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Chapter 22 Neutron Stars and Black Holes
Chapter 22 Neutron Stars and Black Holes

... hole will use up a lot of energy doing so; it cannot slow down, but its wavelength gets longer and longer ...
The abundance of 26Al-rich planetary systems in the Galaxy
The abundance of 26Al-rich planetary systems in the Galaxy

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Universe, Galaxies, and Stars – The Basics

... to yellow… BAM! Rejected! It doesn’t absorb yellow, so that’s what gets reflected to our eyes and that is the color that you see. Last Question: Is it possible to stretch or compress light waves? Answer: YES! Want an example? Think of another kind of wave that you’re very familiar with… sound. Have ...
sections 4-6 instructor notes
sections 4-6 instructor notes

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Population synthesis of Be/white dwarf binaries in the Galaxy
Population synthesis of Be/white dwarf binaries in the Galaxy

... star. This hydrodynamical mechanism was devised because, in the whole early spectral range, synchronous rotators and circular orbits are observed in main-sequence binaries with orbital periods substantially larger than previously thought possible. In a recent paper, Rieutord & Zahn (1997) claim to h ...
A substellar component orbiting the F
A substellar component orbiting the F

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J. A. Caballero`s Humboldt-Foundation Renewed Research Stay in
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A binary merger origin for inflated hot Jupiter planets
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Rotation - Indiana University Astronomy
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The LMC transition star R84 and the core of the LH 39 OB association
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... Luminous Blue Variable (LBV) phenomenon (Stahl et al. 1983) which, according to current massive star evolutionary models (Maeder 1989, Langer et al. 1994) represents a short stage in the evolution of O stars initially more massive than 60 M⊙ before the advent of the Wolf-Rayet phase. In fact Ofpe/WN ...
Star Systems - Palm Beach State College
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Article PDF - IOPscience
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Bellwork: Degenerate Matter (A review form yesterday)
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Winds of Main-Sequence Stars - Harvard

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model of convection

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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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