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- Key Concepts
- Properties of Stars:
- -Luminosity
- -Temperature
- -Masses
- The Hertzsrung-Russell Diagram
- Star Clusters
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- Luminosity - amount of electromagnetic radiation over all wavelengths
emitted by star’s entire photosphere per unit of time
- Measure in watts ( = joule/s) or erg/s
- L = (4pR2)(sT4)
- Luminosities known for several hundred stars
- Examples: Lsun = 3.8
x 1026 watts, LProxima
Centauri = 0.0006Lsun, LBetelgeuse = 38,000Lsun
- Apparent brightness (luminosity-distance formula)
- bstar = Lstar / (4p*distance2)
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- Must know true brightness of class of stars, membership can be based on
- Spectral type
- Luminosity type
- Variability
- Association, etc.
- Calculate distance from observed apparent brightness by inverse-square
law
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- Yes, the distance permits us to determine the intrinsic properties of
stars, such as luminosity, radius, and mass.
- Otherwise, we are restricted to relative values, which is a much weaker
understanding of stars.
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- Light Year - distance light travels in one year at the rate of 300,000
km/s (186,000 miles/s)
- 1 ly
= 9.46 x 1012 km
- Example - Proxima Centauri, nearest star, is 4.2 ly
- Parsec - (parallax of one second of arc) the distance at which one AU
subtends an angle of one second of arc
- 1 pc = 3.26
ly = 3.09 x 1013 km
- Example - Proxima Centauri is 1.3 pc from Solar System
- Formula: d (in parsecs) = 1 / p
(in arcseconds)
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- Hipparchus (2nd century BC) measured (naked eye) apparent
brightness of stars assigning them to 1 of 6 magnitude categories
- Bright stars - 1st magnitude
- Faintest stars - 6th magnitude
- Apparent magnitude - logarithmic measure of apparent brightness
- Ratio of apparent brightness of 1st to 6th magnitude defined to be
100:1
- Formula: b1st/b6th
= 100 = 2.5125 =
2.512(6-1)
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- Formula: b1/b2
= 2.512(m2-m1)
- Apparent scale is an inverted scale
- Bright stars are algebraically small numbers (m<0)
- Faint stars are algebraically large numbers (m>0)
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- Absolute magnitude - apparent magnitude star would have at distance of
10 pc or 32.6 ly
- Formula: B/b = (d/10 pc)2
= 2.512(m-M)
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- Numbers of stars for a given luminosity lying within 1000 pc3
- Faint stars far more numerous than bright stars
- Steep decline toward high luminosities
- Shows that extremely luminous stars are rare
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- Yes
- Temperature of its photosphere.
- Stars are thermal sources of radiation.
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- Slope of thermal radiation curve through the visual depends on temperature
- Ratio of brightness in one part of spectrum, such as blue, to that in
another part, such as green, depends on temperature
- Ratio of brightness is called a color index or just a color
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- Yes, the ability of any atom or ion to absorb radiation at selected
wavelengths depends on the temperature and density of the matter in
which the atom or ion is located (the photosphere of the star).
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- Spectral classification - grouping stars according to similarities in
violet, blue, and green portions of visible spectrum
- Seven spectral classes - O, B, A, F, G, K, M
- Each spectral class subdivided into 10 spectral types
- Spectral class A subdivided into spectral types A0, A1, A2, A3, A4, A5,
A6, A7, A8, A9
- Spectral class O is exception, subdivided into O4, O5, O6, O7, O8, O9
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- Terminology for direction along spectral sequence
- Early-type stars - toward spectral classes O, B, A
- Late-type stars - toward spectral classes G, K, M
- Spectral classification grades stars according to photospheric
temperature (66 bins) and not chemical composition
- Spectral appearance of star depends on temperature and density of the photosphere
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- The overall range of stellar masses runs from 0.08 to about 100 times
the mass of the Sun.
- We can measure the masses of stars in binary star systems using Newton’s
version of Kepler’s third law, if we can measure the orbital period and separation
of the two stars.
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- A star's mass at birth determines virtually everything that happens to
it throughout its life.
- While a star is a main-sequence star, its mass determines its
luminosity, surface temperature, radius, and hydrogen-burning
lifetime—which is shorter for more massive stars.
- Once a star exhausts its core hydrogen, its mass determines how and when
it grows into a giant or super-giant, and also determines what happens
to it when it finally dies.
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- The primary method for determining mass is through the motion in which
stars exert significant gravitational influence on other stars, such as
in a binary system.
- Restrictions
- Most be able to determine orbits or path.
- Sum of the masses of both stars in a binary are determined.
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- Binary system - two (or more) stars held by mutual gravitational
attraction
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- Visual binaries - two or more stars observed
- Widely separated in general
- Fairly close to Solar System in general
- Spectroscopic binaries - appears as single star, Doppler shifts reveal
binary nature
- Double-line systems - absorption spectrum of both stars visible
- In general, not widely separated pair of stars
- Single-line systems - absorption spectrum of only brighter star visible
and undergoing Doppler shifts;
second star too faint
- Eclipsing binaries - systems in which one star passes in front of other
star
- Orbit plane contains line of sight
- Relative few systems, but important for amount of information
obtainable on star properties
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- Visual binary
- Orbit is that of fainter star relative to brighter
- Kepler’s third law yields sum of masses for system
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- Percentage of all stars that are part of binary system is at least 50%,
probably higher
- Probable that all stars form in companion relation with and/or
- Other stars
- Brown dwarfs
- Jovian-like planets
- Terrestrial-like planets
- Even smaller bodies
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- We classify stars according to their spectral type and luminosity class.
- The spectral type tells us the star’s surface temperature and color.
- The luminosity class tells us how much light the star puts out.
- Giant and super-giant stars put out far more light than main-sequence
stars like our Sun, even though their surface temperatures are generally
lower, meaning that their radii must be much larger.
- All stars become giants or super-giants near the ends of their lives,
and many end up as hot but dim white dwarfs.
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- Luminosity class - luminosity obtained from spectra of stars
- More subtle than temperature effects
- I very luminous supergiants
- II bright giants
- III giants (red giants)
- IV subgiants
- V main-sequence (dwarf stars)
- VI subdwarfs
- VII white dwarfs
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- Observation - masses increase from spectral class M to O for
main-sequence stars
- Mass-luminosity relation - plot of mass against luminosity (where
possible)
- Luminosity proportional to approximately fourth power of mass
- Equation: L µ M4
- Fundamental property upon which distinguishes star is mass
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- An H–R diagram plots stars according to their surface temperatures and
luminosities.
- Hydrogen-burning stars occupy a narrow band in the diagram known as the main
sequence.
- Giants and super-giants are to the upper right of the main sequence and white
dwarfs are to the lower left.
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- Examples
- Sun - G2 V
- Sirius - A1 V
- Procyon - F5 IV-V
- Betelguese - M2 I
- Rigel - B8 I
- Names more than poetic
- Supergiants possess large radii
- Main-sequence stars possess small radii
- 90% of all stars are main-sequence stars
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- Stars radiate like blackbodies.
- L = 4pR2sT4
µ R2T4
- R = radius
- T = photospheric temperature (K)
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- Main sequence is defined by hydrogen burning; all stars on the main
sequence derive energy through hydrogen burning
- Time star spends on main sequence is proportional to mass divided by
luminosity
- Equation: tmain sequence µ M/L
- Substituting mass-luminosity relation for main-sequence stars; tmain sequence µ M/(M4) µ 1/M3
- How long H-burning lasts depends on star’s mass
- High-mass stars Þ short main-sequence life
- Low-mass stars Þ long main-sequence life
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- Stellar cluster - many stars, greater than about 100, held together by
mutual gravitational attraction
- Star orbits in cluster unstable
- Motion like a random walk
- Categories
- Open (galactic) clusters
- Globular clusters
- OB Associations
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- Typical separation - » 2-3 ly
- Field stars (Sun) - » 5-6 ly
- Typical size - 10’s of ly
- Typical numbers of stars - 10’s to 1000’s
- Brightest stars
- Either blue main sequence, giants, and supergiants
- Or, red giants and supergiants
- Number of clusters > 20,000
- Located in spiral arms and disk
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- Number of stars - about 500
- Diameter - about 5 ly
- Age - about 100 million years
- Main sequence stars
- No red giant stars
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- Stellar evolution proceeds according to the mass of the star.
- According to our theoretical understanding of stellar evolution,
massive stars evolve faster than low mass stars.
- Star clusters are collections of different mass stars, but they formed
at the same time and from the same material.
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- Turnoff point - most massive main sequence star that has not reached
hydrogen exhaustion line
- Indicates age of cluster from model calculations
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- Typical separation - » 0.2 ly
- Typical size - 100’s ly
- Typical number of stars - 10,000’s to 100,000’s
- Brightest stars
- Always red giants and red supergiants
- No bright blue stars
- Number of globular clusters - » 150
- Located in halo and near nucleus
- Are among the oldest stars in our Galaxy (10-13 billion years)
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- Mass and age determine differences among stars; stars are hydrogen and
helium structures at birth.
- Hertzsprung-Russell (H-R) diagram summarizes properties of stars and
their evolution.
- Stars spend most of their lives as main-sequence stars replacing the luminosity
by converting hydrogen to helium;
masses of stars increases up the main sequence; the more massive the star the shorter
its main-sequence lifetime will be.
- Star clusters provide a validation of our theoretical studies of stellar
structure and evolution.
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