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The Hipparcos Star Globe Booklet - Cosmos
The Hipparcos Star Globe Booklet - Cosmos

... gathered data for four years. The satellite span slowly, controlled in such a way as to gradually shift the axis of rotation so that over time the telescope could repeatedly scan the entire celestial sphere. A simultaneous onboard experiment named Tycho was also to provide astrometric and two-colour ...
SRMP Stars Curriculum - American Museum of Natural History
SRMP Stars Curriculum - American Museum of Natural History

... ACTIVITY: Stellar Temperature and Distance In this activity, students will be given two tables of data – one of nearby stars, and one of bright stars in our sky. There is some overlap in stars, but most of them are separate. The table includes each star’s name, spectral type, apparent and absolute m ...
AAS_winter14rev1final - BU Blogs
AAS_winter14rev1final - BU Blogs

... disk of Epsilon Eridani (K2V, 3.22 pc) in reflected visible light to an inner radius of 1.5 AU (0.5”) from the surface of the star. The first launch of PICTURE suffered a telemetry failure and the primary mirror was shattered upon landing. A new launch is scheduled and the PICTURE payload is currentl ...
Chapter 9 Life and Times on the Main Sequence
Chapter 9 Life and Times on the Main Sequence

... • The assumption that the Sun was formed from a homogenous mixture of gases is motivated by the strong convection expected in the protostar during collapse to the main sequence. • The surface abundances are then assumed to have been undisturbed in the subsequent evolution, so that present surface ab ...
Time, quantum and information
Time, quantum and information

... In the 1920s Eddington formulated the hypothesis that fusion reactions between light elements are the energy source of the stars – a proposition that may be considered as the birth of the field of nuclear astrophysics [1]. It was accompanied by his pioneering work on stellar structure and radiation ...
www.astro.utu.fi
www.astro.utu.fi

... Halo road maps I We can set up test particles following the model, and integrate their orbits for a Hubble time in the Galactic gravitational potential N = 50,000 massless stars in potential due to disk+bulge+dark halo Power law density distribution, velocities as  = (R, ...
ppt - SLAC
ppt - SLAC

... Wolf-Rayet stars are hot (25-50,000+ degrees K), massive stars (20+ solar mass) with a high rate of mass loss. (This is WR124, at 19h11 +16 ) A few other spectral types don't fit the sequence but instead parallel it. Type W or Wolf-Rayet stars are as hot and blue as the hottest O stars but show stro ...
Solutions to Homework #6, AST 203, Spring 2012
Solutions to Homework #6, AST 203, Spring 2012

... c) How many galaxies are there in the observable Universe? Here you can assume that the average distance between galaxies is comparable to the distance between the Milky Way and Andromeda (2.5 mega light-years). Do this calculation for both Universes. (10 points) Solution: Let us assume that the av ...
Topic 2 Chemical Composition of Stars
Topic 2 Chemical Composition of Stars

... Outside of the Solar System abundances can vary due to different factors which include: •  Point in the star’s evolution − for example, some advanced stars can lose the “envelope” of gas around them (we will look more closely at this later in the course) •  Mixing of surface layers •  Certain stars ...
CHP 15
CHP 15

Empirical properties of Very Massive Stars
Empirical properties of Very Massive Stars

50 Years of Quasars
50 Years of Quasars

Equation of State of Dense Matter and the Upper Mass Limit for
Equation of State of Dense Matter and the Upper Mass Limit for

... The theory of dense matter at nuclear and supranuclear densities has developed over several decades and a multitude of papers have been devoted to this subject. Even though we can extrapolate the theory from fits to nuclear phenomena to a description of nuclear matter, basically the parameters must ...
Protogalaxies Encyclopedia of Astronomy & Astrophysics eaa.iop.org S G Djorgovski
Protogalaxies Encyclopedia of Astronomy & Astrophysics eaa.iop.org S G Djorgovski

... minimum amount of energy released by a PG, even with no star formation. A comparable amount of binding energy is released in the collapse of protostars within a PG. There are several possible mechanisms for release of this energy. The gas may be cooling via the inverse Compton effect on the photons ...
Young Stellar Objects in the Orion B Cloud
Young Stellar Objects in the Orion B Cloud

E3 – Stellar distances
E3 – Stellar distances

... Cepheid variables • At distances greater than Mpc, neither parallax nor spectroscopic parallax can be relied upon to measure the distance to a star. • When we observe another galaxy, all of the stars in that galaxy are approximately the same distance away from the earth. What we really need is a li ...
TRIFFID photometry of globular cluster cores – I. Photometric
TRIFFID photometry of globular cluster cores – I. Photometric

Open Problems - Lorentz Center
Open Problems - Lorentz Center

Diapositive 1 - Observatoire de Paris
Diapositive 1 - Observatoire de Paris

... PLATO KO - Paris - November 2010 ...
main sequence stars of a open cluster
main sequence stars of a open cluster

... If a larger value is for N1912Vs.fits, the star is a red-colored one.  Before going forward, quite Makali`i for a time, then start again Makali`i. 4-4. Photometry Many Stars You will photometry about 100 stars for both N1912Bs.fits and N1912Vs.fits. Adjust the viewing so that you can see faint star ...
Absolute magnitudes and kinematics of barium
Absolute magnitudes and kinematics of barium

... (Jorissen & Boffin 1992) and that the orbital period is related to the orbital separation. It may be possible that mild barium stars have wider separations between components, making more difficult the detection of their binary nature. If we consider the stars with known orbits or with variable radi ...
Widener University
Widener University

... b) the escape velocity vesc from this planet, in both m/s and km/s. c) the impact parameter S for a small body falling into this planet at escape velocity. Express in both m and km. d) the impact parameter S for a small body falling into this planet at 100 km/s. Express in m and km. ...
Częstość występowania pierwiastków we Wszechświecie
Częstość występowania pierwiastków we Wszechświecie

... Hydrogen and helium are estimated to make up roughly 74% and 24% of all baryonic matter in the universe respectively. Despite comprising only a very small fraction of the universe, the remaining "heavy elements" can greatly influence astronomical phenomena. Only about 2% (by mass) of the Milky Way g ...
Lab 7
Lab 7

... declination (think of this as a space latitude). The declination runs from -90° (celestial south pole) to +90° (celestial north pole). Both of these coordinates are laminated to the metal pole bases. In addition, the stars have been colored according to their spectral classes; blue balls represent O ...
Protogalaxies
Protogalaxies

... minimum amount of energy released by a PG, even with no star formation. A comparable amount of binding energy is released in the collapse of protostars within a PG. There are several possible mechanisms for release of this energy. The gas may be cooling via the inverse Compton effect on the photons ...
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Stellar evolution



Stellar evolution is the process by which a star changes during its lifetime. Depending on the mass of the star, this lifetime ranges from a few million years for the most massive to trillions of years for the least massive, which is considerably longer than the age of the universe. The table shows the lifetimes of stars as a function of their masses. All stars are born from collapsing clouds of gas and dust, often called nebulae or molecular clouds. Over the course of millions of years, these protostars settle down into a state of equilibrium, becoming what is known as a main-sequence star.Nuclear fusion powers a star for most of its life. Initially the energy is generated by the fusion of hydrogen atoms at the core of the main-sequence star. Later, as the preponderance of atoms at the core becomes helium, stars like the Sun begin to fuse hydrogen along a spherical shell surrounding the core. This process causes the star to gradually grow in size, passing through the subgiant stage until it reaches the red giant phase. Stars with at least half the mass of the Sun can also begin to generate energy through the fusion of helium at their core, whereas more-massive stars can fuse heavier elements along a series of concentric shells. Once a star like the Sun has exhausted its nuclear fuel, its core collapses into a dense white dwarf and the outer layers are expelled as a planetary nebula. Stars with around ten or more times the mass of the Sun can explode in a supernova as their inert iron cores collapse into an extremely dense neutron star or black hole. Although the universe is not old enough for any of the smallest red dwarfs to have reached the end of their lives, stellar models suggest they will slowly become brighter and hotter before running out of hydrogen fuel and becoming low-mass white dwarfs.Stellar evolution is not studied by observing the life of a single star, as most stellar changes occur too slowly to be detected, even over many centuries. Instead, astrophysicists come to understand how stars evolve by observing numerous stars at various points in their lifetime, and by simulating stellar structure using computer models.In June 2015, astronomers reported evidence for Population III stars in the Cosmos Redshift 7 galaxy at z = 6.60. Such stars are likely to have existed in the very early universe (i.e., at high redshift), and may have started the production of chemical elements heavier than hydrogen that are needed for the later formation of planets and life as we know it.
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