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Metallicity maps
Metallicity maps

... but ram-pressure stripping is very important), they yield different metal distributions and have different time scales  ram-pressure in the outskirts of clusters is sufficient to strip gas and form new stars  inhomogeneous metallicity distribution, enriched material is not mixed immediately with I ...
The Milky Way Galaxy 1 Introduction 2 Globular Clusters and
The Milky Way Galaxy 1 Introduction 2 Globular Clusters and

... ˆ Who first observed that the Milky Way is made up of an enormous number of stars? When did this occur, and what was the significance of the observation? ...
The Milky Way galaxy Contents Summary
The Milky Way galaxy Contents Summary

... them to drift inwards. The outward thrust from the bar and the frictional inward drift balance just outside rcr , and gas accumulates here. This accumulation of gas near rcr is conspicuous in the lower panel of Figure 8 as a band of emission that slopes from upper left to lower right at |l| < 25◦ . ...
LIDAR Imaging Detector Could Build `Super Road Maps` of Planets
LIDAR Imaging Detector Could Build `Super Road Maps` of Planets

... operational flexibility. All of these benefits will lead to lower mission cost and greater scientific productivity. Our design efforts will enable a broad range of applications, including demanding hyper-spectral imaging in the most severe radiation environments in the Solar system. They will help N ...
The impact of X-rays on molecular cloud fragmentation and the IMF
The impact of X-rays on molecular cloud fragmentation and the IMF

... that sink particles are created in the compressed cloud edge much earlier than in the shielded and colder parts. A phase diagram is plotted in Fig. 3.3 that shows the decline of temperature as the density increases. The secondary band with a steep decrease in temperature at low densities is the dire ...
THE MYSTERIOUS SICKLE OBJECT IN THE CARINA NEBULA: A
THE MYSTERIOUS SICKLE OBJECT IN THE CARINA NEBULA: A

... close to the tip of the Sickle. The position of the peak of the sub-mm emission is 10h 44m 04.06s , −59◦ 33′ 35.5′′ , i.e. 10 arcseconds (or 0.1 pc) north-west of the star MJ 218 and about 3 arcseconds north-west of the apex point of the Sickle nebula. The sub-mm emission is almost point-like and on ...
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Circumstellar grains: radiation pressure and

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... for the longer-period evolved variables. (More exact values will be computed in a later section of this paper.) Such period changes should be observable. There have been several comparisons between theoretical and observed period changes. The careful compilation by Percy et al. (1980) led to inconcl ...
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Rapid Rotation of Low-Mass Red Giants Using APOKASC: A
Rapid Rotation of Low-Mass Red Giants Using APOKASC: A

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THE DISRUPTION OF STELLAR CLUSTERS CONTAINING

... is part of the collapsing core, we add its mass to a growing central point mass and remove it from the simulation. This central point mass is then used only during the calculation of the cluster gravitational potential. We determine whether a star is part of the collapsing core by monitoring its orb ...
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Spin-Driven Changes in Neutron Star Magnetic Fields
Spin-Driven Changes in Neutron Star Magnetic Fields

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1Lec_1 - The University of Texas at Dallas
1Lec_1 - The University of Texas at Dallas

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$doc.title

... are  s5ll  significant  uncertain5es  in  X-­‐ray   radia5ve  transfer  (porosity;  resonance   scatering)  that  require  further  explora5on   •  Even  a  limited  sample  has  a  big  impact  on  the   field  because  of  the  large  syste ...
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The age structure of the Milky Way`s halo

... on the ages of the stellar populations in the halo of the Milky Way based on the colours of a class of stars known as field blue horizontal-branch (BHB) stars19. Originally identified because of their distinctive position in the colour-magnitude diagrams of globular clusters, BHB stars are less mass ...
Word - Department of Physics - Hong Kong University of Science
Word - Department of Physics - Hong Kong University of Science

... To correct this situation, we have initialized the velocities of the particles of the red giant to be due to the translational motion of the centre of mass of the red giant, plus the rotational motion with respect to the centre of mass of the red giant too. The angular velocity of the rotational mo ...
Chemical composition of halo and disk stars with
Chemical composition of halo and disk stars with

... by fitting Gaussians to the lines. Since only rather weak lines were included, this gives a higher accuracy than area integration, which is more affected by blends in the outer parts of the lines. Altogether 13 halo stars and 16 disk stars were observed. Most of them have magnitudes between mV = 9 a ...
Cluster formation in molecular clouds – I. Stellar populations, star
Cluster formation in molecular clouds – I. Stellar populations, star

... fixed output that does not change with time. As an example, the luminosity of a cluster can be determined from its mass via an averaged IMF (Murray, Quataert & Thompson 2010). This simplified approach misses key aspects of the star formation process. As an attempt to bridge the gap between these two ...
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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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