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Sample Exam for Final (with correct answers)
Sample Exam for Final (with correct answers)

Astrophysics in a Nutshell, Second Edition
Astrophysics in a Nutshell, Second Edition

... the horizontal branch, and then evolves more slowly to the right along this branch, as seen in Fig. 4.1. Stars with higher initial metal abundance, comparable to that of the Sun, instead of undergoing a horizontal-branch phase, move on the H-R diagram directly to a region on the red (right-hand) end ...
CONSTELLATION TUCANA, THE TOUCAN
CONSTELLATION TUCANA, THE TOUCAN

Chapter 3b powerpoint presentation
Chapter 3b powerpoint presentation

... I can now tell you is equivalent to mo = -2.5 log (the flux of the zero magnitude star Vega). So, for a star of magnitude m* we can write m* - mo = 2.5 log {fo/f*} Note: There is no constant ! In this equation mo = 0 of course because it is the magnitude of a zero magnitude star. However, the flux o ...
HST Paα Survey of the Galactic Center – Seeking the Missing
HST Paα Survey of the Galactic Center – Seeking the Missing

... Fig. 6 compares the magnitude distribution in 1.9µm with a stellar population synthesis model. This comparison shows that the overall shape of the distribution can be reasonably modelled with a constant star formation rate, plus a major burst about 350 Myr ago. The large deviation of the distributio ...
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... contained) in the distant past was very high; ● the temperature falls as the universe expands and so does the temperature of the radiation in the universe; ...
HR DIAGRAM (Page 1) - McDonald Observatory
HR DIAGRAM (Page 1) - McDonald Observatory

... Looking up into the night sky, you see thousands of stars at varying distances from Earth. The luminosity and temperature of each star varies as well. These are the reasons behind the wide range of apparent magnitudes of stars. Imagine being able to magically pull or push each star (including the su ...
A model of low-mass neutron stars with a quark core
A model of low-mass neutron stars with a quark core

... To study the functional dependence of the structural and integrated parameters of stellar configurations on the form of the equation of state for superdense matter, we have considered a large set of realistic equations of state that provide the coexistence of neutron matter with strange quark matter. ...
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... Write a letter P on the diagram to show the part showing the P wave arriving and a letter S to show the S wave. Both correct for 1 mark (1 mark) ...
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... Atmospheric extinction (e.g. Rayleigh scattering) will affect the A star more than the K star because it has more flux at shorter wavelength where the extinction is greater ...
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Solution Sheet Lab 1

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... contained) in the distant past was very high; ● the temperature falls as the universe expands and so does the temperature of the radiation in the universe; ...
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color magnitude diagrams - AST 114, Astronomy Lab II for Spring
color magnitude diagrams - AST 114, Astronomy Lab II for Spring

The star Epsilon UMa, or more commonly known as Alioth
The star Epsilon UMa, or more commonly known as Alioth

... and the approximate surface temperature ranges from 7,500 to 11,000 degrees Kelvin. The average luminosity of these stars is around 80 solar luminosity (1 solar luminosity equaling 3.83 x 1033 ergs/s), the average mass is approximately 3.2 solar masses (1 solar mass equaling 1.989 x 1030 kg) and the ...
Nuclear Exotica (online version) - ECM-UB
Nuclear Exotica (online version) - ECM-UB

The Main Sequence - University of Arizona
The Main Sequence - University of Arizona

... CNO vs. PP Chain • Equate CNO and PP energy production to find where each dominates • T ~ 1.7x107(XH/50XCN)1/12.1 • Crossover point occurs at ~ 1.1 M for Pop I • At z=0 must reach He burning T and produce CNO catalysts • (PP)~X2H0(T/T0)4.6 ; (CNO) ~XHXCNOfN0(T/T0)16.7 • PP and CNO have to pr ...
Parallax and Distance
Parallax and Distance

1705 Star Charts
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... Saucepan, now lying on its side. In early June Orion can be seen both in the west at dusk and in the east at dawn. The Orion Nebula is visible in binoculars as a misty glow around the middle star of Orion's Sword or the handle of The Pot. It is a vast cloud of dust and gas about 1300 l.y. away and m ...
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A0620-00 poster

... We used our “LinBrod” program to analyze the spectrum of SS Cyg (Bitner & Robinson 2006). This program calculates the spectrum of a star that fills its Roche lobe in a close binary star by summing wavelength-dependent specific intensities over the visible surface of the star. The surface of the star ...
Detecting Habitable Planets around Nearby Sun-Like Stars
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... angle of sky in the direction of Cygnus/Lyra. – Stars at average distance of ~1 kpc. • Difficult to follow up by direct detection. ...
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... 4. Sub-photospheric – violent mode or strange mode instabilities Glatzel et al, Guzik, Stothers & Chin Caused by increase in opacity due to Fe at base of photosphere leading to ionization induced instability ...
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Astronomy 252: Short Project 2 Stellar Spectra: Their Classification
Astronomy 252: Short Project 2 Stellar Spectra: Their Classification

... stars. The beautiful thing about spectral classification is that one does not really need to know anything about stellar astrophysics to classify a spectrum. Think of spectral classification as simply an exercise in pattern matching. What you want to do is to "bracket" the unknown spectrum between t ...
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s-process

... When does the s-process start? Main s-process occurs during thermal pulses in AGB stars of 2-4 solar masses H mixes inward, giving 12C(p,e+)13C ...
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Stellar evolution



Stellar evolution is the process by which a star changes during its lifetime. Depending on the mass of the star, this lifetime ranges from a few million years for the most massive to trillions of years for the least massive, which is considerably longer than the age of the universe. The table shows the lifetimes of stars as a function of their masses. All stars are born from collapsing clouds of gas and dust, often called nebulae or molecular clouds. Over the course of millions of years, these protostars settle down into a state of equilibrium, becoming what is known as a main-sequence star.Nuclear fusion powers a star for most of its life. Initially the energy is generated by the fusion of hydrogen atoms at the core of the main-sequence star. Later, as the preponderance of atoms at the core becomes helium, stars like the Sun begin to fuse hydrogen along a spherical shell surrounding the core. This process causes the star to gradually grow in size, passing through the subgiant stage until it reaches the red giant phase. Stars with at least half the mass of the Sun can also begin to generate energy through the fusion of helium at their core, whereas more-massive stars can fuse heavier elements along a series of concentric shells. Once a star like the Sun has exhausted its nuclear fuel, its core collapses into a dense white dwarf and the outer layers are expelled as a planetary nebula. Stars with around ten or more times the mass of the Sun can explode in a supernova as their inert iron cores collapse into an extremely dense neutron star or black hole. Although the universe is not old enough for any of the smallest red dwarfs to have reached the end of their lives, stellar models suggest they will slowly become brighter and hotter before running out of hydrogen fuel and becoming low-mass white dwarfs.Stellar evolution is not studied by observing the life of a single star, as most stellar changes occur too slowly to be detected, even over many centuries. Instead, astrophysicists come to understand how stars evolve by observing numerous stars at various points in their lifetime, and by simulating stellar structure using computer models.In June 2015, astronomers reported evidence for Population III stars in the Cosmos Redshift 7 galaxy at z = 6.60. Such stars are likely to have existed in the very early universe (i.e., at high redshift), and may have started the production of chemical elements heavier than hydrogen that are needed for the later formation of planets and life as we know it.
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