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Star Formation in Disks: Spiral Arms, Turbulence, and Triggering
Star Formation in Disks: Spiral Arms, Turbulence, and Triggering

... There are many types and sources of energy in the ISM and many possible causes for triggering. Energy types include thermal, magnetic, turbulent, cosmic ray, and rotational. The first four are all comparable and equal to several tenths of an eV cm−3 . Rotational energy is much denser, several hundred ...
STIS/HST Observations of Large Magellanic Cloud Planetary
STIS/HST Observations of Large Magellanic Cloud Planetary

... This study of LMC PNs, which is still underway, has given us significant insight into the formation and evolution of the nebulae and their central stars. For the first time we can study a relatively unbiased sample of PNs to examine the formation and evolution of the nebulae. Specifically, there is ...
The chemical composition of IK Pegasi
The chemical composition of IK Pegasi

REVIEWS The formation of the first stars and galaxies Volker Bromm
REVIEWS The formation of the first stars and galaxies Volker Bromm

... statistically described as a Gaussian random field. Such high-density peaks are expected to be strongly clustered15, and thus feedback effects from the first stars are important in determining the fate of the surrounding primordial gas clouds. It is very likely that only one star can be formed withi ...
Galactic astroarchaeology: reconstructing the bulge history by
Galactic astroarchaeology: reconstructing the bulge history by

Astrospheres and Solar-like Stellar Winds | SpringerLink
Astrospheres and Solar-like Stellar Winds | SpringerLink

The Mid-Infrared Spectrum of the Short Orbital Period Polar EF
The Mid-Infrared Spectrum of the Short Orbital Period Polar EF

... peak amplitudes, the cyclotron humps are too narrow compared to the observed nearIR spectrum. The fact that discrete cyclotron humps are observed requires kT . 20 keV. θ: In the absence of consistent information constraining this parameter, we chose to set θ = 75◦ for all models. In any case, θ cann ...
Insights into thermonuclear supernovae from the incomplete Si
Insights into thermonuclear supernovae from the incomplete Si

Tidal interaction of a rotating 1 vec {M_sun} star with a - UvA-DARE
Tidal interaction of a rotating 1 vec {M_sun} star with a - UvA-DARE

Radiative feedback from protoplanets in self
Radiative feedback from protoplanets in self

Dust in protoplanetary disks
Dust in protoplanetary disks

... laboratory experiments that the dust agglomeration is an efficient process in dense and relativ environments, like protostellar cores or protoplanetary discs (e.g., Blum et al., 2002; Kemp 1999; Kesselman, 1980; Nuth and Berg, 1994; Ossenkopf and Henning, 1994; Wurm an ...
ASTRONOMY AND ASTROPHYSICS How many low
ASTRONOMY AND ASTROPHYSICS How many low

... Let us focus on the stars of the present sample that have passed the bump and do not behave as the majority. If we consider the objects with MV lower than -0.5, only 3 stars appear to be really “deviant” (see Table 2). V8 (NGC6656). As can be seen in Figs. 1 and 2, as soon as they are more luminous ...
Clusters: age scales for stellar physics
Clusters: age scales for stellar physics

... The second firmly established anchor is the age of the Solar System. The Sun is about 4.57 Gyr old. This value comes from two different methodologies based on estimates for the Sun as a star and for the the remnants of the formation of the Solar System: • Computer models of stellar evolution and ast ...
THE FORMATION OF URANUS AND NEPTUNE IN SOLID
THE FORMATION OF URANUS AND NEPTUNE IN SOLID

Stellar Population Effects on the Inferred Photon Density at
Stellar Population Effects on the Inferred Photon Density at

... 2015). This ‘Lyman continuum’ flux is estimated through the use of stellar population synthesis models, fitted to the available data. For a stellar population of known age, metallicity and ultraviolet flux, the ionizing photon flux can be reliably estimated. However difficulties arise when any of these pr ...
Solar System Constraints on the Dvali-Gabadadze
Solar System Constraints on the Dvali-Gabadadze

Max Planck Institute for Gravitational Physics
Max Planck Institute for Gravitational Physics

... star/body of distant stars/bodies is important: often more important than influence of close stars/bodies Let us consider a IDEALIZED galaxy of N identical stars with mass m, size R and uniform density Let us focus on a single star that crosses the system How long does it take for this star to chang ...
The first gravitational-wave source from the isolated evolution of two
The first gravitational-wave source from the isolated evolution of two

... ity and the intrinsic detectable mass distribution strongly favors sources with total redshifted masses between 25–73 M⊙ , consistent with our recent work (4), and matching the total redshifted mass of GW150914 (Mtot,z = 70.5 M⊙ ). In our simulations the maximum intrinsic mass of a merging BH-BH bi ...
The mass, temperature and distance of the white dwarf in V 471 Tauri
The mass, temperature and distance of the white dwarf in V 471 Tauri

Potential for Life on the Terrestrial Planets
Potential for Life on the Terrestrial Planets

... atmospheres with CO2/N2 mixing ratios lower then 96% and exposed to intense XUV fluxes result in higher exospheric temperatures and more expanded thermosphereexosphere environments and, hence, suffer stronger atmospheric erosion, which may result in the total loss of several hundred bars even if an ...
SOLAR HARD X-RAY AND GAMMA-RAY OBSERVATIONS FROM
SOLAR HARD X-RAY AND GAMMA-RAY OBSERVATIONS FROM

... data was performed at a lower energy (30 keV) where the contribution of the hot thermal plasma is larger. The observations of the 1990 February 11 event with the Konus-B instrument on GRANAT support this explanation, since the time profiles recorded in three energy bands between 10 and 750 keV becom ...
Astronomy 112: The Physics of Stars Class 1 Notes
Astronomy 112: The Physics of Stars Class 1 Notes

... We can actually learn a tremendously larger amount by measuring the spectrum of stars. That’s because a real stellar spectrum isn’t just a simple continuous function like a blackbody. Instead, there are all sorts of spiky features. These were first studied by the German physicist Fraunhofer in 1814 ...
The Space Density of Spiral Galaxies as f(magnitude, size and
The Space Density of Spiral Galaxies as f(magnitude, size and

Parity violating measurements of neutron densities
Parity violating measurements of neutron densities

Document
Document

... Of the many possibilities for combining quarks with colour into colourless hadrons, only two configurations were found, till now… ...
< 1 ... 22 23 24 25 26 27 28 29 30 ... 237 >

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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