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Dusty AGN Tori
Dusty AGN Tori

... density annular ring dust with inner radius a, outer radius b and height h (15). The dust extinction curve is that of Fig. 10. The central luminosity is assumed to be a power-law spectrum The four model parameters are: the inner aspect ratio a/h, the radial and vertical Thomson depths of the torus,τ ...
Planet formation around M-dwarfs: the moving snow line and super
Planet formation around M-dwarfs: the moving snow line and super

... 2–3 AU, and 1–2M⊕ planets at 3–4 AU. If we simply adapt the collisional history of Earth formation to a planetesimal disk around a 0.25M star, mergers of ∼10 oligarchs should yield planets with masses ∼1–2M⊕ at 1 AU and ∼3–5M⊕ at 2.5 AU. To consider whether oligarchs can merge into superEarths on r ...
Diapositiva 1 - INAF-Osservatorio Astronomico di Bologna
Diapositiva 1 - INAF-Osservatorio Astronomico di Bologna

... Bologna 22.01.2009 ...
FIVE NEW TRANSITS OF THE SUPER
FIVE NEW TRANSITS OF THE SUPER

... determine the best-fitting parameter values and confidence intervals. This algorithm delivers an estimate of the a posteriori joint probability distribution for all of the parameters (see Holman et al. 2006 or Winn et al. 2007 for more details). For each parameter we took the mode of the distributio ...
Document
Document

... observations of M dwarfs to determine flare rates • I am creating model galaxy simulations to predict flare rates on a Galactic scale that includes spectral type and activity level. We can ‘observe’ this model to predict what LSST will see. ...
The First Stars in the Universe - Scientific American
The First Stars in the Universe - Scientific American

... and Abraham Loeb of Harvard, one of us (Bromm) devised theoretical models of such stars with masses between 100 and 1,000 solar masses. The models showed that the stars had surface temperatures of about 100,000 kelvins—about 17 times higher than the sun’s surface temperature. Therefore, the first st ...
Lithium production by thermohaline mixing in low
Lithium production by thermohaline mixing in low

an aluminum/calcium-rich, iron-poor, white dwarf star
an aluminum/calcium-rich, iron-poor, white dwarf star

Spectral modeling of nebular-phase supernovae Anders Jerkstrand Department of Astronomy
Spectral modeling of nebular-phase supernovae Anders Jerkstrand Department of Astronomy

... where Z is the proton number, q is the charge unit, and kB is Boltzmann’s constant. For hydrogen (Z = 1), we obtain T ∼ 1010 K. At the beginning of ...
double shell–burning
double shell–burning

... Role of Mass • A star’s mass determines its entire life story because it determines its core temperature. • High-mass stars with > 8MSun have short lives, eventually becoming hot enough to make iron, and end in supernova explosions. • Low-mass stars with < 2MSun have long lives, ...
Solar flux variation of the electron temperature morning
Solar flux variation of the electron temperature morning

... plasma drift velocities further decrease the local ion density, which increases Te. As the ion density builds up after sunrise, Te decreases to daytime values that are reached at about 09 LT. The neutral density and the electron‐neutral cooling rate also build up after sunrise but it has a smaller e ...
Propagation of cosmic rays in the solar wind
Propagation of cosmic rays in the solar wind

Overview spherical accretion
Overview spherical accretion

Hajime Togashi - International Workshop on Neutrino Physics and
Hajime Togashi - International Workshop on Neutrino Physics and

Modified r-matrix analysis of the 19F(p,a)16O HOES reaction
Modified r-matrix analysis of the 19F(p,a)16O HOES reaction

... is a key isotope in astrophysics as it can be used to probe AGB star mixing phenomena and nucleosynthesis. But its production is still uncertain! In AGB stars, the largest observed fluorine overabundances cannot be explained with standard AGB models. A possible lack of proper accounting for the cont ...
Highligh in Physics 2005
Highligh in Physics 2005

... FU Orionis objects are a small class of young stellar objects undergoing periods of enhanced disk accretion activity (outbursts). While T Tauri stars usually have rather low accretion rates (of the order of 10-8 M/yr), during the outburst the accretion rate can reach a few times 10-4 M/yr. Even if ...
Pre-main sequence evolution
Pre-main sequence evolution

... What are T Tauri & Herbig Ae/Be stars? • T Tauri stars are low-mass stars with discs • Herbig Ae/Be stars are intermediate-mass stars with discs • in the Hertzsprung-Russel-Diagram (HRD), both are located above the main sequence, in the region of pre-main sequence evolution Pre-main sequence: • mai ...
The solution of the radiative transfer equation in axial symmetry
The solution of the radiative transfer equation in axial symmetry

... thick regions it’s possible to calculate using a method which uses the diffusion approximation [10]. Both of these methods are inappropriate for stellar atmospheres. The classical way for calculating a solution to this equation in more dimensions is the long characteristic method [2]. This method fu ...
Lecture 2. Thermal evolution and surface emission of
Lecture 2. Thermal evolution and surface emission of

... The total thermal energy of a nonsuperfluid neutron star is estimated as UT ~ 1048 T29 erg. The heat capacity of an npe neutron star core with strongly superfluid neutrons and protons is determined by the electrons, which are not superfluid, and it is ~20 times lower than for a neutron star with a n ...
On the possibility of a helium white dwarf donor in the presumed
On the possibility of a helium white dwarf donor in the presumed

Surface temperatures at the nearside of the Moon as a
Surface temperatures at the nearside of the Moon as a

... variability and the change in the global mean surface temperature. However, model simulations show that the observed change in total solar irradiance has a much smaller impact on the observed temperature change than does the anthropogenic greenhouse effect (Bender et al., 2006; Hansen et al., 2002; L ...
point-like
point-like

... Goal: a deeper understanding of a particular issue/problem analyzed in class, or a totally new AGN-related topic we did not have time to talk about Either a literature search or original data analysis (using data from public archives) Submit an outline for pre-approval by November 1 Your paper (< 20 ...
STELLAR SPECTRA A. Basic Line Formation
STELLAR SPECTRA A. Basic Line Formation

... division on the basis of spectral line appearances; – Hertzsprung (1908) and Russell (1913) independently plot a diagram of stellar absolute magnitude against spectral type (Figure 1). It shows that stars occupy sharply defined locations in this parameter space; – Cecilia Payne (1925): demonstration ...
FINAL STAGES OF MASSIVE STARS. SN EXPLOSION AND
FINAL STAGES OF MASSIVE STARS. SN EXPLOSION AND

Multiple sources or late injection of short-lived r
Multiple sources or late injection of short-lived r

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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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