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The extreme physical properties of the CoRoT-7b super
The extreme physical properties of the CoRoT-7b super

document
document

... Thought Question What happens in a low-mass star when core temperature rises enough for helium fusion to begin? A. Helium fusion slowly starts up. B. Hydrogen fusion stops. C. Helium fusion rises very sharply. (Hint: Degeneracy pressure is the main form of pressure in the inert helium core.) ...
the printable Observing Olympics Object Info Sheet in pdf
the printable Observing Olympics Object Info Sheet in pdf

... nebula has been expanding at a constant rate of 10 milli-arcseconds a year, then it would take 1000 ± 260 years to reach a diameter of 20 arcseconds. This may be an upper limit to the age, because ejected material will be slowed when it encounters material ejected from the star at earlier stages of ...
3P31.pdf
3P31.pdf

... phenomenon is a powerful tool to study the kinematics of the environment of young stellar objects (YSOs) at high angular and spectral resolution. ...
Galaxy Questions Info
Galaxy Questions Info

... Spiral arms — Curved extensions beginning at the bulge of a spiral galaxy, giving it a "pinwheel" appearance. Spiral arms contain a lot of gas and dust as well as young blue stars. Spiral arms are found only in spiral galaxies. Halo — The halo primarily contains individual old stars and clusters of ...
Non-thermal hard X-ray emission from stellar coronae
Non-thermal hard X-ray emission from stellar coronae

... (deep sensitivity and hard X-ray fine imaging required: NXHM OK, NuSTAR No, ASTRO-H No) ...
Galaxy5
Galaxy5

Killer Skies
Killer Skies

... billion Kelvin. This pattern of core ignition and shell ignition continues with a series of heavier nuclei as fusion fuel. At higher temperatures than carbon fusion, nuclei of oxygen, neon, and magnesium fuse to make silicon and sulfur. At even higher temperatures, silicon can fuse to make iron. Thu ...
Star Formation in Our Galaxy - Wiley-VCH
Star Formation in Our Galaxy - Wiley-VCH

Document
Document

Publisher: Emily Barrosse Acquisitions Editor: Kelley Tyner
Publisher: Emily Barrosse Acquisitions Editor: Kelley Tyner

... core will heat up again. Hydrogen will begin “burning” in a shell around the core. (The process is nuclear fusion, not the chemical burning we have on Earth.) The new energy will cause the outer layers of the star to swell by a factor of 10 or more. They will become very large, so large that when th ...
Effects of Mutual Transits by Extrasolar Planet
Effects of Mutual Transits by Extrasolar Planet

... material inflow to the satellites and the satellite loss through orbital decay driven by the gas. They suggested that similar processes could limit the largest satellite of extrasolar giant planets. Such theoretical predictions await future observational tests. There still remains a possibility to d ...
The masses of stars
The masses of stars

... mass stars are thought to be much more common than those of high mass. The lower limit of about 8% of a Solar mass comes about because objects of lesser mass never achieve a high enough core temperature for nuclear fusion to begin. Low mass objects are thought to commonly form in the same way as, an ...
Evolution in circumstellar envelopes of Be stars: From disks to rings?
Evolution in circumstellar envelopes of Be stars: From disks to rings?

... the conventional, static picture of the disk being in quasi-contact with the central star is justified primarily (or perhaps only) after an outburst event. Some weeks to months later, a low-density region seems to develop above the star and slowly grows outwards. A subsequent outburst may later repl ...
Small Bodies in the Outer Solar System
Small Bodies in the Outer Solar System

Astronomy 112: The Physics of Stars Class 16 Notes: Post
Astronomy 112: The Physics of Stars Class 16 Notes: Post

... the Schönberg-Chandrasekhar limit. This does not stop it from heating up, but it does change what happens once the He ignites. Recall our discussion of runaway nuclear burning instability. In a degenerate gas, the pressure and density are not connected to the temperature. As a result, once a nuclea ...
Document
Document

... You need a reference point source (star) for the wavefront measurement. The reference star must be within the isoplanatic angle, of about 10-30 arcseconds If there is no bright (mag ~ 14-15) nearby star then you must use an artificial star or „laser guide star“. All laser guide AO systems use a sodi ...
Particle-Gas Dynamics and Primary Accretion
Particle-Gas Dynamics and Primary Accretion

... underestimate the disk mass once particles have grown past millimeter size. The concept of the minimum mass nebula (MMN) (e.g., Hayashi, 1981; Hayashi et al., 1985) is a handy benchmark, but has no solid physical basis and (by construction) is an underestimate to the degree that solids were lost eit ...
Encyclopedia of Optical Engineering Stellar Evolution
Encyclopedia of Optical Engineering Stellar Evolution

... The first phase of stellar birth is the gravitational collapse of small mass concentrations in a nebula. The process is quite rapid, taking only a few thousand years to form a protostar cloud, which is about the size of the solar system. At this point, the increase in temperature, pressure, and dens ...
neutron star.
neutron star.

... • As a white dwarf’s mass approaches 1.4MSun, its electrons must move at nearly the speed of light. • Because nothing can move faster than light, a white dwarf cannot be more massive than 1.4MSun, the white dwarf limit (also known as the Chandrasekhar limit). ...
Planetary internal structures
Planetary internal structures

... the first planetary system around a star other than the Sun, namely a pulsar (Wolszczan and Frail, 1992) and the first Jupiter-mass companion to a solar-type star (Mayor and Queloz, 1995). Before that, the development and application of planetary structure theory was restricted to the few planets be ...
Timescales for the evolution of oxygen isotope compositions in the
Timescales for the evolution of oxygen isotope compositions in the

Chapter 12
Chapter 12

Chapter 17
Chapter 17

Primary and secondary eclipse spectroscopy with JWST: exploring
Primary and secondary eclipse spectroscopy with JWST: exploring

... atmosphere of hot jupiters and neptunes. At the same time, ∼40 likely large terrestrial planets are announced or confirmed. Two of these are transiting, and another is deemed habitable. Therefore the potential for eclipse spectroscopy of terrestrial planets with the James Webb Space Telescope (JWST) ...
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Nebular hypothesis

The nebular hypothesis is the most widely accepted model in the field of cosmogony to explain the formation and evolution of the Solar System. It suggests that the Solar System formed from nebulous material. The theory was developed by Immanuel Kant and published in his Universal Natural History and Theory of the Heaven. Originally applied to our own Solar System, this process of planetary system formation is now thought to be at work throughout the universe. The widely accepted modern variant of the nebular hypothesis is the solar nebular disk model (SNDM) or simply solar nebular model. This nebular hypothesis offered explanations for a variety of properties of the Solar System, including the nearly circular and coplanar orbits of the planets, and their motion in the same direction as the Sun's rotation. Some elements of the nebular hypothesis are echoed in modern theories of planetary formation, but most elements have been superseded.According to the nebular hypothesis, stars form in massive and dense clouds of molecular hydrogen—giant molecular clouds (GMC). These clouds are gravitationally unstable, and matter coalesces within them to smaller denser clumps, which then rotate, collapse, and form stars. Star formation is a complex process, which always produces a gaseous protoplanetary disk around the young star. This may give birth to planets in certain circumstances, which are not well known. Thus the formation of planetary systems is thought to be a natural result of star formation. A Sun-like star usually takes approximately 1 million years to form, with the protoplanetary disk evolving into a planetary system over the next 10-100 million years.The protoplanetary disk is an accretion disk that feeds the central star. Initially very hot, the disk later cools in what is known as the T tauri star stage; here, formation of small dust grains made of rocks and ice is possible. The grains eventually may coagulate into kilometer-sized planetesimals. If the disk is massive enough, the runaway accretions begin, resulting in the rapid—100,000 to 300,000 years—formation of Moon- to Mars-sized planetary embryos. Near the star, the planetary embryos go through a stage of violent mergers, producing a few terrestrial planets. The last stage takes approximately 100 million to a billion years.The formation of giant planets is a more complicated process. It is thought to occur beyond the so-called frost line, where planetary embryos mainly are made of various types of ice. As a result, they are several times more massive than in the inner part of the protoplanetary disk. What follows after the embryo formation is not completely clear. Some embryos appear to continue to grow and eventually reach 5–10 Earth masses—the threshold value, which is necessary to begin accretion of the hydrogen–helium gas from the disk. The accumulation of gas by the core is initially a slow process, which continues for several million years, but after the forming protoplanet reaches about 30 Earth masses (M⊕) it accelerates and proceeds in a runaway manner. Jupiter- and Saturn-like planets are thought to accumulate the bulk of their mass during only 10,000 years. The accretion stops when the gas is exhausted. The formed planets can migrate over long distances during or after their formation. Ice giants such as Uranus and Neptune are thought to be failed cores, which formed too late when the disk had almost disappeared.
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