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The effects of red supergiant mass loss on
The effects of red supergiant mass loss on

... lower than the escape velocity from the stellar photosphere, v esc ∼ 100 km s−1 . He assessed the possibility that radiation pressure on the circumstellar ions (and atoms) could drive the wind until the local escape velocity would have dropped below the wind speed, but the values for the achieved ac ...
Review: How does a star`s mass determine its life story?
Review: How does a star`s mass determine its life story?

Chapter 5 Stellar Energy Production
Chapter 5 Stellar Energy Production

N Brickhouse
N Brickhouse

... • How does the magnetic field evolve? • Do turbulent “hot spots” develop on more massive accretors? • What MHD processes drive stellar and/or disk outflows? • How does the magnetic field connect star and disk? Donati et al. 2008 ...
FP11: DRAKE et al. - Astronomical Institute WWW Homepage
FP11: DRAKE et al. - Astronomical Institute WWW Homepage

... Figure 3 shows spectra of HD 3980 in the Li I 6708 Å spectral region. The rotational phases of HD 3980 were calculated using the ephemeris from Maitzen et al. (1980). Two “Li spots” are observed on the surface of the star. The Li I line originated in spot 1 appears at the phase φ = – 0.146 = 0.832 a ...
Leverhulme lectures on stellar magnetism. 1. Overview
Leverhulme lectures on stellar magnetism. 1. Overview

... dichroic. Right and left circularly polarised light will be absorbed differently, and the continuum radiation will be circularly polarised by a field that has large component along the line of sight. Observable continuum circular polarisation is found above about 10 MG. For still larger fields (abov ...
BRC_prop1 - CoolWiki
BRC_prop1 - CoolWiki

... ignition of a very hot star nearby, collision with another molecular cloud, or ...
Galaxies - Center for Astrostatistics
Galaxies - Center for Astrostatistics

the magellanic clouds newsletter - Keele University Astrophysics
the magellanic clouds newsletter - Keele University Astrophysics

Wroclaw_VanGrootel
Wroclaw_VanGrootel

... > Tassoul & Tassoul (e.g. 1992; large scale hydrodynamical currents) ...
G040141-00 - DCC
G040141-00 - DCC

... – 3 decades after pulsars are discovered we don’t fully understand why pulsars pulse or glitch – Observing normal modes in neutron stars, combined with radio observations, could teach us about glitches, equation-of-state of high-density neutrons (or other matter) ...
Stars in the Sky Stars in the Sky
Stars in the Sky Stars in the Sky

–1– 2. Milky Way We know a great deal, perhaps more than any
–1– 2. Milky Way We know a great deal, perhaps more than any

ISOLATED, MASSIVE SUPERGIANTS NEAR THE GALACTIC
ISOLATED, MASSIVE SUPERGIANTS NEAR THE GALACTIC

Key paper.
Key paper.

... letters to nature flux density, d is the distance to the source, and Bn is the blackbody Planck intensity. We can improve on this estimate by using a model14,15 in which radial disk temperature and density are allowed to vary as power laws. The exponent, 0.61, of the radial profile in disk temperat ...
Entropy
Entropy

... coordinates of effective temperature Teff versus luminosity L. Stars tend to fall only into certain regions of the HR diagram. About 90% of the observed stars belong to the main sequence that represents a narrow strip running from hot stars with high luminosity to brown dwarfs with low luminosity. T ...
Cosmology
Cosmology

... formed as hot, primordial energy cools and forms into matter can be predicted by physical laws The fraction of helium in the Universe can be measured with observations The observed abundances of elements support the predictions of the Big Bang theory ...
The Initial Mass Function (IMF) Continued
The Initial Mass Function (IMF) Continued

Document
Document

The Big Bang - Community Resources for Science
The Big Bang - Community Resources for Science

... This is picture made by the Hubble telescope. This star is many times larger than the sun and has used fuel very quickly and has started to collapse. And just like the whoopee cushion it is jetting off gas (only from both ends). This star may eventually become what is known as a supernova. A super- ...
Measurements of Neutron Star Masses
Measurements of Neutron Star Masses

... phase of hadronic and deconfined quark matter they are almost touching. At somewhat lower develops (34), even if strange quark matter is densities, the nuclear lattice can turn insidenot the ultimate ground state of matter. Delinout and form a lattice of voids, which is eating the phase structure of ...
The Transient Radio Sky Astrophysical and Artificial
The Transient Radio Sky Astrophysical and Artificial

... 1148+5651: Hyperluminous IR galaxies  Detect low order CO emission in seconds, including imaging on subkpc scales.  Detect high dipole moment molecules (HCO+, HCN…) in minutes (critical densities > 1e5 cm^-3).  Image non-thermal emission associated with star formation and/or AGN at mas resolution ...
Primas
Primas

A New Hypothesis On The Origin and Formation of The Solar And
A New Hypothesis On The Origin and Formation of The Solar And

... that HD 106906b (11 MJupiter ) are located at a very large distance 650 AU to its parent star HD 106906 (K-type star) with only 13 million years age (Bailey etal. 2013), and PSO J318.5-22 is a free-floating gas giant (6.5 MJupiter ) formed without a parent star 12 million years ago (Liu et al. 2013) ...
Spectral classification of blue supergiants in M31
Spectral classification of blue supergiants in M31

< 1 ... 92 93 94 95 96 97 98 99 100 ... 410 >

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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