5–25 L☉ |
0.6% |
F |
6,000–7,500 K |
yellow white |
1.5–5 L☉ |
3% |
G |
5,200–6,000 K |
yellow |
0.6–1.5 L☉ |
7.6% |
K |
3,700–5,200 K |
orange |
0.08–0.6 L☉ |
12.1% |
M |
2,000–3,700 K |
red |
≤ 0.08 L☉ |
76.45% |
Data source
Luminosity and temperature
Stefan's law: the power radiated by a "black body" at temperature T per unit surface area is proportional to T4
- In physics, "black body" is an ideal emitter (and absorber) of light
- T4 = T×T×T×T
Flux and Stefan's law
- Power per unit area is often called a flux.
- If T is in kelvin, then the flux F is
F = 5.67×10-8 T4
where F will be in W m-2 (watts per square metre)
Flux at the solar surface
The solar surface is at temperature 5800 K
F |
= 5.67×10-8 × 5800 × 5800 × 5800 × 5800 |
|
= 64,164,532 W m-2 |
|
= 64,200,000 W m-2 |
|
= 6.42×107 W m-2 |
Since we only started with three significant figures (e.g. 5.67), we round to 3 significant figures in the last step.
Flux and luminosity
- The flux is power per unit area.
- Luminosity is total power over the entire surface.
- So flux times surface area will give luminosity.
- L = F × A
- where A is the area of the Sun in square metres.
Surface area of the Sun
- For a sphere A = 4π R2
- where π = 3.141592... but we'll use 3.14
- From earlier: R = 6.96×108 m
A |
= 4π R2 |
|
= 4 × 3.14 × 6.96×108 × 6.96×108 |
|
= 4 × 3.14 × 4.84 × 1017 |
|
= 6.08×1018 m2 |
Theoretical solar luminosity
- Plugging our values for F and A into L = F A, we find
L |
= 6.42×107 × 6.08×1018 |
|
= 3.90×1026 W |
- This is very close to measured values (see earlier).
- This confirms that stars are indeed good approximations to black bodies.
Deducing star radius
- L is proportional to R2 and T4
- Double R and L increases by a factor of 2×2=4
- Double T and L increases by a factor of 2×2×2×2=16
- So is, say, an O type star more luminous than a B type star because R or T is greater?
- Answer: both!
Red giants
- Betelegeuse:
- L = 100,000 L☉
- R = 1000 R☉
- If the Sun was 1000 times larger at the same surface temperature, then its luminosity would be 1000×1000=1,000,000 times larger.
- But Betelgeuse is only 100,000 times more luminous than the Sun.
- So we can deduce that Betelgeuse must have a lower surface temperature than the Sun.
- It is about 3400 K, which corresponds to a red colour.
- Hence red and giant.