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The Brightest Stars in the Sky
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Common Name |
Luminosity Solar Units |
Distance LY |
Spectral Type |
Proper Motion arcsec / year |
R. A. hours min |
Declination deg min |
|
| Rigel |
80,000 |
815 |
B8Ia |
0.00 |
05 12.1 |
-08 12 |
| Betelgeuse |
100,000 |
500 |
M2Iab |
0.03 |
05 55.2 |
+07 24 |
| Deneb |
80,000 |
1400 |
A2Ia |
0.00 |
20 41.4 |
+45 17 |
|
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Source: Fraknoi, Morrison, and Wolff |
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Die hellsten Sterne liegen im Sternbild Orion, sind aber nicht
mit der Wolke assoziiert.
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Dies sind die hellsten Sterne in Sonnennähe,
weiter entfernt und heller
sind Eta Carinae (D = 2.3 kpc)
mit dem Homunculus Nebel
und Rho Cassiopeiae (D = 3.3 kpc).
Einer der hellsten Sterne in der Milchstraße (und der lokalen Gruppe) ist
h
Car.
Zwei historische Ausbrüche (integriertes Licht vergleichbar mit einer
Supernova) in den Jahren 1844 und 1885 haben den Homunculus Nebel erzeugt:
Expansionsgeschwindigkeit dex(3.5) km/s und dex(3.1) km/s.
Mit L »
dex(6.7)L
= 2×
1040 erg/s und einer
Masse von M »
100 M
übertrifft h
Car die Eddington Leuchtkraft,
LEdd = 4p
GmHM/sTh = dex(40)(M/100M
) erg s-1.
In unserer Galaxie gehören zu den hellsten Sternen:
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HD 97950, ein Stern mit MV = - 7m,9; vom SpTyp O3,
Masse »
80 M
in NGC 3603.
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Eta Carinae, ein Stern vom SpTyp O3 (MV = -7m),
L »
dex(6.7)L
= 2×
1040
erg/s, Masse »
100 M
.
-
z
Pup und c
Vel ein Doppelsternsystem mit MV = - 7m,3; SpTyp O5.
Zu unserer nächsten
Nachbarschaft gehört die Große Maghellansche Wolke. Die hellsten Sternen dort sind:
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Mk42, ein Stern mit SpTyp O3, Masse »
110 M
, T = 42 000 K,
L = 2.3×
106L
(MV = -7m,1).
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R136a1, ein Stern mit SpTyp O3, Masse »
100 M
im Sternhaufen R136 im Zentrum des 30-Doradus-Nebels.
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R127 = HDE 269858, ein variabler Stern mit SpTyp OIafpe
und mit bipolarem Ausfluß (im Zentrum des 30-Doradus-Nebels).
Die Entfernung zu diesen Sternen ist damit gut bekannt.
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Harlow Shapley
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Hellste Sterne wurden erstmals von Shapley geeicht und von Hubble
zur kosmologischen Entfernungsbestimmung herangezogen.
Es ist allerdings fraglich, ob diese Sterne wirklich
als Eichstandards zu gebrauchen sind. Sie
sind nicht mehr im hydrostatischen Gleichgewicht, sie pulsieren und verlieren
Masse mit einer Rate von bis zu dM/dt = 3×
10-4 M
yr-1.
Die Massenverlust-Rate ist hier so groß, daß die Entwicklungszeit von 1 Myr
für solche Sterne deutlich unterschritten wird, die Leuchtkraft wird damit
eine Funktion der Zeit. Der Stern R127 = HDE 269858 war 1989 der hellste in
LMC.
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Light Curve of Delta Cephei
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Cepheid Variable Stars - Nearby Galaxies
(Reichweite 20 Mpc)
The pulsations of Cepheids are very regular; Cephei has a period of pulsation
(time between maxima or minima) of 5.366341 days. Furthermore the period is
directly related to the luminosity of the star as shown from the
Period-Luminosity Relation.
This relationship was first discovered by Henrietta Leavitt at Harvard who
noticed that Cepheids in the Magellanic Clouds have a relationship between
apparent brightness and period in the sense that brighter Cepheids have longer
pulsation periods.
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Period-Luminosity Relation W Virginis.
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In 1912 Henrietta Leavitt (lived 1868--1921) published the results of her
study of variable stars in the Large and Small Magellanic Clouds. These are
two small satellite galaxies orbiting the Milky Way. The linear size of each
Magellanic Cloud is much smaller than its distance from us. Therefore, to a
good approximation all of the stars in each galaxy are at the same distance
from us. Leavitt found a very useful relationship for a certain type of
variable star called a Cepheid variable (after the prototype in the
constellation Cepheus).
The fainter Cepheids in the Magellanic Clouds have shorter periods. Because
all the Cepheids in a Magellanic Cloud are at the same distance from us,
Leavitt reasoned that the more luminous Cepheids pulsated more slowly. This is
the period-luminosity relation. Leavitt did not know the distances to the
Magellanic Clouds, so she could not tell what the actual value of the
luminosity part of the relation was.
Astronomers had to wait a few years for Harlow Shapley to calibrate Leavitt's
relation using Cepheids in our galaxy for which the distances could be
determined. In the calibration process Shapley put actual values to the
luminosity part of the period-luminosity relation. With a calibrated
period-luminosity relation astronomers could use Cepheid variables as standard
candles to determine the distances to distant clusters and even other
galaxies.
Cepheids have pulsation periods of 1 to 50 days. In the 1950's astronomers
found that there are two types of Cepheids:
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Type I:
classical Cepheids are from young high-metallicity stars and are about
4 times more luminous than Type II Cepheids. Above is the
light curve
(the plot of brightness vs. time) of a classical Cepheid from the Hipparcos
database of variable stars.
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Type II:
W Virginis Cepheids are from older low-metallicity stars and are
about 4 times less luminous than Type I.
Above is the
light curve
of a W
Virginis Cepheid from the Hipparcos database of variable stars. Note the
differences in the shape of the light curve. The two types of Cepheids are
distinguished from each other by the shape of the light curve profile. In
order to compare the shapes without having to worry about the pulsation
periods, the time axis is divided by the total pulation period to get the
``phase'': one pulsation period = one ``phase''.
Early measurements of the distances to galaxies did not take into account the
two types of Cepheids and astronomers underestimated the distances to the
galaxies. Edwin Hubble measured the distance to the Andromeda Galaxy in 1923
using the period-luminosity relation for Type II Cepheids. He found it was
about 90,000 light years away. However, the Cepheids he observed were Type I
(classical) Cepheids that are about four times more luminous. Later, when the
distinction was made between the two types, the distance to the Andromeda
Galaxy was increased by about two times to about 700 kpc.
Recent results from the Hipparcos satellite have given a larger distance of
770 kpc to the Andromeda Galaxy.
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Period-Luminosity Relation.
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Since all the stars in the Magellanic clouds are about the same distance, this
relationship must be a relationship between luminosity and period as well.
Cepheids exemplify the desirable characteristics of standard candles:
-
Their luminosities may be determined from the P-L relationship which has very
little scatter.
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They are giant stars so they are pretty luminous and can be seen out to
relatively large distances. With HST Cepheids are being studied in galaxies in
the Virgo Cluster. about 50 million light-years away.
-
The variability of Cepheids makes them easy to pick out. Photographs (now
digital images) are obtained of galaxies over several nights. When the images
are compared, most stars don't change, but the Cepheids blink brighter and
fainter and are easily distinguished from the billions of other "normal"
stars.
Another type of pulsating star similar to the Cepheids are the RR Lyrae
variable stars (named after the prototype star RR Lyrae). They are smaller
than Cepheids and, therefore, have shorter periods and lower luminosities.
They pulsate with a period between 5 and 15 hours (Cepheid pulsation periods
are greater than 24 hours). Low-mass stars will go through a RR Lyrae
pulsation stage while the high-mass stars will go through a Cepheid stage.
Because low-mass stars live longer than high-mass stars, the Cepheid stars as
a group are younger than the RR Lyrae stars.
RR Lyrae are found in old star clusters called globular clusters and in the
stellar halo part of our galaxy. All of the RR Lyrae stars in a cluster have
the same average apparent magnitude. In different clusters, the average
apparent magnitude was different.
This is because all RR Lyrae have about the
same average absolute magnitude (Mv = +0.6, or L = 49 L
). If the
cluster is more distant from us, the RR Lyrae in it will have greater apparent
magnitudes.
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Cepheid Variable in M100
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RR Lyrae stars can be used as standard candles to measure distances out to
about 760 kpc.
The more luminous Cepheid variables can be used to measure distances out to 40
Mpc. These distances are many thousands of times greater than the distances to
the nearest stars found with the trigonometric parallax method.
One of the prime goals of the Hubble Space Telescope has been the detection of
Cepheid variable stars in distant galaxies. Before HST Cepheids had only been
detected in very nearby galaxies, out to about 4 Mpc.
A team led by Dr. Wendy Freedman of the Carnegie Observatories has detected
the furthest Cepheids yet in the Virgo Cluster spiral M100 at a distance of
about 18 Mpc.
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Lupe: NGC 891 mit IR Spektrum (ISO)
The galaxy NGC 891 (AAO)
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Our galaxy probably closely resembles the galaxy NGC 891 as seen edge-on. Note
the prominent dust lanes going through the disk mid-plane and how flat the
galaxy is.
From above our galaxy may resemble
NGC 2997 = AAT 17 in Antila (at a distance of 10
Mpc, z = 0.003626) or the galaxy
Messier 83 (VLT).
In 1918 Harlow Shapley used his calibrated variable star period-luminosity
relation to find distances to 93 globular clusters. Globular clusters are
spherical clusters of 100,000's to several million stars (looking like a glob
of stars) in very elliptical orbits around the center of the galaxy. Two
globular clusters are shown below:
Messier 5 (in Serpens Caput constellation)
and
47 Tucanae (in the southern constellation Tucana).
In this side view picture of the Galaxy
the globular clusters are represented by the small circles congregating
around the bulge of the Galaxy (they have been enlarged over a 100 times to
make them visible).
Shapley found a strong concentration of globular clusters
in the direction of the constellation Sagittarius.
Eine Sammlung von Supernova Überresten in LMC.
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Supernovae
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Probably the most promising new distance determination technique involves the
use of Type Ia Supernovae as "Standard Candles".
Type Ia Supernovae are white
dwarf stars in binary systems in which mass is being transferred from an
evolving companion onto the white dwarf. If the amount of matter transferred
is enough to push the white dwarf over the
1.4 M
"Chandrasekhar limit" for
electron-degeneracy support, the white dwarf will begin to collapse under
gravity. Unlike massive stars with iron cores, the white dwarf will have a C/O
core which can undergo further nuclear reactions. The collapse of the white
dwarf liberates enough heat that nuclear reactions ignite and blow the remnant
apart in a thermonuclear deflagration.
These SNIa explosions have all the
right characteristics for Standard Candles; they are:
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extremely bright, outshining the entire galaxy of stars in which they reside.
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easily detected, but very rare, occurring only about once every 100 years in
our galaxy.
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very uniform in brightness at maximum light.
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Hubble's (1929) Velocity-Distance Relation for Nearby Galaxies
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From the work of Slipher in the early part of the 1900's astronomers knew that
most of the spiral nebulae (galaxies) are receding from us. Edwin Hubble
demonstrated that there was a linear relationship between distance and
velocity for galaxies.
The data from Hubble's original velocity-distance relationship. Hubble's
distance scale was in error by a factor of several, but his result was a most
important one, demonstrating that the Universe is expanding and providing a
means of estimating the distances to galaxies at the "edge of the Universe.
Hubble's "law" is
H = v×
D
with the modern value of the slope, H, called the Hubble Parameter (sometimes
called Hubble Constant, but as we shall see it is not constant):
H = 70 km/s×
Mpc.
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