
Lec8_2D
... How the Sun Does Not Shine • As the energy leaks out, the central temperature of the Sun drops • Lower temperature means lower gas pressure • The lower gas pressure cannot hold up against gravity – the Sun shrinks • The added compression puts the Sun’s center under greater pressure, so the central ...
... How the Sun Does Not Shine • As the energy leaks out, the central temperature of the Sun drops • Lower temperature means lower gas pressure • The lower gas pressure cannot hold up against gravity – the Sun shrinks • The added compression puts the Sun’s center under greater pressure, so the central ...
The most energetic light ever observed from a few
... new observations extend this tail to much higher, above TeV energies, that is, several times more energetic than the previous measurement, violating all the theory models believed to be at work in neutron stars.” The photons arrive in two precise beams which should be created far from the neutron st ...
... new observations extend this tail to much higher, above TeV energies, that is, several times more energetic than the previous measurement, violating all the theory models believed to be at work in neutron stars.” The photons arrive in two precise beams which should be created far from the neutron st ...
–1– Lectures 18 and 19 Optical Depth vs. Density Imaging a sphere
... isothermal. Since Jeans fragmentation requires an isothermal gas, this will also halt the fragmentation of the collapsing gas into progressively smaller pieces. Low and Lynden-Bell (1976) calculated that this occurs at a few hundredths of a stellar mass. This suggests the initial pieces are much sma ...
... isothermal. Since Jeans fragmentation requires an isothermal gas, this will also halt the fragmentation of the collapsing gas into progressively smaller pieces. Low and Lynden-Bell (1976) calculated that this occurs at a few hundredths of a stellar mass. This suggests the initial pieces are much sma ...
Eruptive Variables - Scientific Research Publishing
... In this paper, a solution of the problem about how a massive star knows that it gets rid of its excess of mass before it can become a white dwarf, a pulsar or a black hole, is proposed. Many astronomers believe that this may take place in the form of a nova and supernova outburst, as well as in the ...
... In this paper, a solution of the problem about how a massive star knows that it gets rid of its excess of mass before it can become a white dwarf, a pulsar or a black hole, is proposed. Many astronomers believe that this may take place in the form of a nova and supernova outburst, as well as in the ...
Futuro da Ci^encia no IAG
... observed but should be detected in 2 ways: -High mass stars explode as supernovae and produce a GRBs (z ~ 15 ?) GRB at z~8.2 = pop. III? -First generations of low mass stars should be still evolving, identified by a very low metallicity (or no metals) (z ~ 5 to 15) ...
... observed but should be detected in 2 ways: -High mass stars explode as supernovae and produce a GRBs (z ~ 15 ?) GRB at z~8.2 = pop. III? -First generations of low mass stars should be still evolving, identified by a very low metallicity (or no metals) (z ~ 5 to 15) ...
Return both exam and scantron sheet when you
... (a) their motion along epicycles. (b) difference in speeds of the Earth and another planet in their orbits around the Sun. (c) planets stopping their eastward motion , moving westward awhile, and then resuming their eastward motion. (d) [None of the above.] 71. At the time of Copernicus, the fact th ...
... (a) their motion along epicycles. (b) difference in speeds of the Earth and another planet in their orbits around the Sun. (c) planets stopping their eastward motion , moving westward awhile, and then resuming their eastward motion. (d) [None of the above.] 71. At the time of Copernicus, the fact th ...
Astronomy Library wk 6.cwk (WP)
... As a body is heated, the peak intensity occurs at shorter (more energetic) wavelengths. ...
... As a body is heated, the peak intensity occurs at shorter (more energetic) wavelengths. ...
Measuring the Properties of Stars
... Math Help: Stefan-Boltzman Law Math Help: (m + M)P2 = a3 Math Help: Stefan-Boltzman Law This equation, L=4R2T4, known as the Stefan-Boltzman Law, tells us how much power per second is being radiated by the surface of a particular star. Astronomers call this power Luminosity, and it has dependancy ...
... Math Help: Stefan-Boltzman Law Math Help: (m + M)P2 = a3 Math Help: Stefan-Boltzman Law This equation, L=4R2T4, known as the Stefan-Boltzman Law, tells us how much power per second is being radiated by the surface of a particular star. Astronomers call this power Luminosity, and it has dependancy ...
Astronomy 1020 Exam 4 Review Questions
... 1. What is meant by the asymptotic giant branch? Describe the interior structure of a star when it is on the AGB. 2. What is meant by dredge up and by thermal pulse ? 3. How are carbon stars made? 4. What is a planetary nebula? Why does such a nebula shine? 5. What are the differences between a deta ...
... 1. What is meant by the asymptotic giant branch? Describe the interior structure of a star when it is on the AGB. 2. What is meant by dredge up and by thermal pulse ? 3. How are carbon stars made? 4. What is a planetary nebula? Why does such a nebula shine? 5. What are the differences between a deta ...
10438 starlight - The Described and Captioned Media Program
... nuclear physics, and theoretical physics. In this program, viewers examine how our basic knowledge about stars has been gained from studying the light we receive from stars. The study of starlight not only reveals straightforward information like the varying brightness of stars, but it also shows ot ...
... nuclear physics, and theoretical physics. In this program, viewers examine how our basic knowledge about stars has been gained from studying the light we receive from stars. The study of starlight not only reveals straightforward information like the varying brightness of stars, but it also shows ot ...
Astrophysics by Daniel Yang
... wavelengths. The frequencies absorbed are identical to the frequencies it would emit when incandescent. - Describe the technology needed to measure astronomical spectra To measure spectra, light from the source must be collected then dispersed to form a spectrum. Afterwards, the spectrum can be reco ...
... wavelengths. The frequencies absorbed are identical to the frequencies it would emit when incandescent. - Describe the technology needed to measure astronomical spectra To measure spectra, light from the source must be collected then dispersed to form a spectrum. Afterwards, the spectrum can be reco ...
Fulltext PDF
... The process of formation of a star can be divided into three phases. The first, known as 'star formation', involves massive interstellar clouds or cloud fragments, which have cooled to the point where they are detectable in molecular lines (such as CO) but which are unable to collapse because of an ...
... The process of formation of a star can be divided into three phases. The first, known as 'star formation', involves massive interstellar clouds or cloud fragments, which have cooled to the point where they are detectable in molecular lines (such as CO) but which are unable to collapse because of an ...
Type II supernova

A Type II supernova (plural: supernovae or supernovas) results from the rapid collapse and violent explosion of a massive star. A star must have at least 8 times, and no more than 40–50 times, the mass of the Sun (M☉) for this type of explosion. It is distinguished from other types of supernovae by the presence of hydrogen in its spectrum. Type II supernovae are mainly observed in the spiral arms of galaxies and in H II regions, but not in elliptical galaxies.Stars generate energy by the nuclear fusion of elements. Unlike the Sun, massive stars possess the mass needed to fuse elements that have an atomic mass greater than hydrogen and helium, albeit at increasingly higher temperatures and pressures, causing increasingly shorter stellar life spans. The degeneracy pressure of electrons and the energy generated by these fusion reactions are sufficient to counter the force of gravity and prevent the star from collapsing, maintaining stellar equilibrium. The star fuses increasingly higher mass elements, starting with hydrogen and then helium, progressing up through the periodic table until a core of iron and nickel is produced. Fusion of iron or nickel produces no net energy output, so no further fusion can take place, leaving the nickel-iron core inert. Due to the lack of energy output allowing outward pressure, equilibrium is broken.When the mass of the inert core exceeds the Chandrasekhar limit of about 1.4 M☉, electron degeneracy alone is no longer sufficient to counter gravity and maintain stellar equilibrium. A cataclysmic implosion takes place within seconds, in which the outer core reaches an inward velocity of up to 23% of the speed of light and the inner core reaches temperatures of up to 100 billion kelvin. Neutrons and neutrinos are formed via reversed beta-decay, releasing about 1046 joules (100 foes) in a ten-second burst. The collapse is halted by neutron degeneracy, causing the implosion to rebound and bounce outward. The energy of this expanding shock wave is sufficient to accelerate the surrounding stellar material to escape velocity, forming a supernova explosion, while the shock wave and extremely high temperature and pressure briefly allow for theproduction of elements heavier than iron. Depending on initial size of the star, the remnants of the core form a neutron star or a black hole. Because of the underlying mechanism, the resulting nova is also described as a core-collapse supernova.There exist several categories of Type II supernova explosions, which are categorized based on the resulting light curve—a graph of luminosity versus time—following the explosion. Type II-L supernovae show a steady (linear) decline of the light curve following the explosion, whereas Type II-P display a period of slower decline (a plateau) in their light curve followed by a normal decay. Type Ib and Ic supernovae are a type of core-collapse supernova for a massive star that has shed its outer envelope of hydrogen and (for Type Ic) helium. As a result, they appear to be lacking in these elements.