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Celebrating Astronomy: The Life of a Star
Celebrating Astronomy: The Life of a Star

Abstracts - Physics of Evolved Stars 2015
Abstracts - Physics of Evolved Stars 2015

... intermediate main-sequence mass (5-8 solar masses) stars before they evolve into the post-AGB and planetary-nebula stages. AGB stars lose most of their stellar envelope in the form of a gaseous and dusty stellar wind. This wind eventually grows to such high mass-loss rates that the central star beco ...
NSDL/NSTA Web Seminar: Celebrating Astronomy: A Star`s Story
NSDL/NSTA Web Seminar: Celebrating Astronomy: A Star`s Story

... evolves and eventually dies is its initial mass. ...
neutron star
neutron star

Evolution of eccentricity and inclination of migrating planets in the 2
Evolution of eccentricity and inclination of migrating planets in the 2

... 420 by the Kepler mission. A significant fraction of these systems contain planet pairs in or near a 2:1 mean motion resonance. Capture in mean motion resonance is thought to be the result of convergent migration of planets. The evolution of planetary systems in mean motion resonance has been studie ...
Multiplicity in Early Stellar Evolution
Multiplicity in Early Stellar Evolution

Formation of Molecular Clouds and Global Conditions for Star
Formation of Molecular Clouds and Global Conditions for Star

... 2009; Juneau et al. 2009; Garcı́a-Burillo et al. 2012) also show power-law correlations but with smaller indices; the index appears to depend mostly on the line critical density, a result that can be explained through models (Krumholz and Thompson 2007; Narayanan et al. 2008b,a). Within galaxies the ...
ULXs: General Properties and Variability - X
ULXs: General Properties and Variability - X

... luminous photo-ionized nebulae around them- require high luminosity to photoionize them •Quite a few have “soft” components well fit by low kT black body- consistent with high mass (Miller this meeting). ...
CHEOPS Science Requirements Document
CHEOPS Science Requirements Document

... confirmed. We have learned that planets are quite common, and that their properties are much more diverse than originally predicted (Udry et al. 2007). We have even witnessed the first few direct detections and analysis of their atmospheres in recent years. These pioneering measurements, previously ...
1 Pau Amaro Seoane - modest 15-s
1 Pau Amaro Seoane - modest 15-s

... Several star clusters show a roughly flat velocity dispersion profile at large radii, which is not predicted from self-consistent models with a tidal truncation (such as ‘King models’). This non-zero temperature of stars has previously been attributed to deviations from Newtonian gravity in the weak ...
Galactic Nebulae
Galactic Nebulae

Protoplanetary Discs
Protoplanetary Discs

... Irradiation of central star light Angular momentum transport Spectral energy distributions A brief introduction to SEDs Disc classification scheme Disc models The optically thick accretion disc Measuring disc masses Disc evolution & depletion mechanims Andrea Stolte ...
Regular Keplerian motions in classical many-body
Regular Keplerian motions in classical many-body

... In most textbooks on mechanics the two-body system generally is not referred to as a manybody system because the problem of relative motion of two interacting bodies (irrespective of the physical nature of the interaction) mathematically is equivalent to the problem of motion of a virtual single bod ...
Document
Document

The formation and destruction of molecular clouds and galactic star
The formation and destruction of molecular clouds and galactic star

... We first model the growth of molecular clouds. Inoue & Inutsuka (2012) showed that we need multiple episodes of compression of HI clouds to create molecular clouds. According to the standard picture of supernova-regulated ISM dynamics (e.g., McKee & Ostriker 1977), the typical timescale between cons ...
Document
Document

...  If a massive additional body with a shorter perturbation timescale exists, Kozai migration due to the binary cannot occur (Innanen et al. 1997, Wu and Murray 2003)  conditional equation:  (smaller bodies are allowed) ...
Stellar radii from long-baseline interferometry
Stellar radii from long-baseline interferometry

... JMMC, Jean-Marie Mariotti Center web site, http://www.mariotti.fr/ Kervella, P., Coudé du Foresto, V., Glindemann, A. & Hofmann, R. 2000, SPIE, 4006, 31 Kervella, P., Gitton, Ph., Ségransan, D., et al. 2003a, SPIE, 4838, 858 Kervella, P., Thévenin, F., & Ségransan, D., et al. 2003b, A&A, 404, 10 ...
silicon and oxygen abundances in planet-host stars
silicon and oxygen abundances in planet-host stars

Downloaded - Royal Society Open Science
Downloaded - Royal Society Open Science

Angular momentum transport in accretion discs
Angular momentum transport in accretion discs

... object and falling onto its surface gives up angular momentum to outer parts of the disc. During this process disc spreads, because small amount of matter should eventually carry all the angular moment outwards, while the rest of the mass losing angular momentum falls onto the star (Lynden-Bell & Pr ...
Is there life in space? Activity 1: The Vastness of Space
Is there life in space? Activity 1: The Vastness of Space

Observational Data
Observational Data

Physical Properties of the Gas and Dust in the Orion B Molecular
Physical Properties of the Gas and Dust in the Orion B Molecular

... form and their mass spectrum (LBS; Tatematsu et al. 1993) differs significantly from that of the stellar initial mass function (IMF) (see discussion in Zinnecker 1990). What else are then the actual birthplaces of stars in a molecular cloud and how can one find them? Progress in this field has been ...
Simulations of the galaxy population constrained by observations
Simulations of the galaxy population constrained by observations

... in this model. The data require the efficiency with which galactic wind ejecta are reaccreted to vary with redshift and halo mass quite differently than previously assumed, but in a similar way as in some recent hydrodynamic simulations of galaxy formation. We propose a specific model in which reinc ...
Complete Lecture Notes (pdf file)
Complete Lecture Notes (pdf file)

... • Binary systems • Star clusters....these reveal how stars evolve with time • Nuclear physics...energy source, synthesis of heavy elements No direct information about physical conditions in stellar interiors (except from helioseismology and solar neutrinos) No direct evidence for stellar evolution.. ...
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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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