D.1 Stellar Quantities
Light year (Ly) & Astronimical unit (AU)
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A Light year is the distance travelled by light in one year, which is 9.46×10^15^m
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An Astronimical unit is the average radius of the Earth’s orbit around the Sun, which is 1.5×10^11^m = 3.26ly
Stellar parallax
The parallax angle is the angle, at the position of the star, that is subtended by a distance equal to the radius of the Earth’s orbit around the Sun (1AU).
A parsec is the distance to a star whose parallax is 1 arc second, which is 3.09×10^16^m
An arc second is 1/3600 of a degree
- The average distance between stars in a galaxy is about 1pc
- Obveratory on Earth could see star within 100pc (Because of the distortion caused by atmosphere)
- High resolution satellite could see star within 100,000pc
- Distance toward the edge of milky way galaxy is 30,000pc
- Galaxy cluster (30 galaxies): 1,000,000pc
The parallax method is also a means of measuring astronomical distances:
$$ d \textcolor{grey}{\text{ (parsecs)}}=\frac{1}{p\textcolor{grey}{\text{ (arc seconds)}}} $$
But if the star is too far, p would be too small to be measured accureately!
Apparent brightness & Luminosity
Apparent brightness: The received power per unit area $$ b=\frac{L}{4\pi d^2} $$ $b$: Apparent brightness ($Wm^{-2}$)
$L$: Luminosity ($W$)
$d$: Distance ($m$)
Luminosity: Total power radiated by the star
$$ L=\sigma AT^4 $$
$\sigma$: Stefan-Boltzmann constant
$A$: Area of the star ($m^2$)
$T$: Temperature ($K$)
A star is assumed to radiate like a black body.
$L_{\bigodot}$ symbolized the luminosity of the sun, the same for other variables.
The nature of stars
The stability of a star depends on the equilibrium between radiation pressure and gravitational pressure
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Radiation pressure make the star expand
- Nuclear fusion provides the energy the star needs to keep it hot so that the star’s radiation pressure is high enough to oppose gravitational contraction.
- Gravitation make the star collapse
Proton–proton cycle (fusion reactions)
- $^1_1\text H+^1_1\text H\rightarrow^2_1\text H+^0_1e^++v_e$
- $^2_1\text H+^1_1\text H\rightarrow^3_2\text He+\gamma$
- $^3_2\text He+ ^3_2\text He\rightarrow^4_2\text He+2^1_1\text H$
Main sequence star
A normal star that is undergoing nuclear fusion of hydrogen into helium.
- 90% of stars are main sequence star
Composition | Proportion |
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Hydrogen | 70% |
Helium | 28% |
Other heavier elements | 2% |