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Electromagnetic pulse from final gravitational stellar collapse
Electromagnetic pulse from final gravitational stellar collapse

Kinetics and Numerical Modeling of Competitive Fusion Processes
Kinetics and Numerical Modeling of Competitive Fusion Processes

... temperatures and pressures of a stellar core are suitable for proton-proton fusion—anything less dense or less hot and fusion simply cannot occur due to Coulombic repulsion (this has important implications as to the explanation of pre-stellar mass objects observed in recent years known as brown dwar ...
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chap7 (WP)

... finally emitted from the stellar surface in the form of light and other radiation. This energy, as we discuss in Chap. 11, originates in nuclear reactions that proceed at temperatures much higher than 104 oK. It is estimated from simulations of the generation and transport of energy in the Sun that ...
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슬라이드 1

... Protocluster - in qualitative and quantitative agreement : Spatial extent, specific SFR, gas properties, and so on. Quasar - In agreement with with the models of the later phases of massivegalaxy formation when the quasar becomes visible. Unlike for previously described overdensities at z>5: - Stron ...
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... order of 10-100 Mo undergoing mixing and fallback, or rapidly rotating mega metal-poor (MMP; [Fe/H] < -6.0) stars, both of which eject large amount of CNO, but little heavy metals. Low-mass stars formed with the help of C, O cooling Stars with “normal” carbon and light-element abundances, apparently ...
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... • Global parameters of the star (mass, radius, luminosity, etc.) • Structural and core parameters (Menv, Mcore, core composition, etc) • Constraints for convection, stellar formation & evolution theories... ...
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Star and Earth Chemistry Lecture Notes (PDF

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star - Cloudfront.net

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Chapter 14

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The DBV stars: Progress and problems

... ’whitedwarfs. There are at least two possible progenitors of DB white dwarfs: the PG 1159 stars and the interacting binary white dwarfs. Dehner & Kawaler (1995) show the seismological helium profile of PG 1159-035 can evolve into something similar to what Bradley & Winget (1994) derive for GD 358, b ...
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... by the AIS, due to avoidance of the galactic plane, is young stars. According to Fischer (1998; PhD Thesis, UCSC) only 1% (2/189) of a volume-limited (d < 25 pc) sample of K stars have lithium abundances and chromospheric activity suggesting ages possibly <100 Myr, with an additional 6% (11/189) pla ...
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Astronomy 112: The Physics of Stars Class 1 Notes: Observing Stars

... extended mnemonic Oh Be A Fine Girl/guy, Kiss Me Like That, which proves one thing – astronomers have way too much time on their hands. There has been a theoretical proposal that a new type of spectral class should appear for objects even dimmer than T dwarfs, although no examples of such an object ...
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Introduction to Astronomy and the Celestial Sphere
Introduction to Astronomy and the Celestial Sphere

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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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