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D2.2 - aspera
D2.2 - aspera

Studying explosive phenomena in astrophysics by the example of
Studying explosive phenomena in astrophysics by the example of

... stars (Population III stars) formed, but according to modern theory of stellar evolution these stars should be very massive (about 100 M⊙ ). Population III stars also have a potential to produce probably most energetic flashes in the Universe – gamma-ray bursts (GRBs). GRBs may provide one of the mo ...
The half-light radius distribution of LBGs and their
The half-light radius distribution of LBGs and their

Contents
Contents

Document
Document

... The density profile was taken to be the same as in the jet for simplicity, but with different value at r0. ...
ICP-MS and Planetary Geosciences
ICP-MS and Planetary Geosciences

... region of interstellar space where the Sun formed. For example, the variability of the amount of 60 Fe and 26 Al (both are short-lived, now extinct, isotopes) might conceivably mean that 60 Fe was added to our Solar System a million years after it formed, but when the solar nebula was still present. ...
ASTRONOMY AND ASTROPHYSICS Properties of solar pores
ASTRONOMY AND ASTROPHYSICS Properties of solar pores

Surface temperature distribution and absorption features in Isolated
Surface temperature distribution and absorption features in Isolated

Problem Set 2 for Astro 322 Read chapter 24.2. (Some of this
Problem Set 2 for Astro 322 Read chapter 24.2. (Some of this

... For the Milky Way, 1.5 × 1010 L = 2πh2R I(R = 0), and I(R) = I(R = 0) exp[−R/hR ]. We find I(R = 0) = LD /(2πh2R ) = 1.5 × 1010 L /(2π(4000pc)2 ) = 149 L pc−2 . Then I(R = 8kpc) = I(R = 0)exp(−8/4) = 20.2 L pc−2 . We note that this M/LV ratio is integrated over all z, through the thick disk as w ...
The physics of high-mass star formation
The physics of high-mass star formation

on limiting the thickness of the solar tachocline
on limiting the thickness of the solar tachocline

... hκ , γ is the adiabatic index, and all other variables take their usual meanings. In all of the above equations, reference state variables are denoted by an overbar. Equation (4) represents the energy equation written as a temperature equation, where ur represents the radial velocity. The first term ...
NATS 1311 From the Cosmos to Earth
NATS 1311 From the Cosmos to Earth

... relative sizes of a lowmass star as a mainsequence star, a red giant, and a heliumburning star. The scale is not precise; in particular, the size of the main-sequence star is even smaller compared to the ...
Saturn - Delapre Blog
Saturn - Delapre Blog

Oscillation Modes of Strange Quark Stars with a Strangelet Crust
Oscillation Modes of Strange Quark Stars with a Strangelet Crust

... Figure 1. Mass-Radius relation for homogeneous quark stars described by the EoS (Eq. 1). The interaction parameter a4 =0.7 and ms =100 MeV. Measured limits on the mass of PSR J1614-2230 (1.97±0.04 M ) and PSR J0348-0432 (2.01±0.04 M ) are shown. ...
transparencies
transparencies

... For GRBs of group xI and xII, we can estimate the redshift needed for being compliant with the B&G relation • Proof on the bursts defining the ...
Gaseous Planets, Protostars And Young Brown Dwarfs
Gaseous Planets, Protostars And Young Brown Dwarfs

Transient events in the EUV transition region and chromosphere
Transient events in the EUV transition region and chromosphere

... extreme ultraviolet emission, observed by the cds instrument on soho, are discussed. Numerous transient brightenings are observed in network features in both a transition region line (O v 629.73 Å) and a chromospheric line (He i 584.33 Å), indicating a dynamic coupling between the chromospheric an ...
Habitable Zone
Habitable Zone

On the trend of [Mg/Fe] among giant elliptical galaxies
On the trend of [Mg/Fe] among giant elliptical galaxies

... Davies et al. 1993), indicating that the Mg/Fe ratio should increase with galactic luminosity and mass. We transform the abundance of Fe, as predicted by classic wind models and alternative models for the chemical evolution of elliptical galaxies, into the metallicity indices M g2 and < F e >, by me ...
The fundamental parameters of the roAp star γ Equulei
The fundamental parameters of the roAp star γ Equulei

Basics about stars
Basics about stars

Cosmoclimatology: a new theory emerges
Cosmoclimatology: a new theory emerges

... of clouds on Antarctica, and meteorologists at far southern latitudes confirm it by observation. Greenland too has an ice sheet, but it is smaller and not so white. And while conditions in Greenland are coupled to the general climate of the northern hemisphere, Antarctica is largely isolated by vort ...
The spectral energy distribution of protoplanetary
The spectral energy distribution of protoplanetary

A Reservoir of Ionized Gas in the Galactic Halo to Sustain Star
A Reservoir of Ionized Gas in the Galactic Halo to Sustain Star

... of the iHVCs seen toward the AGNs and stars is moreover remarkably similar considering our better sampled north Galactic sky (Fig. 2). These and the fact that the H I HVCs and iHVCs are now known to be at similar distances strongly suggest they are all related, probing separate phases where the H I ...
Cosmic Microwave Background Anisotropies:
Cosmic Microwave Background Anisotropies:

... •Curvature or dark energy can be only important in very late time for evolution of the Universe Since late time=larger horizon size, ISW affects Cl on very small l’s Late ISW •However, when the universe became matter domination from radiation domination, potential decayed! This epoch is near recombi ...
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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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