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1446 Introductory Astronomy II

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Title: 1446 Introductory Astronomy II


1
1446 Introductory Astronomy II
  • Chapter 11
  • The Nature of Stars
  • R. S. Rubins
    Fall, 2009

2
The Lives of Stars 1
  • Birth they are created from interstellar gas
    clouds.
  • Life they shine from millions to hundreds of
    billions of years with the energy created by
    thermonuclear fusion.
  • Death they die spectacularly, by one of several
    methods, which, for an isolated star, depends
    only on its mass.
  • After the Sun, the nearest star to us (after the
    Sun) is Proxima Centauri, which is about 25
    trillion miles (4 ly) away, so that its light
    about 4 years to reach us.
  • In all its stages, the life of a star is a battle
    between the inward pressure of gravity, which
    tends to collapse the star, and the net outward
    thermal pressure, which tends to expand the star.
  • (Heating the air in a balloon causes it to
    expand.)

3
The Lives of Stars 2
  • Gravity is always present, but throughout its
    life, the star must continually replenish its
    thermal energy to prevent collapse.
  • Both nuclear fusion, in which matter is converted
    to energy, and gravitational collapse, in which
    potential energy is lost, produce thermal energy.
  • Ultimately, gravity secures at least a partial
    victory.
  • Except for the most massive stars, which end
    their lives as black holes, gravitational
    collapse is ultimately stopped by a quantum
    mechanical effect, known as degeneracy pressure.
  • The outcome for an isolated star depends on its
    birth mass.

4
Total Luminosity
  • The total luminosity L of a star is the total
    energy per second that it radiates into space.
  • L depends only on its surface temperature T and
    radius R, and is given by
  • L ? T4R2.
  • The visual luminosity is the visible energy per
    second radiated into space.
  • The apparent brightness is the visible energy per
    second which crosses unit area of a surface
    perpendicular to the light flow
  • The variation of brightness with distance in
    space is given by
  • apparent brightness ? 1/(distance)2.
  • This is an example of an inverse-square law.

5
Inverse Square Law
6
Apparent Magnitude
  • In the magnitude system, introduced by the Greek
    astronomer Hipparcos (2nd Century BCE), the
    brightest stars were given magnitude 1, the
    next brightest magnitude 2, and so on.
  • In the modern system, the apparent magnitude m is
    a measure of the visual brightness of objects as
    measured from the Earth.
  • Very bright objects have negative magnitudes
  • e.g. MSun 26.7 , Mfull moon 12.5.
  • Very dim objects have positive magnitudes
  • e.g. MPluto 15 , Munaided-eye limit
    6.

7
Apparent Magnitude Scale
8
Absolute Magnitude
  • The absolute magnitude M is a means of comparing
    the true brightnesses (or visual luminosities)
    of stars.
  • This is done by calculating the apparent
    magnitude it would have if it were at a
    designated distance of 10 pc (parsec).
  • Calculation of M, knowing m and the distance d.
  • M m 5 log (d/10),
  • where d is in pc, and log(10n) n.
  • Example Find the absolute magnitude of star at a
    distance of
  • 1000 pc, with an apparent
    magnitude of m 5.
  • Solution
  • M 5 5 log(1000/10) 5 5 log(102)
    5 (5x2) 5.

9
H-R Diagram 1
  • The two basic properties needed to characterize
    stars are
  • i. the surface temperature T,
  • ii. the luminosity L or the absolute
    magnitude M.
  • In an H-R diagram,
  • M or log L
  • is plotted against
  • T or the spectral type.
  • Notes
  • T increases from right to left (the left side is
    hotter).
  • The spectral type is symbolized as follows by the
    letters
  • O (hottest), B, A, F, G, K, M (coldest).

10
Spectral Classes
  • Major classification
  • O B A F G
    K M
  • oh be a fierce giraffe
    kick me
  • hottest
    coolest
  • Minor classification
  • 0 1 2 3 4 5 6
    7 8 9
  • hottest
    coolest
  • A5 is hotter than G2.
  • A3 is hotter than A6.
  • B5 is hotter than A5.

11
Annie Cannon and Spectral Type
  • In the 1880s, Edward Pickering used female
    students to analyze star data at Harvard College,
    classifying 10,000 stellar spectra were
    classified with the letters A to O, based on the
    relative strengths of their H spectra, which he
    incorrectly assumed was proportional to the
    surface temperature of the star.
  • The confused situation was sorted out by
    Annie Cannon, 20 years before Bohrs theory of
    the H atom gave a theoretical connection between
    spectral intensities and temperature.
  • Reducing the number of letters to 7, she
    reorganized the scheme into its present form, and
    classified over 400,000 stars.
  • She became the first woman to be awarded an
    honorary degree by Oxford University in England.

12
Stellar Spectra 1
13
Stellar Spectra 2
14
H-R Diagram 2
  • Satellite data are shown for almost 41,500 nearby
    stars.
  • The thickness is due to the presence of star
    clusters of widely different ages.

15
H-R Diagram 3
16
H-R Diagram 4
17
H-R Diagram 5
18
Relative Sizes of Stars 1
19
Relative Sizes of Stars 2
20
Radii of Stars 1
1000 RSun
100 RSun
10 RSun
RSun
0.1 RSun
21
Radii of Stars 2
  • Luminosity L ? R2T4.
  • White dwarfs are found in the lower left of the
    diagram. Since they are hot and have low
    luminosities, they must be very small.
  • Their radii are about 0.01 RSun.
  • Red giants and red supergiants lie mainly at the
    upper right of the diagram. Since they are cool
    and have high luminosities, they must be
    extremely large.
  • Red giants have radii in the range 10 RSun to
    100 RSun.
  • Red supergiants have radii from 100 RSun to
    1,000 RSun.
  • Main sequence stars lie on a diagonal line from
    lower right(radius 0.1 RSun) to the upper left
    (radius 10 RSun).

22
Luminosity Classes
  • The Sun is a G2 V star.
  • Aldeberan, a red giant, is a K5 III star.
  • Regulus, a hot blue main sequence star, is a B7 V
    star.
  • Betelgeuse, a red supergiant, is an M2 Ia star.

23
Binary Stars Mass Measurement
  • True binary stars are pairs of stars that orbit
    each other about their center of mass.
  • About 1/2 of the objects in the night sky which
    appear to us as single stars, are actually binary
    stars.

24
Binary System Kruger 60
25
Large Separation Binary Stars
  • While only a few low-mass binary star systems
    have been found with separations greater than 50
    AU, two such sets with separations of 1800 AU and
    5100 AU were discovered in 2007, with the latter
    pair taking about 500,000 years to complete one
    orbit.
  • On a human scale, it would be equivalent to two
    baseballs orbiting each other at a distance of
    200 miles (which could only occur if there were
    no other matter in their neighborhood).

26
Measurement of Mass
  • There is no direct method of determining the mass
    of an isolated star, other than the Sun, the mass
    of which may be found from planetary motion.
  • Newtons generalization of Keplers 3rd Law
    applied to a binary system gives
  • Star masses of between about 0.1 MSun and 100
    MSun are normally found, although a star of mass
    120 MSun has recently been measured.

27
Log (Luminosity) vs. Log (Main-Sequence Mass)
  • The life of a star depends only on its birth
    mass, and hence on its main-sequence position on
    the H-R diagram.

28
Main Sequence Masses (in solar masses)
29
A Receding Spectroscopic Doublet
30
Light Curves of Partially Eclipsing Binaries
31
Light Curves of Totally Eclipsing Binaries
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