The Nature of Stars Flashcards
What is a parsec?
Parsecs (pc) and lightyears (ly) are used as convenient astronomical distance units because they are very large.
- A lightyear is simple: the distance light travels in 1 year.
- A parsec is DEFINED to be that distance at which a star will have a parallax angle of 1 arcsecond – see next slide.
One Parsec (pc)
One pc is the distance from which Earth would appear to be one arcsecond from the Sun.
How do you determine the distance to a star?
If we are to know exactly how luminous is a star, then we need to know how far it is away.
- This is tricky for most stars because of variable interstellar absorption effects.
- But for nearby stars we can use Parallax.
d=1/p
where d = distance in parsecs and p = parallax angle in arcseconds NB 1 AU = 1 astronomical unit (the average Earth-Sun distance)
Gaia - NT
How do you determine the luminosity of a star?
Since starlight spreads out uniformly over a sphere, and we (on the earth) intercept just a part of this light, we need to multiply up to account for the whole sphere of light.
If L is the star’s absolute luminosity, and d is its distance, then, b, the apparent luminosity is given by:
b = L / (4π d2) (where 4πd2 = the surface area of a sphere)
What is the proper motion of a star?
- We cannot directly measure the component of velocity along the line of sight (vr) since this does not cause the position of the star on the sky to change.
- But we can determine the tangential component (vt) by observing the changing location of the star at distance d pc.
- Proper motion, μ = vt/(4.74d) arcsec/year
Quantifying brightness - understanding the logarithmic scale
Magnitudes
A logarithmic based scale for quantifying brightness.
A difference of 1 magnitude corresponds to a factor of 2.5 in brightness.
A difference of 5 magnitudes corresponds to
2.5 x 2.5 x 2.5 x 2.5 x 2.5 = (2.5)5 ~ 100 in brightness.
• If we have two stars of apparent magnitude of m1 and m2, then they are related to their apparent brightness b1 and b2 by:
m2 – m1=2.5 log (b1/b2) …..Eqn 1
Quantifying brightness - absolute magnitude
We observe apparent magnitude, m.
What we need to know is the absolute magnitude, M, of an object
The absolute magnitude is defined as the magnitude that object would have at a distance of 10pc.
So if it’s actually at a distance, d parsecs, away:
m – M = 2.5 log (b1/b2) from Equn 1 where b1 is the brightness at 10 pc and b2 is the brightness at d pc.
• • •
But also we have that b1/b2 = (d/10)2 (brightness falls off as 1/d2) So we have (m-M) = 2.5 log (d2/100)
=2.5(log d2 – log100)
Finally we have (m–M)=5logd–5
where (m-M) is called the distance modulus to an object.
Spread of stars of a given luminosity
Temperature and colour relationship
Astronomical Filters
The brightness of stars is normally measured through certain standard coloured filters.
- This process is called photometry.
- The filters cover the entire visible and IR range and given letters. The most common system, the Johnson-Morgan system, uses:
UBVRIJHK
Colour being described as magnitude differences
Because the magnitude scale is a logarithmic one, if we convert the brightness ratios into magnitudes then we end up with the colour being described as magnitude differences :
e.g. brightness ratio bB/bV is equivalent to (apparent mag B) – (apparent mag V) or just (B-V).
Classifying stars
Using the spectra of stars it is possible to classify a star as a particular spectral type.
- This is done by examining the emission or absorption lines present in a stars spectrum.
- For historical reasons the sequence now used is:
OBAFGKM
This takes us from very hot to very cool stars.
Subclassification
With the advent of superior spectrographs in the last 50 years it became apparent that the OBAFGKM classification needed refining.
So each class is now given a number between 0 and 9 to sub-divide the type
So we have, for example, A7, G3, B5 etc (the Sun is G2).
The key to classification is the relative strength of many different absorption lines from many different elements in the star.
What is a Hertzsprung-Russell diagram?
- Discovered independently by a Danish and US astronomer in 1911
- It allows us to understand stars relative to other stars
- It allows us to see evolutionary paths for stars