
On the onset of runaway stellar collisions in dense star clusters I
... objects evolve into intermediate mass black holes. Numerical simulations carried out by Portegies Zwart et al. (2004) show that the onset of a runaway merger depends on both the dynamical friction timescale and the central concentration of the star cluster. In particular, a necessary condition for t ...
... objects evolve into intermediate mass black holes. Numerical simulations carried out by Portegies Zwart et al. (2004) show that the onset of a runaway merger depends on both the dynamical friction timescale and the central concentration of the star cluster. In particular, a necessary condition for t ...
PPT - Cornell University
... • As self-gravity decouples the protogalaxy from the Hubble flow, [l/(d l/d t)] becomes v.large and the growth of l ceases ...
... • As self-gravity decouples the protogalaxy from the Hubble flow, [l/(d l/d t)] becomes v.large and the growth of l ceases ...
THE DEARTH OF UV-BRIGHT STARS IN M32
... The exposure times retained for each visit are listed in Table 1. We then applied a geometric distortion correction to each visit’s image, using the IRAF DRIZZLE package (Fruchter & Hook 2002). Because of inaccuracies in the STIS geometric distortion solution, the residual distortions in the resulti ...
... The exposure times retained for each visit are listed in Table 1. We then applied a geometric distortion correction to each visit’s image, using the IRAF DRIZZLE package (Fruchter & Hook 2002). Because of inaccuracies in the STIS geometric distortion solution, the residual distortions in the resulti ...
Detection of Planetary Transits Across a Sun
... variations were due to an orbiting companion and not due to some form of stellar variability), and to search for planetary transits. We obtained photometric observations using the STARE Project Schmidt camera (focal length = 286 mm, f/2.9), which images a eld 6 square onto a 2034 2034 pixel CCD ...
... variations were due to an orbiting companion and not due to some form of stellar variability), and to search for planetary transits. We obtained photometric observations using the STARE Project Schmidt camera (focal length = 286 mm, f/2.9), which images a eld 6 square onto a 2034 2034 pixel CCD ...
Slide 1
... i. If a collapsing star of over 3 solar masses does not eject matter, it becomes a black hole. ii. a mass of an order of magnitude between 105 and 1010 of solar masses. Most, if not all galaxies, including the Milky Way, contain supermassive black holes at their galactic centers. 7. Dark Matter and ...
... i. If a collapsing star of over 3 solar masses does not eject matter, it becomes a black hole. ii. a mass of an order of magnitude between 105 and 1010 of solar masses. Most, if not all galaxies, including the Milky Way, contain supermassive black holes at their galactic centers. 7. Dark Matter and ...
M. Meixner
... NIRCam and MIRI can be used to identify dusty evolved stars which can then be compared to precomputed models such as GRAMS to derive dust mass loss returns. Spectroscopy of sources with MIRI or NIRSpec can help identify the dust species and correlate with type of star and environment. Time monitorin ...
... NIRCam and MIRI can be used to identify dusty evolved stars which can then be compared to precomputed models such as GRAMS to derive dust mass loss returns. Spectroscopy of sources with MIRI or NIRSpec can help identify the dust species and correlate with type of star and environment. Time monitorin ...
3-D Star Map of the 15 Nearest Stars
... • Poke a starter hole in the base plate for each of the 11 star systems • Poke the hole using the left-over “starter pin” • Make sure the starter hole only penetrates the upper cardboard, not the foam beneath • The two binaries, UV Ceti and Sirius, and the triple star system Alpha and Proxima Centau ...
... • Poke a starter hole in the base plate for each of the 11 star systems • Poke the hole using the left-over “starter pin” • Make sure the starter hole only penetrates the upper cardboard, not the foam beneath • The two binaries, UV Ceti and Sirius, and the triple star system Alpha and Proxima Centau ...
Summary of Astronomy
... auroras, too. In 1955, scientists discovered that Jupiter was giving off radio emissions, which suggested the planet might have a magnetic field. In 1974, the Pioneer-10 spacecraft had instruments aboard that detected a magnetosphere on Jupiter. Five years later, the spacecraft Voyager captured the ...
... auroras, too. In 1955, scientists discovered that Jupiter was giving off radio emissions, which suggested the planet might have a magnetic field. In 1974, the Pioneer-10 spacecraft had instruments aboard that detected a magnetosphere on Jupiter. Five years later, the spacecraft Voyager captured the ...
OUTFLOW INFALL AND ROTATION IN HIGH
... On the other hand, if O protostars do not have disks, a physical explanation is required: • O-star disks “hidden” inside toroids • O-star disk lifetime too short, i.e. less than rotation period: photo-evaporation by O star (Hollenbach et al. ...
... On the other hand, if O protostars do not have disks, a physical explanation is required: • O-star disks “hidden” inside toroids • O-star disk lifetime too short, i.e. less than rotation period: photo-evaporation by O star (Hollenbach et al. ...
Brans-Dicke Boson Stars: Configurations and Stability through
... relativistic case (for a given central scalar field density), irrespective of the coupling. A vital point to consider is that when one finds cosmological solutions in scalar–tensor theories, the gravitational coupling is normally evolving. This has important implications for astrophysical objects, b ...
... relativistic case (for a given central scalar field density), irrespective of the coupling. A vital point to consider is that when one finds cosmological solutions in scalar–tensor theories, the gravitational coupling is normally evolving. This has important implications for astrophysical objects, b ...
DETECTION OF PLANETARY TRANSITS ACROSS A SUN
... of the transit curve. These are the planetary radius Rp, the stellar radius Rs, the stellar mass Ms, the orbital inclination angle i, and the limb darkening parameter cl, where the normalized stellar surface brightness profile is written as Bl(m) = 1 ! c l(1 ! m) and m is the cosine of the angle bet ...
... of the transit curve. These are the planetary radius Rp, the stellar radius Rs, the stellar mass Ms, the orbital inclination angle i, and the limb darkening parameter cl, where the normalized stellar surface brightness profile is written as Bl(m) = 1 ! c l(1 ! m) and m is the cosine of the angle bet ...
幻灯片 1
... masses: ~1.5 - 2.5 Msun • spectral type: A5 - F2. • found on the intersection of the classical instability strip and the main sequence in the Hertzsprung-Russell diagram • excitation mechanism: κ mechanism ...
... masses: ~1.5 - 2.5 Msun • spectral type: A5 - F2. • found on the intersection of the classical instability strip and the main sequence in the Hertzsprung-Russell diagram • excitation mechanism: κ mechanism ...
L45 DETECTION OF PLANETARY TRANSITS ACROSS A SUN
... of the transit curve. These are the planetary radius Rp, the stellar radius Rs, the stellar mass Ms, the orbital inclination angle i, and the limb darkening parameter cl, where the normalized stellar surface brightness profile is written as Bl(m) = 1 2 c l(1 2 m) and m is the cosine of the angle bet ...
... of the transit curve. These are the planetary radius Rp, the stellar radius Rs, the stellar mass Ms, the orbital inclination angle i, and the limb darkening parameter cl, where the normalized stellar surface brightness profile is written as Bl(m) = 1 2 c l(1 2 m) and m is the cosine of the angle bet ...
Astronomy 321 --- Homework Exercise: Star Wheel
... In the tables below, the first column is the constellation, with its standard 3-letter abbreviation in parentheses. For constellations with bright stars, one or two of these bright stars are listed in the 2nd column and should also be learned. The 3rd column lists other objects of interest (e.g., st ...
... In the tables below, the first column is the constellation, with its standard 3-letter abbreviation in parentheses. For constellations with bright stars, one or two of these bright stars are listed in the 2nd column and should also be learned. The 3rd column lists other objects of interest (e.g., st ...
FP11: DRAKE et al. - Astronomical Institute WWW Homepage
... Li spots Figure 3 shows spectra of HD 3980 in the Li I 6708 Å spectral region. The rotational phases of HD 3980 were calculated using the ephemeris from Maitzen et al. (1980). Two “Li spots” are observed on the surface of the star. The Li I line originated in spot 1 appears at the phase φ = – 0.146 ...
... Li spots Figure 3 shows spectra of HD 3980 in the Li I 6708 Å spectral region. The rotational phases of HD 3980 were calculated using the ephemeris from Maitzen et al. (1980). Two “Li spots” are observed on the surface of the star. The Li I line originated in spot 1 appears at the phase φ = – 0.146 ...
A hypervelocity star from the Large Magellanic Cloud
... initial velocity between the binary and the single star as the total energy of the system is dominated by the binding energy of the binary rather than by the kinetic energy of the incoming star. Additional experiments performed with initial velocities of 5 and 10 km s−1 showed no appreciable differe ...
... initial velocity between the binary and the single star as the total energy of the system is dominated by the binding energy of the binary rather than by the kinetic energy of the incoming star. Additional experiments performed with initial velocities of 5 and 10 km s−1 showed no appreciable differe ...
Empirical properties of Very Massive Stars
... Spectrally, massive stars appear as O and early B (i.e. earlier than B3) stars on the main sequence. Once they evolve, they become supergiants of all sorts: blue supergiants (spectral type O, B and A), yellow supergiants (spectral type F and G) and red supergiants (spectral type K and M). The most m ...
... Spectrally, massive stars appear as O and early B (i.e. earlier than B3) stars on the main sequence. Once they evolve, they become supergiants of all sorts: blue supergiants (spectral type O, B and A), yellow supergiants (spectral type F and G) and red supergiants (spectral type K and M). The most m ...
Chapter 9 Parallax and Distance to Stars
... distance of 1 AU. The angle p will be small (measured in arcseconds) and is 21 of the total observed angular displacement. Astronomers adopted a new unit of distance, the parsec, to measure stellar distances. If d is in parsecs, then the following equation applies: d= ...
... distance of 1 AU. The angle p will be small (measured in arcseconds) and is 21 of the total observed angular displacement. Astronomers adopted a new unit of distance, the parsec, to measure stellar distances. If d is in parsecs, then the following equation applies: d= ...
The white dwarf binary pathways survey – I. A sample of FGK stars
... Key words: binaries: close – stars: white dwarfs – stars: early-type – stars: evolution ...
... Key words: binaries: close – stars: white dwarfs – stars: early-type – stars: evolution ...
arXiv:1604.01613v2 [astro-ph.SR] 23 Aug 2016
... Key words: binaries: close – stars: white dwarfs – stars: early-type – stars: evolution ...
... Key words: binaries: close – stars: white dwarfs – stars: early-type – stars: evolution ...
Astronomy 535 Stellar Structure Evolution
... formation, populations, galaxies, baryonic matter in general profoundly depends on stellar evolution • Fits of models to observations by means of free parameters is standard procedure, but gives unreliable or downright bad results for most applications • Must be able to predict evolution of a star a ...
... formation, populations, galaxies, baryonic matter in general profoundly depends on stellar evolution • Fits of models to observations by means of free parameters is standard procedure, but gives unreliable or downright bad results for most applications • Must be able to predict evolution of a star a ...
The DWARF project
... Practice: We can calculate the recommended texp for a given telescope, CCD, and star brightness combination in order to achieve the required precision ...
... Practice: We can calculate the recommended texp for a given telescope, CCD, and star brightness combination in order to achieve the required precision ...
Contents
... The only introduced concept in this section is that the gravitational field outside a sphericallysymmetric body is identical to that of an identical point mass situated at the centre of the body. The point of introducing this statement [essentially Gauss’s Law] is to allow for the application of New ...
... The only introduced concept in this section is that the gravitational field outside a sphericallysymmetric body is identical to that of an identical point mass situated at the centre of the body. The point of introducing this statement [essentially Gauss’s Law] is to allow for the application of New ...
Intro to the Night Sky - AST 114, Astronomy Lab II for Spring 2017!
... When one looks at the sky, or at the photos in the Audubon Guide, one quickly notices that all stars do not appear the same. There is a very wide range in brightness. Stars also appear in different colors. Astronomers occasionally use an archaic method of specifying the brightness of an object. This ...
... When one looks at the sky, or at the photos in the Audubon Guide, one quickly notices that all stars do not appear the same. There is a very wide range in brightness. Stars also appear in different colors. Astronomers occasionally use an archaic method of specifying the brightness of an object. This ...
Models of red giants in the CoRoT asteroseismology fields
... present a comparison between radii and masses determined using the different combinations of seismic and non-seismic constraints. Radii and masses are computed using Eqs. (1) and (2), and obtained by the other methods (Eqs. (3), (4), and parallax). We also consider extinctions, AV , using Drimmel et ...
... present a comparison between radii and masses determined using the different combinations of seismic and non-seismic constraints. Radii and masses are computed using Eqs. (1) and (2), and obtained by the other methods (Eqs. (3), (4), and parallax). We also consider extinctions, AV , using Drimmel et ...
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.