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G030163-03 - DCC
G030163-03 - DCC

... Search for binaries with neutron stars and/or black holes Rate limits or detections of binary inspirals beyond Virgo cluster: – Constraint on stellar evolution and faint pulsar population – Measurement of neutron star size and equation of state – Determine if neutron star disruption causes -ray bur ...
The Chemical Composition of an Extrasolar Kuiper-Belt
The Chemical Composition of an Extrasolar Kuiper-Belt

Rosolowsky
Rosolowsky

... 2. Another factor [f(R)] determines what fraction of these clouds are converted to molecular gas 3. Different environments create different mass distributions of bound molecular clouds. ...
Metallicity, Age, and Mass of Star Forming Galaxies at z~3
Metallicity, Age, and Mass of Star Forming Galaxies at z~3

... Aging z>4 exLBG should be visible in the HDF images as red sources. There are no such galaxies. But we do see z>4 LBGs. Where are they at Z~3? Recurrent SF? Just bad luck in The HDF? ...
The Milky Way galaxy Contents Summary
The Milky Way galaxy Contents Summary

... billions of stars. The smaller galaxies are much more numerous than the larger ones, but not by a sufficient factor to compensate for their lower luminosities. So most of the luminosity in the Universe is contributed by galaxies that lie just below the top of the scale. The Sun lies in just such a g ...
Draft paper (submitted to MNRAS)
Draft paper (submitted to MNRAS)

... We explore the impact of cosmic reionization on nearby isolated dwarf galaxies using a compilation of star formation histories estimated from deep HST data and a cosmological hydrodynamical simulation of the Local Group. The nearby dwarfs show a wide diversity of star formation histories; from ancie ...
Cygnus X-2, super-Eddington mass transfer, and pulsar binaries
Cygnus X-2, super-Eddington mass transfer, and pulsar binaries

Who’s Afraid of a Stellar Superflare? Rachel Osten GSFC
Who’s Afraid of a Stellar Superflare? Rachel Osten GSFC

... superflaring in normal stars -- Schaefer et al. (2000) normal solar-like stars undergoing flaring events with energy releases 1033-1038 ergs, occurring roughly once every 100 years or so ...
Chapter 5 Energy transport in stellar interiors
Chapter 5 Energy transport in stellar interiors

Monthly Target Matrix Excel
Monthly Target Matrix Excel

... Each month the sky presents us with a dazzling assortment of spectacular objects on which to train our telescopes: variable stars, nebulae, galaxies, and clusters of galaxies, to name a few. As the Earth makes its yearly trip aroundthe Sun, different objects slide into view in the nighttime sky. Any ...
Implications for dwarf spheroidal mass content from interloper removal
Implications for dwarf spheroidal mass content from interloper removal

... removal of significant numbers of potential interlopers and enabled them to find consistent mass-follows-light models that fit the data. An alternative to these methods is the caustic technique which utilises the three known phase-space coordinates to delineate caustics (escape speed curves) in the ...
Observational studies of stellar rotation
Observational studies of stellar rotation

... N.B. If ω(r) = Ω∗ , J = IΩ∗ = k 2 M∗ R∗2 Ω∗ , where kR∗ is the stellar radius of gyration‡ ...
Resultados del Concurso 2008A para Observaciones en
Resultados del Concurso 2008A para Observaciones en

Slide - Fort Lewis College
Slide - Fort Lewis College

... High-Mass Evolutionary Tracks ...
Interpretation of the Helix Planetary Nebula using Hydro
Interpretation of the Helix Planetary Nebula using Hydro

... may collapse from inadequate radial mass mixing, giving a SNe Ia event. Modest star growth may be even more dangerous because enhanced turbulence may mix and burn the carbon core but not mix the resulting incombustible iron core, which explodes at 1.4M to form a neutron star in a supernova II event ...
Rapid Rotation of Low-Mass Red Giants Using APOKASC: A
Rapid Rotation of Low-Mass Red Giants Using APOKASC: A

... the cross-correlation peak between the observed spectrum and its template to the width of the cross-correlation peak between the template and an artificially rotationally broadened version of the template, a rotational broadening is determined (see White & Hillenbrand 2004, with additions by Will Fi ...
Chemical Composition and Evolutionary Status of the Ap Star HD
Chemical Composition and Evolutionary Status of the Ap Star HD

... names of the elements and their ionization stages, wavelengths, the corresponding excitation energies, oscillator strengths, damping parameters, Lande factors, and central depths of the lines, an additional list is used in this version of the code. It provides the hyperfine structure constants for th ...
The National Ignition Facility and Basic Science
The National Ignition Facility and Basic Science

... The NRC committee on the Physics of the Universe highlighted the new frontier of HED Science Eleven science questions for the new century: 2. What is the nature of dark energy? — Type 1A SNe (burn, hydro, rad flow, EOS, opacities) ...
flyer
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... compared to the star's radius, r, so ε ∼ Δr/r. But, technically this is a ratio of the difference between two perpendicular moments of inertia and the third perpendicular, principal, moment of inertia. Sensitivity: A description of a detector's ability to detect a signal. Detectors with lower noise ...
Astronomy 401 Lecture 8 Spiral Galaxies II 1 The Tully
Astronomy 401 Lecture 8 Spiral Galaxies II 1 The Tully

... • Stellar orbits about the center of the galaxy aren’t perfectly circular (we saw before that the Sun has a peculiar velocity (the solar motion) with respect to the local standard of rest). • We can describe these orbits as motion about an equilibrium position that is moving in a perfectly circular ...
Gamma-ray absorption and pair echos at very high
Gamma-ray absorption and pair echos at very high

... filtering mass prescription of [15], and which give nearly equally good fits to the existing high-z observations. ...
3.2 Black body Radiation
3.2 Black body Radiation

... Almost all astronomical information from beyond the Solar System comes to us from some form of electromagnetic radiation (EMR). (Can you think of any sources of information from beyond the Solar system that do not involve EMR in some form?) We can now detect and study EMR over a range of wavelength ...
On the role of the WNH phase in the evolution of very massive stars
On the role of the WNH phase in the evolution of very massive stars

ASTR 001 Introduction to the Cosmos
ASTR 001 Introduction to the Cosmos

... 1. At a certain point in the Universes history, the density of matter in the Universe was 64 times larger than it is today while the energy density of radiation in the Universe at that time was 256 times than what it is today. This means the the average distance between galaxies at that time was A) ...
SS_L1
SS_L1

... Our theory of stellar structure must reproduce both these results ...
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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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