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Lecture 2. Thermal evolution and surface emission of neutron stars
Lecture 2. Thermal evolution and surface emission of neutron stars

TheFlowOfEnergyOutOf..
TheFlowOfEnergyOutOf..

... most effective. The result of these processes is that every time a photon interacts with matter, it is redirected so that it travels in a new and complete random direction. The resulting zigzag path is called a random walk. This is graphically demonstrated in the Flow simulation. Use the Flow simula ...
The Flow of Energy Out of the Sun
The Flow of Energy Out of the Sun

... most effective. The result of these processes is that every time a photon interacts with matter, it is redirected so that it travels in a new and complete random direction. The resulting zigzag path is called a random walk. This is graphically demonstrated in the Flow simulation. Use the Flow simula ...
Lecture01-ASTA01 - University of Toronto
Lecture01-ASTA01 - University of Toronto

... • Although these stars are roughly the same size as the Sun, they are so far away that you cannot see them as anything but points of light. • Even with the largest single telescopes on Earth, you still see only points of light when you look at stars, and any planets that might circle those stars are ...
Thermohaline mixing and the photospheric composition of low
Thermohaline mixing and the photospheric composition of low

1 Dynamos in Planets
1 Dynamos in Planets

... The giant planets Jupiter and Saturn both have strong fields; Saturn’s field is unusual for its high degree of axisymmetry; in table 1.1 we note that the inclination of Saturn’s dipole field is less than one degree from its rotation axis. A possible theoretical explanation has been given by Stevenso ...
First axion bounds from a pulsating helium
First axion bounds from a pulsating helium

... white dwarfs (WDs), which are among the most studied classes of stars. These stars represent the final stage of the evolution of low and intermediate mass stars (see [10] and references therein). Our knowledge of the physical processes governing the evolution of WDs relies on solid grounds, since th ...
The Indian Calendar
The Indian Calendar

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Document

1. INTRODUCTION 2. THE MODEL
1. INTRODUCTION 2. THE MODEL

Astronomy Astrophysics
Astronomy Astrophysics

... (1996) find a decreasing gradient outwards, while we find first an increase followed by a decrease in the halo. In addition to the different region samplings and spectral domains, the way the background is taken into account may have produced differences. Since binarism is important in M 67 (Montgom ...
3. Solar System Formation and Early Evolution
3. Solar System Formation and Early Evolution

... (i) The Sun was born in a ‘‘rich’’, Orion-like environment. (see Hillenbrand 1997; Figure 3.3) The most massive stars (the Trapezium-like stars) are very hot, and thus emit UV photons able to strongly ionize their immediate environment. The disks of the less massive stars then tend also to be ionize ...
Galactic chemical evolution of heavy elements: from Barium to
Galactic chemical evolution of heavy elements: from Barium to

... low-mass stars, mainly in the mass range ∼ 1–4 M⊙ (see e.g. Gallino, Busso, & Lugaro 1997; Busso, Gallino, & Wasserburg 1999, hereafter BGW). A different site for the production of s-process nuclei is required to account for the weak component, i.e. for s-nuclei below the Sr-peak. This site was iden ...
Observations with Herschel: High-mass star formation and the
Observations with Herschel: High-mass star formation and the

... antennas. The thesis therefore continues with an overview of the general principles governing the energy-level structure of molecules, absorption and emission of radiation by molecules, and how this radiation can be detected. The main focus of this thesis - star formation - is then presented in chap ...
Solar Probe: Mission to the Sun
Solar Probe: Mission to the Sun

... Determine the acceleration processes and find the source regions of the fast and slow solar wind at maximum and minimum solar activity; Locate the source and trace the flow of energy that heats the corona; Construct the three-dimensional coronal density configuration from pole to pole and determine ...
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Jeremy Heyl et al. (PDF document)

Mass transport in the heliosphere by energetic neutral atoms
Mass transport in the heliosphere by energetic neutral atoms

Homologous Stars: Simple Scaling Relations
Homologous Stars: Simple Scaling Relations

Magnetar-driven Hypernovae
Magnetar-driven Hypernovae

... Required magnetic flux , Y=1027-28 Gcm-2, close to the highest value observed in magnetic stars. • Accretion rate through the polar region can strongly decline several seconds after the collapse (Woosley & MacFadyen 1999), reducing the magnetic flux required for explosion (for solid rotation factor ...
Understanding LMXBs in Elliptical Galaxies
Understanding LMXBs in Elliptical Galaxies

Scorpio - Interactive Stars
Scorpio - Interactive Stars

The 13C(α,n)16O reaction rate. Recent estimates, new
The 13C(α,n)16O reaction rate. Recent estimates, new

... track), until it stops on the Main Sequence (hereafter MS) that corresponds to reaching central temperatures and densities (T = 107 K, ρ = 100 g/cm3 ) sufficient to start hydrogen fusion. Core hydrogen burning starts on the socalled zero age main sequence (ZAMS) and the star remains near this zone f ...
Powerpoint
Powerpoint

... The acoustic detection of UHE neutrinos is a promising technique that would complement high energy neutrino detection using the optical and radio techniques It is likely that any development of a large volume acoustic sensor array would “piggy back” the infrastructure of first and second generation ...
Hands-On Radio Astronomy Mapping the Milky Way
Hands-On Radio Astronomy Mapping the Milky Way

... • If cos l < 0 (in Quadrant II or III), one can show that there is one and only one positive solution, r+ , because R is always larger than R0 . • In the other quadrants, there can be two positive solutions. Negative values of r should be discarded because they have no physical meaning. If one obtai ...
Document
Document

... (Gammie 1996) ...
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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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