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Munshi_washington_0250E_12611
Munshi_washington_0250E_12611

... Anyalysis of mass recovered as a function of stellar population age when using M/L ratios to estimate stellar mass. In this figure, we use B-V color, as in the analysis for the SMHM relation. The first point is so high because the stellar population is so old that the B-V colors are undefined. The x ...
discovery of four new massive and dense cold cores
discovery of four new massive and dense cold cores

... single-dish telescopes have shown that massive stars form in regions of molecular gas with distinctive physical parameters, which we refer to as massive dense cores.1 For example, from observations of the CS (5 ! 4) line emission toward massive star–forming regions associated with H2O masers, Plume ...
Testing the Initial-Final Mass Relationship of White Dwarfs Silvia Catal´ an Ruiz
Testing the Initial-Final Mass Relationship of White Dwarfs Silvia Catal´ an Ruiz

... constraints can be observationally derived. Since this method involves the use of theoretical stellar evolutionary tracks the resulting initial-final mass relationship is, in fact, semi-empirical. From an observational perspective, the statistical significance of the current semiempirical initial-fi ...
Observed Properties of Exoplanets: Masses, Orbits, and Metallicities
Observed Properties of Exoplanets: Masses, Orbits, and Metallicities

... FGKM dwarfs at the Lick, Keck 1, and Anglo-Australian telescopes. The majority of stars had their first high-quality measurement between 1995 and 1998, giving a time coverage of ∼7–10 years thus far. The target stars and their properties are available,81), 88) and were drawn from the Hipparcos catal ...
Tidal Disruptions of White Dwarfs from Ultra
Tidal Disruptions of White Dwarfs from Ultra

... incoming star. Thus the disk formed from the tidal debris will have angular momentum that is also misaligned with the BH spin direction (Rees 1988). For thin disks, the BardeenPetterson effect will align the BH spin with the angular momentum of the inner region of the disk (Bardeen & Petterson 1975) ...
Determination of the position angle of stellar spin axes
Determination of the position angle of stellar spin axes

... As an intrinsic 1D stellar spectrum, we took a synthetic phoenix spectrum (Hauschildt & Baron (2005)) calculated for a cool giant like Aldebaran using the following parameters: an effective temperature of 4 000K, a surface gravity log(g) = 1.8, and solarlike metallicity. It was calculated under the ...
A Legacy Study of Stellar Life Cycles in the Galactic Center
A Legacy Study of Stellar Life Cycles in the Galactic Center

... Sgr A* currently has a quiescent X-ray luminosity of ~2x1033 erg s-1 or ~10-10 Ledd Flares daily by 10-100x for <~ few hrs Fluorescent Fe features in the central 6’ suggest Sgr A* may have been >~ 1038 erg s-1 for at least 2-3 yr about 60 yr ago, before the first X-ray satellites were launched; howe ...
Properties of rapidly rotating PNS with antikaon condensates at
Properties of rapidly rotating PNS with antikaon condensates at

... that Bose-Einstein condensates such as those of pions and/or antikaons are favourable to appear at highly dense NS cores[8, 9]. The appearance of new particles such as antikaon condensates results in the softening of matter EoS as negatively charged leptons are replaced by the slow-moving massive co ...
Binary evolution using the theory of osculating orbits
Binary evolution using the theory of osculating orbits

... the perturbing forces acting on the orbit of each star arising from mass exchange via Roche lobe overflow. The scheme is compared to results calculated from a “classical” prescription. Methods. Using our stellar binary evolution code BINSTAR, we calculate the orbital evolution of Algol binaries unde ...
Modelling the observed properties of carbon-enhanced metal
Modelling the observed properties of carbon-enhanced metal

... distribution, and the binary fraction. We vary the assumptions in our model about these parameters, as well as the wind mass-transfer process, and study the consequent variations of our synthetic CEMP population. The CEMP fractions calculated in our synthetic populations vary between 7% and 17%, a r ...
Physics of the Interstellar and Intergalactic Medium
Physics of the Interstellar and Intergalactic Medium

... 2.1 Consider an electron-proton plasma at temperature T . Let ts (e − e) be the time scale for 90 degree scattering of one electron with kinetic energy ∼ kT by encounters with other electrons. The electron-proton mass ratio mp /me = 1836. The following time scales tx will differ from ts (e − e) by f ...
FY1995 Q1 Oct-Dec NO.. - National Optical Astronomy Observatory
FY1995 Q1 Oct-Dec NO.. - National Optical Astronomy Observatory

... elements compared to hydrogen is constant from star to star. This suggests that the cluster formation was rapid, occurring in less than the characteristic time for heavy metal enrichment by Type II supernovae. (In fact, the energetics of these supernovae may have been responsible for clearing the ga ...
6th Grade The Theoretical Beginning of the Universe / Big Bang
6th Grade The Theoretical Beginning of the Universe / Big Bang

... Earth by looking at its brightness. Hubble used a number of methods to estimate how far away each star is. But he did much more. He used the color of each star's light to determine which direction they are moving...and how fast. ...
Leaky Stars: Pulsations, Waves, and Turbulence in Stellar Winds
Leaky Stars: Pulsations, Waves, and Turbulence in Stellar Winds

... • Exterior: continuous ...
Presentation on the universe
Presentation on the universe

... previous video) or how far away in space something is, scientists measure not with meters or miles, but rather by using light-years. A light-year is the distance a beam of light travels in one year. ...
radioactive 26a1 in the galaxy: observations versus theory
radioactive 26a1 in the galaxy: observations versus theory

... estimated (a rather rare case in astronomy); it required a large ratio of 26A1/27A1 from supernovae, larger than what was obtained from supernova models in the early 80ies. Based on galactic chemical evolution arguments, Clayton [27] pointed out that supernovae, the main producers of the stable isot ...
Constraining the Warm Dark Matter Particle Mass through Ultra
Constraining the Warm Dark Matter Particle Mass through Ultra

... their mixing with active neutrinos through the Dodelson & Widrow (1994) mechanism; ii) resonant production including the case of lepton asymmetry (Shi & Fuller 1999); iii) coupling with other fields (Kusenko 2009; Shaposhnikov & Tkachev 2006). Several astrophysical constraints are leading to a rathe ...
molecular cloud evolution. ii. from cloud formation to the
molecular cloud evolution. ii. from cloud formation to the

... of the collision of gas streams (‘‘inflows’’) in the WNM at moderately supersonic velocities. The collisions cause compression, cooling, and turbulence generation in the gas, forming a cloud that then becomes self-gravitating and begins to collapse globally. Simultaneously, the turbulent, nonlinear ...
The Binary Populations of Eight Globular Clusters in the Outer Halo
The Binary Populations of Eight Globular Clusters in the Outer Halo

... We exploit three indexes provided by the adopted software and described in detail by Anderson et al. (2008) as diagnostics of photometric quality: the fraction of flux in the stellar aperture from its neighbours (o), the fractional residuals in the fit of the PSF to the pixel (q), and the rms of the ...
The Space Density of Spiral Galaxies as f(magnitude, size and
The Space Density of Spiral Galaxies as f(magnitude, size and

... and the Structural luminosity, scale size, Chemical Evolution within galaxies? surface brightness, mass,disk velocity distribution – current star formation in disks semi-regular, related to morphology andstudies: structural parameters Statistical scaling relations – are spirals determined by initial ...
400 YEARS OF STELLAR ROTATION - DFTE
400 YEARS OF STELLAR ROTATION - DFTE

... In 1609 the news reached Venice that a certain Flemish optician had built a special spyglass through which it was possible to see distant objects closer with a magnification of about 4 times. Galileo (or some friends of him) was able just on empirical basis to quickly push the magnification first to ...
What causes the large extensions of red supergiant
What causes the large extensions of red supergiant

... The normalized flux spectra show typical spectra of RSGs in the K band (cf. Lançon et al. 2007; Arroyo-Torres et al. 2013). The flux variations at wavelengths below about 2.0 μm are due to a higher noise level, possibly caused by the lower atmospheric transmission. In the K-2.3 band, we observe a de ...
The European Large Area ISO Survey – IV. The preliminary 90
The European Large Area ISO Survey – IV. The preliminary 90

... function defined below and are excluded from the luminosity function analysis. Two galaxies (ELAISP90_J003721-434228 and ELAISP90_J003021-423657) are Seyfert 2 galaxies, and two further galaxies (ELAISP90_J003431-433806 and ELAISP90_ J003133-425100) have an early-type spectrum; all the remainder (in ...
AN EXPERT COMPUTER PROGRAM FOR CLASSIFYING STARS
AN EXPERT COMPUTER PROGRAM FOR CLASSIFYING STARS

... The MK Classification System, first devised by Morgan et al. (1943), classifies stars by direct comparison with MK standard stars. The most recent detailed discussion of the MK system is that of Gray & Corbally (2009); that reference also has an appendix with extensive lists of MK standard stars. Th ...
The mass of the Milky Way: Limits from a newly assembled set of
The mass of the Milky Way: Limits from a newly assembled set of

... up to distances of 10 kpc from the Sun. Roughly half of the objects in this sample have measured proper motions, permitting the use of their full space motions in our analysis. In order to bind these sample objects to the Galaxy, their rest-frame velocities must be lower than their escape velocities ...
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Main sequence



In astronomy, the main sequence is a continuous and distinctive band of stars that appears on plots of stellar color versus brightness. These color-magnitude plots are known as Hertzsprung–Russell diagrams after their co-developers, Ejnar Hertzsprung and Henry Norris Russell. Stars on this band are known as main-sequence stars or ""dwarf"" stars.After a star has formed, it generates thermal energy in the dense core region through the nuclear fusion of hydrogen atoms into helium. During this stage of the star's lifetime, it is located along the main sequence at a position determined primarily by its mass, but also based upon its chemical composition and other factors. All main-sequence stars are in hydrostatic equilibrium, where outward thermal pressure from the hot core is balanced by the inward pressure of gravitational collapse from the overlying layers. The strong dependence of the rate of energy generation in the core on the temperature and pressure helps to sustain this balance. Energy generated at the core makes its way to the surface and is radiated away at the photosphere. The energy is carried by either radiation or convection, with the latter occurring in regions with steeper temperature gradients, higher opacity or both.The main sequence is sometimes divided into upper and lower parts, based on the dominant process that a star uses to generate energy. Stars below about 1.5 times the mass of the Sun (or 1.5 solar masses (M☉)) primarily fuse hydrogen atoms together in a series of stages to form helium, a sequence called the proton–proton chain. Above this mass, in the upper main sequence, the nuclear fusion process mainly uses atoms of carbon, nitrogen and oxygen as intermediaries in the CNO cycle that produces helium from hydrogen atoms. Main-sequence stars with more than two solar masses undergo convection in their core regions, which acts to stir up the newly created helium and maintain the proportion of fuel needed for fusion to occur. Below this mass, stars have cores that are entirely radiative with convective zones near the surface. With decreasing stellar mass, the proportion of the star forming a convective envelope steadily increases, whereas main-sequence stars below 0.4 M☉ undergo convection throughout their mass. When core convection does not occur, a helium-rich core develops surrounded by an outer layer of hydrogen.In general, the more massive a star is, the shorter its lifespan on the main sequence. After the hydrogen fuel at the core has been consumed, the star evolves away from the main sequence on the HR diagram. The behavior of a star now depends on its mass, with stars below 0.23 M☉ becoming white dwarfs directly, whereas stars with up to ten solar masses pass through a red giant stage. More massive stars can explode as a supernova, or collapse directly into a black hole.
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