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Extreme abundance ratios in the polluted atmosphere of the cool
Extreme abundance ratios in the polluted atmosphere of the cool

The Evryscope: the first full-sky gigapixel-scale telescope Nicholas Law
The Evryscope: the first full-sky gigapixel-scale telescope Nicholas Law

... Transiting exoplanets The nearest & brightest stars Habitable zone of M-dwarfs Asteroids around white dwarfs Confirmation of long-period TESS single-transit detections ...
the red supergiant content of m31
the red supergiant content of m31

... below ∼30Me spend their He-burning lives as red supergiants (RSGs) after passing through a yellow supergiant (YSG) stage during their quick journey across the Hertzsprung–Russell diagram (HRD). At some intermediate masses (∼30Me, say) stars may pass through both a RSG and WR phase, passing through t ...
Gravitational Radiation:
Gravitational Radiation:

... Radiation reaction in source PN corrections to all of these Radiation reaction due to tails of emitted GWs and tails of tails ...
The Evolution of Isotope Ratios in the Milky Way Galaxy
The Evolution of Isotope Ratios in the Milky Way Galaxy

... pattern of the Galaxy at the time when the stars formed. The He core mass is set as Mremnant = 0.459 and 0.473M⊙ for 0.7 and 0.9M⊙ , respectively. Asymptotic Giant Branch (AGB) stars — Stars with initial masses between about 0.8 − 8M⊙ (depending on metallicity) pass through the thermally-pulsing AGB ...
1998 - Universitäts-Sternwarte München
1998 - Universitäts-Sternwarte München

Exposing the hidden white dwarf binary origin by means of a
Exposing the hidden white dwarf binary origin by means of a

... present-day WDs that did not evolve from single stars. While previously single stars and related WD numbers were overestimated, earlier observed WD samples such as that of Holberg, Oswalt & Sion (2002) still suffered from significant incompleteness. That led to a by-chance coincidence in the matchin ...
PDF
PDF

... probably  gives  insight  into  epoch  and  physics  of  formation;   mass  of  PBH  DM  is  typically  the  mass  inside  the  horizon   during  formation  epoch.     Thus  all  efforts  should  be  made  to  discover  PBH  DM   ...


... In the RRL data base of GEOS (2012) one can find a list of 96 times of maxima and the corresponding O-C diagram built with the ephemerides 2419130.305+0.28779276 E is reproduced in Figure 4. Visual observations show a particularly large scatter at HJD ∼ 2443800 which may be due to their larger uncer ...
The Gould Belt
The Gould Belt

... nebulae of the Gould belt. These are dwarfs in late spectral classes with masses of ≈ 1M⊙ and ages of several million years that have not reached the Main sequence stage. Stars have also been identified in terms of their emission in the HJ line, their lithium abundance, xray emission, position in the ...
Validation of the frequency modulation technique applied to the
Validation of the frequency modulation technique applied to the

... Hotter stars in Kepler data are studied less. This is particularly true for the δ Sct and γ Dor stars, where matching models to the observed frequency spectra remains a challenge. Compared with cooler stars, hot stars are not well suited for planetary searches either, for two principal reasons: (i) ...
A CCD Search for Variable Stars of Spectral Type B in the Northern
A CCD Search for Variable Stars of Spectral Type B in the Northern

Stars
Stars

... Just first 2 minutes https://www.youtube.com/watch?v=01U7ZUKVW8o https://www.youtube.com/watch?v=N3IgVidGjQk https://www.youtube.com/watch?v=Rj1sDWjvgjM ...
Modeling the chemical evolution of the Galaxy halo
Modeling the chemical evolution of the Galaxy halo

... unraveling the origin of halo stars through a detailed analysis of their chemical abundances revealed the existence of two distinct halo populations with a systematic difference in [α/Fe], [Cu/Fe], [Zn/Fe] and [Ba/Y], but not in [Mn/Fe], at a given metallicity (Nissen & Schuster 2010, 2011, and refer ...
Chapter 3a powerpoint presentation
Chapter 3a powerpoint presentation

... Also, beware the subscripts are reversed on either side f the equals sign.  Nick Devereux 2006 ...
White dwarf dynamical interactions and fast optical transients
White dwarf dynamical interactions and fast optical transients

... explosions in old white dwarfs belonging to faint globular clusters or dwarf galaxies, which are difficult to detect — see, for instance, Waldman et al. (2011). However, Lyman et al. (2014) obtained deep VLT images of two members of the class (SN 2005E and 2012hn) and found no evidence for any under ...
Massive Star Formation - Max-Planck
Massive Star Formation - Max-Planck

... range of masses from the surrounding, fragmenting clump environment. They then undergo relatively ordered collapse via a central disk to form a single star or a small-N multiple. In this case, the pre-stellar core mass function has a similar form to the stellar initial mass function. In Competitive ...
Origin and Evolution of Neutron Star Magnetic Fields - if
Origin and Evolution of Neutron Star Magnetic Fields - if

discovery of four new massive and dense cold cores
discovery of four new massive and dense cold cores

... conditions for the formation of massive stars at the scale of parsecs is not clear. All of the above surveys have been carried out toward luminous sources, either ultracompact (UC) H ii regions and /or luminous IRAS sources, implying that massive stars have already been formed within the core. For i ...
Excitation of Solar-like Oscillations: From PMS to MS Stellar Models
Excitation of Solar-like Oscillations: From PMS to MS Stellar Models

... (ZAMS), their outer layers have the same properties as their MS counterpart in the HR diagram. For this reason, we expect stochastically excited modes in such objects. Detecting such oscillations would be a valuable way of probing the modeling of such active and very fast rotating young objects. We ...
The Recent Star Formation Histories of M81 Group Dwarf Irregular
The Recent Star Formation Histories of M81 Group Dwarf Irregular

... of the stars, for the larger galaxies, NGC 2366 and Ho II, we observed two fields each, and for IC 2574, an ACS field from the HST Archive was supplemented by two additional fields. The ninth galaxy, the Garland, was also added from the HST archive. Both of these galaxies were observed in the same f ...
Here - Astrophysics Research Institute
Here - Astrophysics Research Institute

Diapositiva 1 - Yale University
Diapositiva 1 - Yale University

... +3.0) in three passbands (BRI), with one colour (R) represented at two epochs. • All SSA global astrometry is tied to the Hipparcos-Tycho reference frame via the Tycho-2 and ACT catalogues. • Astrometry is globally good between 0.2 and 0.3 arcsec. ...
Lecture 39: Early Universe Test 3 overview 11/21
Lecture 39: Early Universe Test 3 overview 11/21

... Cosmology. Hubble law  Universe is expanding, gives universe’s age, depends on Hubble “constant” changes with time. Closed universe has gravity slowing the expansion so it starts to contract. Open universe expands forever. Early universe was very hot and when matter was created. First electrons, pr ...
A variation of the fraction of stars that form in
A variation of the fraction of stars that form in

< 1 ... 46 47 48 49 50 51 52 53 54 ... 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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