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Structure of the hot object in the symbiotic prototype Z And during its
Structure of the hot object in the symbiotic prototype Z And during its

... UV continuum with an additional attenuation below 1300 Å accompanied by a decline in the radio flux during the 1985 optical maximum. In the line spectrum they measured a broadening of all emission lines with signatures of P-Cygni type profiles for strong resonance lines. Fernández-Castro et al. (19 ...
full text pdf
full text pdf

... cooler white dwarf sample of Bergeron, Saffer & Liebert (1992), then the hydrogen layer mass must be considerably less than 1 0 - 4 M * . In this context, Mh < 1 0 - 6 M * suffices, and this is not surprising, given that the two major channels of spectral evolution will have DA stars through the 30 ...
4. Stars and resolved stellar populations
4. Stars and resolved stellar populations

astrolabe
astrolabe

STELLAR MASSES AND STAR FORMATION RATES OF LENSED DUSTY STAR-FORMING... FROM THE SPT SURVEY
STELLAR MASSES AND STAR FORMATION RATES OF LENSED DUSTY STAR-FORMING... FROM THE SPT SURVEY

... a population of high-redshift dusty star-forming galaxies (DSFGs) has been established, expanding our understanding of galaxy formation and evolution. These massive galaxies (M∗ ∼ 1011 M⊙ ; Hainline et al. 2011; Michalowski et al. 2012; Simpson et al. 2014) are extremely bright at submillimeter wave ...
A model of slingshot prominences in rapidly rotating stars
A model of slingshot prominences in rapidly rotating stars

... slingshot prominences have been observed is AB Dor. Collier Cameron et al. (1990) derived a mass of 2±6  1017 g; a projected area of 1022 cm2 and a lifetime of a few days for clouds on this star. Stellar slingshot prominences are not peculiar to particular stars but rather a very common property in ...
- UCL Discovery
- UCL Discovery

... Pelupessy, van der Werf & Icke 2004). The thermal energy of the feedback particles is calculated with the SPH scheme with radiative cooling and additional heating from stellar wind, SNe II and SNe Ia. Eight out of the 19 feedback particles spend no time being stars and immediately become SNe II feed ...
ONE- AND MULTI- ZONE MODELS: Chemical properties
ONE- AND MULTI- ZONE MODELS: Chemical properties

Matter and antimatter in the same universe?
Matter and antimatter in the same universe?

Modelling the Ultra-Faint Dwarf Galaxies and Tidal
Modelling the Ultra-Faint Dwarf Galaxies and Tidal

... Boo II) have been found to date, in SDSS data covering ~20% of the sky  tens more likely remain undiscovered • Properties: Ultra-low luminosities (-3.8 ≥ MV ≥ -7.9) and ...
What We Might Learn from Gravitational Waves
What We Might Learn from Gravitational Waves

... Most promising GW+EM source: Short/hard Gamma-ray burst GRBs definitely exist ~1/day in the Universe GRBs are very bright/relativistic GRBs can be detected “all sky” throughout the Universe GRBs have been observed “nearby” Some long, and some short (2 second divide) ...
Semiar PPT
Semiar PPT

... 3. The rapid fall off of the early x-ray afterglow suggests that -ray emission is produced by a short lived source; we find that it is most likely SSC at a distance of ~ 1016 cm  baryonic jets have a few problems. 4. X-ray lightcurves show flares on time scale of minutes to a day suggesting that t ...
Review: A Coherent and Comprehensive Model of the Evolution of
Review: A Coherent and Comprehensive Model of the Evolution of

review: a coherent and comprehensive model of the evolution
review: a coherent and comprehensive model of the evolution

The Alpha Centauri binary system
The Alpha Centauri binary system

The role of neutron star mergers in the chemical evolution of the
The role of neutron star mergers in the chemical evolution of the

6th Grade The Theoretical Beginning of the Universe / Big Bang
6th Grade The Theoretical Beginning of the Universe / Big Bang

... (Some astronomers give a rough estimate that there are 1022 stars, although this is always changing!) ...
Modeling non-thermal emission from stellar bow shocks
Modeling non-thermal emission from stellar bow shocks

Astrophysical Journal - Harvard-Smithsonian Center for Astrophysics
Astrophysical Journal - Harvard-Smithsonian Center for Astrophysics

Effects of neutron-star superconductivity on
Effects of neutron-star superconductivity on

Interstellar neutral oxygen in a two-shock
Interstellar neutral oxygen in a two-shock

Demonstration of multilayer reflective optics at photon energies
Demonstration of multilayer reflective optics at photon energies

... < 3 μ rad RMS figure over the entire 150x150 mm2 substrate surface area and 3.3 Å RMS midand 0.5 Å RMS high spatial frequency roughness. Specular reflectivity data were acquired off of the mirror at beamline ID15A at the European Synchrotron Radiation Facility (ESRF) in a θ − 2θ geometry with a ve ...
EUV and X-ray Spectroscopy of the Active Sun
EUV and X-ray Spectroscopy of the Active Sun

... flare was carried out using RHESSI, CDS, GOES and TRACE. Evidence for pre-flare heating, explosive and gentle chromospheric evaporation and loop draining were observed in the data. The observations were compared to a 0-D hydrodynamic model, EBTEL, to aid interpretation. This led to the conclusion th ...
Sources of Stellar Energy and the Theory of the Internal Constitution
Sources of Stellar Energy and the Theory of the Internal Constitution

... any stars, including even super-giants, the radiant pressure plays no essential part — it is negligible in comparison to the gaseous pressure; (2) inner regions of stars are filled mainly by hydrogen (the average molecular weight is close to 1/2); (3) absorption of light is derived from Thomson disp ...
When Extrasolar Planets Transit Their Parent Stars
When Extrasolar Planets Transit Their Parent Stars

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Standard solar model

The standard solar model (SSM) is a mathematical treatment of the Sun as a spherical ball of gas (in varying states of ionisation, with the hydrogen in the deep interior being a completely ionised plasma). This model, technically the spherically symmetric quasi-static model of a star, has stellar structure described by several differential equations derived from basic physical principles. The model is constrained by boundary conditions, namely the luminosity, radius, age and composition of the Sun, which are well determined. The age of the Sun cannot be measured directly; one way to estimate it is from the age of the oldest meteorites, and models of the evolution of the Solar System. The composition in the photosphere of the modern-day Sun, by mass, is 74.9% hydrogen and 23.8% helium. All heavier elements, called metals in astronomy, account for less than 2 percent of the mass. The SSM is used to test the validity of stellar evolution theory. In fact, the only way to determine the two free parameters of the stellar evolution model, the helium abundance and the mixing length parameter (used to model convection in the Sun), are to adjust the SSM to ""fit"" the observed Sun.
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