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7/30/2019 Stars Lecture3(1)
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Professor David AlexanderRochester 335 (top floor)Chapter 7 of Carroll and Ostlie
Lecture 3:Observed properties Binaries, orbits, masses
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Saha equation:
ionisation states
Boltzmann equation:
excitation states
Review of previous lecture
The tight relationship between mass and luminosity further constraint the physical
power source and structure of starsOBAFGKM (RNS): Oh Be A Fine Girl/Guy Kiss Me (Right Now Sweetie)!
Definition of line
equivalent width2
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Aims of lecture
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Binary stars: basic properties
Binary stars provide important insight intothe formation and evolution of stars. As we will see, binary stars provide a
direct method for determining masses.
About 70% of stars in
our galaxy are membersof binary systems.Planets have even been
found around binary (ormultiple) star systems!
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Binary stars: basic properties
In any binary/multiple star system the stars orbit about the centre of mass inelliptical orbits (semi-major axes of a1 and a2 for a binary system)
a2a1
Equation 7
a1 a2
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Binary stars: classification
Binary stars are classified depending on how they are identified:(1) Visual binaries(2) Astrometric binary(3) Eclipsing binary(4) Spectroscopic binaryThese classes are not mutually exclusive (a system can be in more than one
class). We focus mostly on visual, spectroscopic, and eclipsing
spectroscopic binaries (combination of eclipsing and spectroscopic).
Visual binary
In a visual binary both stars can be spatially resolved.Assuming that the orbits of both stars are not long then
it is possible to monitor the duration of the orbit and the
orbital parameters directly.
This image here shows the Castor star system, takenwith a small telescope. The Castor star system was the
first multiple-star system to be identified (in 1678).
Castor is actually a sextuple star system! Both of these
stars have a faint companion (spectroscopic binary) andanother faint binary pair orbits at a greater distance
(which is an eclipsing binary!).
Castor through a small telescope
We wont cover optical doublesand spectrum binaries
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Binary stars: classification
Eclipsing binary:For binaries with orbital planes orientatedapproximately along the line of sight to the observer,
one star may periodically pass in front of the other,
blocking the light of the eclipsed component. Such a
system is recognised by regular variations in the
amount of observed light.
This technique is also used to search for exo-planets
from the small dip in brightness due to the eclipse of a
planet in front of a star.
Astrometric binary:If one member of the binary is much brighter than theother then it may not be possible to directly see the
fainter star. However, the existence of the unseen star
can be inferred from the motion of the brighter star.
A famous example is Sirius B, the white dwarfdiscovered from the motion of Sirius A in 1844
(explored in a later lecture).
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Binary stars: classification
Spectroscopic binary:If the period of a binary system is not
prohibitively long, and if the orbital
motion has a component along the line of
sight, a periodic shift in the spectral lines
will be observable.
If the luminosities of the two stars arecomparable, both spectra will be
observable (double lined). If one is much
fainter than the other is, only one set of
lines is seen (single lined).
Orbital
configuration Wavelength(velocity) line shiftObserver
Stars must be quite close together for changes in velocity to be seen
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Visual binary stars: mass determination
a2a1
Equation 8
a1 a2
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Visual binary stars: mass determination
This picture is a bit idealised because most binary systems will beinclined away from our line of sight and therefore the effect of the
inclination angle on our calculations need to be considered.
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Focus of observed
ellipse
Visual binary stars: mass determination
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Spectroscopic binary stars
Recall from earlier slide:
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Spectroscopic binary stars: eccentricity
Orbital eccentricity has a marked effect on the shape of the velocity curves. Theinclination angle has no effect on the shape but it does effect the amplitude.
Circular orbit (no eccentricity)
Eccentric orbit: skewed velocity curves
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Spectroscopic binary stars: masses
Equation 9
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Spectroscopic binary stars: masses
So we can also express both the mass and the mass ratio in terms of velocity and period.But, again, knowledge of i is required to determine the most accurate masses.
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The inclination angle must be close to 90 degrees for aneclipse to occur, particularly if the secondary star is not in
close orbit. If the secondary star is in close orbit than i will
still be quite close to 90 degrees.
Eclipsing spectroscopic binaries
Eclipsing spectroscopic binaries are a special case of binary star. As the stars areeclipsing the inclination of the system must be close to 90 degrees. Therefore, there are
small inclination angle corrections and so we will have reliable velocity measurements.
We can use also eclipses to estimate stellar radii (as weexplored in lecture 1). The relative drop in light curve also
indicates the effective-temperature ratio of the two stars,
which we will explore in more detail here.
Primary
eclipse
Secondary
eclipse
Therefore, in eclipsing spectroscopic binarieswe get reliable velocity (and therefore mass)
measurements (little angle dependence)
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Eclipsing spectroscopic binaries
The shape of the light profile during the eclipse can further refine estimates of theinclination angle; compare these two plots. Note the overall width of the light-curve
dips are the same irregardless of whether it is a primary or secondary eclipse.
The inclination angle is almostexactly 90 degrees and the dip
in the light curve is flat.
The inclination angle is lessthan 90 degrees (but still highly
inclined) and the dip in the light
curve is peaked.
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Eclipsing spectroscopic binaries: temperature
The relative depths of the light-curve dips indicate the ratio of effective temperaturesPrimary
minimum
Secondary
minimumB0
BP
BS
(see Ch 7 of CO book for
more details)
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Stellar mass-luminosity relationship
Using the best mass constraints, astronomers have found a tight relationship between
mass and luminosity this provides constraints on the energy source (and lifetimes)
Equation 10
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