Sporadic Mass Ejection in Red Supergiants
... (Kukarkin et al. 1969). Using the bolometric data obtained from Flower (1977), we estimate the mean radius at maximum and at minimum spectral phase, for which we have, at MS, R = 1.9 X 102 R 0 , T. = 3220 K, and at M8, R = 4.8 X 102 R 0 , T. = 2480 K. The difference between the radii found at extrem ...
... (Kukarkin et al. 1969). Using the bolometric data obtained from Flower (1977), we estimate the mean radius at maximum and at minimum spectral phase, for which we have, at MS, R = 1.9 X 102 R 0 , T. = 3220 K, and at M8, R = 4.8 X 102 R 0 , T. = 2480 K. The difference between the radii found at extrem ...
the opportunities and challenges for astrometry in the 21st century
... to map the shape of the corrugations in real time and distorting a flexible transfer mirror to compensate for the atmospheric corrugations; however, it is a very costly approach. At a good observing site the correlation between the atmospheric shifts experienced by two stars separated by 4 arcminute ...
... to map the shape of the corrugations in real time and distorting a flexible transfer mirror to compensate for the atmospheric corrugations; however, it is a very costly approach. At a good observing site the correlation between the atmospheric shifts experienced by two stars separated by 4 arcminute ...
Exploring the Helium Reionization Era
... cooled to the point where the electrons could combine with protons to form atoms of hydrogen and other light elements. Following this transition, called Recombination, photons were not as scattered and the universe became transparent. Ironically, the period immediately after Recombination is referre ...
... cooled to the point where the electrons could combine with protons to form atoms of hydrogen and other light elements. Following this transition, called Recombination, photons were not as scattered and the universe became transparent. Ironically, the period immediately after Recombination is referre ...
Presentazione di PowerPoint
... rather incoherent picture. The new HST cameras that will be available after SM4 will play a main role in composing the puzzle. 2) For the first time, we might have the key to solve a number of problems, like the abundance anomalies and possiby the second parameter problem (which have been there as a ...
... rather incoherent picture. The new HST cameras that will be available after SM4 will play a main role in composing the puzzle. 2) For the first time, we might have the key to solve a number of problems, like the abundance anomalies and possiby the second parameter problem (which have been there as a ...
FIRST LIGHT IN THE UNIVERSE
... formation in the Universe • We have a good understanding of the evolution of the co-moving density of SF since z~3 which accounts for the observed stellar mass density at z=0. Half the stars we see today were formed by z~2. • Galaxy populations identified by various means (sub-mm, LBGs, BzK, DRG..) ...
... formation in the Universe • We have a good understanding of the evolution of the co-moving density of SF since z~3 which accounts for the observed stellar mass density at z=0. Half the stars we see today were formed by z~2. • Galaxy populations identified by various means (sub-mm, LBGs, BzK, DRG..) ...
M - ASTRONOMY GROUP – University of St Andrews
... Very bright (MV ~ -2) Pulsate regularly (~ few days) Pulsation period P increases with luminosity L P-L relation is calibrated using Cepheids in star clusters of known distance • (e.g. Cepheids in the Hyades cluster, whose distance is known from parallax) ...
... Very bright (MV ~ -2) Pulsate regularly (~ few days) Pulsation period P increases with luminosity L P-L relation is calibrated using Cepheids in star clusters of known distance • (e.g. Cepheids in the Hyades cluster, whose distance is known from parallax) ...
ppt
... • A number of galaxies have been detected at z>6. • Mostly via Lyman-α emission lines. • JWST (if it ever flies) would find more of them at even higher redshifts. ...
... • A number of galaxies have been detected at z>6. • Mostly via Lyman-α emission lines. • JWST (if it ever flies) would find more of them at even higher redshifts. ...
ASTRONOMY 5
... What is the strongest evidence that 90% of the mass of the Galaxy is _____ in the form of dark matter? a) The orbital speeds of stars far from the Galactic center are surprisingly high, suggesting that these stars are feeling gravitational effects from unseen matter. b) Although dark matter emits no ...
... What is the strongest evidence that 90% of the mass of the Galaxy is _____ in the form of dark matter? a) The orbital speeds of stars far from the Galactic center are surprisingly high, suggesting that these stars are feeling gravitational effects from unseen matter. b) Although dark matter emits no ...
Stars and Fareys: A Screen Size Romance
... However, the center of the screen is not necessarily the point that will fit the largest possible star. Thus, we derive a 2-dimensional generalization of Farey numbers that gives the exact number of visible points from any point of an integer lattice by looking at the number of co-prime pairs in a r ...
... However, the center of the screen is not necessarily the point that will fit the largest possible star. Thus, we derive a 2-dimensional generalization of Farey numbers that gives the exact number of visible points from any point of an integer lattice by looking at the number of co-prime pairs in a r ...
Astronomy HOMEWORK Chapter 15 1. Where in the Galaxy is the
... are too high to be explained by the mass of stars, gas, and dust inside their orbits. In particular, as one goes into the extreme outskirts, orbital speeds continue to climb. Kepler’s third law would require them to go down, if there were not some large mass density in these extreme outskirts. The s ...
... are too high to be explained by the mass of stars, gas, and dust inside their orbits. In particular, as one goes into the extreme outskirts, orbital speeds continue to climb. Kepler’s third law would require them to go down, if there were not some large mass density in these extreme outskirts. The s ...
2009 - thephysicsteacher.ie
... 11. Read this passage and answer the questions below. Why do stars and the lights of distant objects twinkle? The twinkling of stars, also known as stellar scintillation, is due to atmospheric turbulence. The turbulence of the air is caused by heat changing the density and thus the refractive index ...
... 11. Read this passage and answer the questions below. Why do stars and the lights of distant objects twinkle? The twinkling of stars, also known as stellar scintillation, is due to atmospheric turbulence. The turbulence of the air is caused by heat changing the density and thus the refractive index ...
Powerpoint
... Reactions below 24Mg, e.g., 20Ne(ag)24Mg and 12C(ag)16O are, in general, not in equilibrium with their inverses (exception, 16O(ag)20Ne which has been in equilibrium since neon burning). Within the groups heavier than A = 24, except at the boundaries of the clusters, the abundance of any species ...
... Reactions below 24Mg, e.g., 20Ne(ag)24Mg and 12C(ag)16O are, in general, not in equilibrium with their inverses (exception, 16O(ag)20Ne which has been in equilibrium since neon burning). Within the groups heavier than A = 24, except at the boundaries of the clusters, the abundance of any species ...
Tom Maccarone (Texas Tech University)
... R Corona Borealis star whose wind is photoionized by an unrelated BHXB? (Maccarone & Warner 2010) ...
... R Corona Borealis star whose wind is photoionized by an unrelated BHXB? (Maccarone & Warner 2010) ...
Chapter 12 Pre-supernova evolution of massive stars
... temperature reached in these stars is smaller than the temperature required for carbon fusion. During the latest stages of evolution on the AGB these stars undergo strong mass loss which removes the remaining envelope, so that their final remnants are C-O white dwarfs. The evolution of massive stars ...
... temperature reached in these stars is smaller than the temperature required for carbon fusion. During the latest stages of evolution on the AGB these stars undergo strong mass loss which removes the remaining envelope, so that their final remnants are C-O white dwarfs. The evolution of massive stars ...
The origin of magnetism on the upper main sequence
... disc fragmentation, competitive accretion and close dynamical interactions all playing a role. Current ideas have been developed to take account of the observations that stars form in highly turbulent, high-density regions, that they form in relatively dense clusters and that most of them are in bin ...
... disc fragmentation, competitive accretion and close dynamical interactions all playing a role. Current ideas have been developed to take account of the observations that stars form in highly turbulent, high-density regions, that they form in relatively dense clusters and that most of them are in bin ...
Detecting Habitable Planets around Nearby Sun-Like Stars
... angle of sky in the direction of Cygnus/Lyra. – Stars at average distance of ~1 kpc. • Difficult to follow up by direct detection. ...
... angle of sky in the direction of Cygnus/Lyra. – Stars at average distance of ~1 kpc. • Difficult to follow up by direct detection. ...
Sample Exam for Final (with correct answers)
... (a) Clusters of galaxies are all moving away from each other. ∗ (b) Clusters of galaxies are all moving closer together. (c) New matter is always coming into existence between clusters of galaxies. (d) The laws of physics were much different in the remote past. (e) The primary properties of the univ ...
... (a) Clusters of galaxies are all moving away from each other. ∗ (b) Clusters of galaxies are all moving closer together. (c) New matter is always coming into existence between clusters of galaxies. (d) The laws of physics were much different in the remote past. (e) The primary properties of the univ ...
Structure of Neutron Stars - Relativistic Astrophysics Department
... The closest millisecond PSR. MNS=1.76+/-0.2 solar. Hopefully, this value will not be reconsidered. 2. The case of PSR J0751+1807. Initially, it was announced that it has a mass ~2.1 solar [astro-ph/0508050]. However, then in 2007 at a conference the authors announced that the result was incorrect. A ...
... The closest millisecond PSR. MNS=1.76+/-0.2 solar. Hopefully, this value will not be reconsidered. 2. The case of PSR J0751+1807. Initially, it was announced that it has a mass ~2.1 solar [astro-ph/0508050]. However, then in 2007 at a conference the authors announced that the result was incorrect. A ...
IL CIELO COME LABORATORIO – 2010/2011 STAR FORMATION
... difference of about 1 Mpc between the closest and the furthest arm of the galaxy. The mean quantity of ionizing photons is 8·1049, that is also the amount of the ionized gas. The number of stars which belong to O5 spectral class, needed to warm all the ionized gas is nearly 12 stars. In the same way ...
... difference of about 1 Mpc between the closest and the furthest arm of the galaxy. The mean quantity of ionizing photons is 8·1049, that is also the amount of the ionized gas. The number of stars which belong to O5 spectral class, needed to warm all the ionized gas is nearly 12 stars. In the same way ...
P1 The Earth in the Universe
... This theory states that the universe has always existed as it does now and hasn’t changed. The trouble is that the night sky would be completely lit up because of the billions of stars, but it’s not, so… The “Big Bang” theory This theory states that the universe started off with an explosion and eve ...
... This theory states that the universe has always existed as it does now and hasn’t changed. The trouble is that the night sky would be completely lit up because of the billions of stars, but it’s not, so… The “Big Bang” theory This theory states that the universe started off with an explosion and eve ...
Neutron Stars and Black Holes
... Map shows observed bursts with no “clumping” of bursts anywhere, particularly not within the Milky Way Bursts must originate from outside our Galaxy ...
... Map shows observed bursts with no “clumping” of bursts anywhere, particularly not within the Milky Way Bursts must originate from outside our Galaxy ...
Hot HB stars in globular clusters
... for which the existence of EHB stars has been proven spectroscopically. While the helium abundance of F1-1 is typical for sdB stars (i.e. subsolar), F2-2 surprisingly turned out to be a helium rich star. This is the first time ever that a helium rich sdB star has been reported in a globular cluster. ...
... for which the existence of EHB stars has been proven spectroscopically. While the helium abundance of F1-1 is typical for sdB stars (i.e. subsolar), F2-2 surprisingly turned out to be a helium rich star. This is the first time ever that a helium rich sdB star has been reported in a globular cluster. ...
Gravitationally redshifted absorption lines in the x
... absorption lines of Fe xxvi during the early phase of the bursts, and Fe xxv and perhaps O viii during the late phase The lines would then all have a gravitational redshift of z = 0.35, which would correspond to a neutron star in the mass range of 1.4–1.8 M๏ and in the radius range of 9–12 km. ...
... absorption lines of Fe xxvi during the early phase of the bursts, and Fe xxv and perhaps O viii during the late phase The lines would then all have a gravitational redshift of z = 0.35, which would correspond to a neutron star in the mass range of 1.4–1.8 M๏ and in the radius range of 9–12 km. ...
Main sequence
In astronomy, the main sequence is a continuous and distinctive band of stars that appears on plots of stellar color versus brightness. These color-magnitude plots are known as Hertzsprung–Russell diagrams after their co-developers, Ejnar Hertzsprung and Henry Norris Russell. Stars on this band are known as main-sequence stars or ""dwarf"" stars.After a star has formed, it generates thermal energy in the dense core region through the nuclear fusion of hydrogen atoms into helium. During this stage of the star's lifetime, it is located along the main sequence at a position determined primarily by its mass, but also based upon its chemical composition and other factors. All main-sequence stars are in hydrostatic equilibrium, where outward thermal pressure from the hot core is balanced by the inward pressure of gravitational collapse from the overlying layers. The strong dependence of the rate of energy generation in the core on the temperature and pressure helps to sustain this balance. Energy generated at the core makes its way to the surface and is radiated away at the photosphere. The energy is carried by either radiation or convection, with the latter occurring in regions with steeper temperature gradients, higher opacity or both.The main sequence is sometimes divided into upper and lower parts, based on the dominant process that a star uses to generate energy. Stars below about 1.5 times the mass of the Sun (or 1.5 solar masses (M☉)) primarily fuse hydrogen atoms together in a series of stages to form helium, a sequence called the proton–proton chain. Above this mass, in the upper main sequence, the nuclear fusion process mainly uses atoms of carbon, nitrogen and oxygen as intermediaries in the CNO cycle that produces helium from hydrogen atoms. Main-sequence stars with more than two solar masses undergo convection in their core regions, which acts to stir up the newly created helium and maintain the proportion of fuel needed for fusion to occur. Below this mass, stars have cores that are entirely radiative with convective zones near the surface. With decreasing stellar mass, the proportion of the star forming a convective envelope steadily increases, whereas main-sequence stars below 0.4 M☉ undergo convection throughout their mass. When core convection does not occur, a helium-rich core develops surrounded by an outer layer of hydrogen.In general, the more massive a star is, the shorter its lifespan on the main sequence. After the hydrogen fuel at the core has been consumed, the star evolves away from the main sequence on the HR diagram. The behavior of a star now depends on its mass, with stars below 0.23 M☉ becoming white dwarfs directly, whereas stars with up to ten solar masses pass through a red giant stage. More massive stars can explode as a supernova, or collapse directly into a black hole.