
Lecture 12: Accretion
... L1 point and be captured by the companion: Roche-lobe overflow Even if the stars are not close enough for Roche-lobe overflow to occur, mass from a strong stellar wind can be captured by the other star: wind-driven accretion ...
... L1 point and be captured by the companion: Roche-lobe overflow Even if the stars are not close enough for Roche-lobe overflow to occur, mass from a strong stellar wind can be captured by the other star: wind-driven accretion ...
STRUCTURAL CHARACTERISTICS AND STELLAR
... 1991). The area weighted colors are less aected and should be more representative of the underlying stellar population. Indeed, this is a much greater concern for broad band colors of HSB disks, where the star formation rate and H II region covering factor are higher. Due to bad weather, some galax ...
... 1991). The area weighted colors are less aected and should be more representative of the underlying stellar population. Indeed, this is a much greater concern for broad band colors of HSB disks, where the star formation rate and H II region covering factor are higher. Due to bad weather, some galax ...
Hunting for Orphaned Central Compact Objects among Radio Pulsars
... Ė ≡ 4π 2 I Ṗ /P 3 = 1031 –1032 erg s−1 , where I is the neutron star moment of inertia. These values are nearly two orders of magnitude smaller than the CCO’s X-ray luminosities, implying that the sources cannot be entirely powered by rotation. The characteristic age τc = P/2Ṗ of the three CCOs i ...
... Ė ≡ 4π 2 I Ṗ /P 3 = 1031 –1032 erg s−1 , where I is the neutron star moment of inertia. These values are nearly two orders of magnitude smaller than the CCO’s X-ray luminosities, implying that the sources cannot be entirely powered by rotation. The characteristic age τc = P/2Ṗ of the three CCOs i ...
A Second Shell in the Fornax dSph Galaxy
... all the stars within this feature are real stellar sources, and the star-finding algorithm does not appear to have missed any stars in the remainder of the field. Also, given the high Galactic latitude of Fornax, we do not expect this feature to be caused by dust extinction. Correspondingly, a visua ...
... all the stars within this feature are real stellar sources, and the star-finding algorithm does not appear to have missed any stars in the remainder of the field. Also, given the high Galactic latitude of Fornax, we do not expect this feature to be caused by dust extinction. Correspondingly, a visua ...
A Theory of Extrasolar Giant Planets
... results of GG73 and GPGO to infer simple power-law relations for the variation of luminosity L and radius R as a function of mass M and time t. Black's relations are roughly valid for objects close in mass to 1 MJ and close in age to 4.5 Gyr. However, as we discuss below, Black's formulas become ver ...
... results of GG73 and GPGO to infer simple power-law relations for the variation of luminosity L and radius R as a function of mass M and time t. Black's relations are roughly valid for objects close in mass to 1 MJ and close in age to 4.5 Gyr. However, as we discuss below, Black's formulas become ver ...
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... March, and it is followed by the marriage season, from Chaita (around April) to Ashad (June) —before the monsoon season. During the New Moon of Akhadi (July), a goat is sacrificed in anticipation of a good monsoon. When young girls come of age, there is the festival of teej in August/ September when ...
... March, and it is followed by the marriage season, from Chaita (around April) to Ashad (June) —before the monsoon season. During the New Moon of Akhadi (July), a goat is sacrificed in anticipation of a good monsoon. When young girls come of age, there is the festival of teej in August/ September when ...
Discovery of the optical counterpart to the X
... λ7065. The Balmer series up to H13 can be seen. The spectra were taken from the WHT on September 14, 2003 ...
... λ7065. The Balmer series up to H13 can be seen. The spectra were taken from the WHT on September 14, 2003 ...
ertan et al 11cesme
... AXP/SGRs. For the sources with weaker magnetic dipole fields, rin comes out of the light cylinder earlier than it does for the sources with stronger dipole fields. After this point, P remains almost constant because of decreasing efficiency of the disk torque [2]. As seen in Fig. 1, the model source ...
... AXP/SGRs. For the sources with weaker magnetic dipole fields, rin comes out of the light cylinder earlier than it does for the sources with stronger dipole fields. After this point, P remains almost constant because of decreasing efficiency of the disk torque [2]. As seen in Fig. 1, the model source ...
A self-consistent empirical model atmosphere, abundance and
... Context. Chemically peculiar (CP) stars are unique natural laboratories for the investigation of the microscopic diffusion processes of chemical elements. The element segregation under the influence of gravity and radiation pressure leads to the appearance of strong abundance gradients in the atmosph ...
... Context. Chemically peculiar (CP) stars are unique natural laboratories for the investigation of the microscopic diffusion processes of chemical elements. The element segregation under the influence of gravity and radiation pressure leads to the appearance of strong abundance gradients in the atmosph ...
Microlensing - Caltech Astronomy
... lightcurve: this method is potentially sensitive to low-mass planets down to a few Earth masses, below the range accessible to radial-velocity planet searches. Two groups called PLANET and MPS are now searching for this effect. ...
... lightcurve: this method is potentially sensitive to low-mass planets down to a few Earth masses, below the range accessible to radial-velocity planet searches. Two groups called PLANET and MPS are now searching for this effect. ...
Dynamical Tides in Rotating Binary Stars
... The standard weak friction theory for tidal interaction in binary stars, first introduced by Darwin (1879), and developed in detail by many authors (e.g., Alexander 1973; Kopal 1978; Hut 1981), is based on the assumption of static tide in hydrostatic equilibrium. In the presence of finite dissipatio ...
... The standard weak friction theory for tidal interaction in binary stars, first introduced by Darwin (1879), and developed in detail by many authors (e.g., Alexander 1973; Kopal 1978; Hut 1981), is based on the assumption of static tide in hydrostatic equilibrium. In the presence of finite dissipatio ...
Feedback from winds and supernovae in massive stellar clusters – I
... Published by Oxford University Press on behalf of the Royal Astronomical Society ...
... Published by Oxford University Press on behalf of the Royal Astronomical Society ...
EL CVn-type binaries - Discovery of 17 helium white dwarf
... is typically 0.001 – 0.005M⊙ , much greater than for typical white dwarfs (hydrogen layer mass < 10−4 M⊙ ). The preHe-WD then evolves at nearly constant luminosity towards higher effective temperatures as a result of the gradual reduction in the hydrogen layer mass through stable p-p chain shell bur ...
... is typically 0.001 – 0.005M⊙ , much greater than for typical white dwarfs (hydrogen layer mass < 10−4 M⊙ ). The preHe-WD then evolves at nearly constant luminosity towards higher effective temperatures as a result of the gradual reduction in the hydrogen layer mass through stable p-p chain shell bur ...
PS1-12SK IS A PECULIAR SUPERNOVA FROM A HE
... (Gehrels et al. 2004), in the time period MJD 56013 − 56056, for a total of 26.4 ks. Swift-XRT data have been analyzed using the latest version of the HEASOFT package available at the time of writing (v. 6.12) and corresponding calibration files. Standard filtering and screening criteria have been a ...
... (Gehrels et al. 2004), in the time period MJD 56013 − 56056, for a total of 26.4 ks. Swift-XRT data have been analyzed using the latest version of the HEASOFT package available at the time of writing (v. 6.12) and corresponding calibration files. Standard filtering and screening criteria have been a ...
The chemical composition of two supergiants in the dwarf
... globular cluster space velocities are not known. The distance to WLM puts the tip of the red giant branch at V ∼ 22, which is out of reach for detailed chemical abundance analyses of its RGB population. However, there are bright blue supergiants in WLM’s central star forming region with V ∼ 18. Thes ...
... globular cluster space velocities are not known. The distance to WLM puts the tip of the red giant branch at V ∼ 22, which is out of reach for detailed chemical abundance analyses of its RGB population. However, there are bright blue supergiants in WLM’s central star forming region with V ∼ 18. Thes ...
L43 THE STARFISH TWINS: TWO YOUNG
... N1 with S4, N2 with S3, and N3 with S1 is equally plausible. A comparison of the fluxes of both PNs at different wavelengths indicates that they are intrinsically similar in size and brightness but are located at different distances. We find that the stellar blue and visual (continuum) fluxes, the H ...
... N1 with S4, N2 with S3, and N3 with S1 is equally plausible. A comparison of the fluxes of both PNs at different wavelengths indicates that they are intrinsically similar in size and brightness but are located at different distances. We find that the stellar blue and visual (continuum) fluxes, the H ...
Astronomy Astrophysics Astrophysical parameters and orbital solution of the peculiar X-ray
... et al. 2006a; Blay et al. 2012), leading to the definition of the supergiant fast X-ray transients (SFXTs, Negueruela et al. 2006b) as a sub-class of SGXBs. SFXTs spend most of their time at X-ray luminosities between LX ∼ 1032 to 1034 erg s−1 , well below the “normal” X-ray luminosity of SGXBs, wit ...
... et al. 2006a; Blay et al. 2012), leading to the definition of the supergiant fast X-ray transients (SFXTs, Negueruela et al. 2006b) as a sub-class of SGXBs. SFXTs spend most of their time at X-ray luminosities between LX ∼ 1032 to 1034 erg s−1 , well below the “normal” X-ray luminosity of SGXBs, wit ...
Abstracts - Space Telescope Science Institute
... Over the past three years, two of the largest-ever HST stellar spectroscopic Guest Observer programs have been undertaken. The “Advanced Spectral Library (ASTRAL)” Project (PI = T. Ayres) consists of two Treasury Programs, the first in Cycle 18 on “Cool Stars” (GO-12278) and the second in the curren ...
... Over the past three years, two of the largest-ever HST stellar spectroscopic Guest Observer programs have been undertaken. The “Advanced Spectral Library (ASTRAL)” Project (PI = T. Ayres) consists of two Treasury Programs, the first in Cycle 18 on “Cool Stars” (GO-12278) and the second in the curren ...
Kinematics of Arp 270: gas flows, nuclear activity
... Condon, Cotton & Broderick (2002). Then, using the calibration of Kennicutt et al. (2009) (equation 12) to correct for dust attenuation using 1.4 GHz luminosity, we have found that the global SFR for NGC 3396 needs to be corrected by a factor of 2.3 and NGC 3395 needs to be corrected by a factor of ...
... Condon, Cotton & Broderick (2002). Then, using the calibration of Kennicutt et al. (2009) (equation 12) to correct for dust attenuation using 1.4 GHz luminosity, we have found that the global SFR for NGC 3396 needs to be corrected by a factor of 2.3 and NGC 3395 needs to be corrected by a factor of ...
PS1-10jh: The Disruption of a Main-Sequence Star of Near
... This means that a complete simulation of the full problem within a single simulation is very computationally expensive. Instead, we run two separate simulations that are each wellequipped to describe the behavior of the debris stream at two different epochs. To determine the fate of the debris liber ...
... This means that a complete simulation of the full problem within a single simulation is very computationally expensive. Instead, we run two separate simulations that are each wellequipped to describe the behavior of the debris stream at two different epochs. To determine the fate of the debris liber ...
distribution and properties of a sample of massive young stars
... the slightly later ultra compact (UC) H II region stage. It is unclear whether core hydrogen burning has begun in the MYSO phase, however their association with strong molecular outflows indicates accretion is going on. As the MYSO evolves and moves towards the main sequence, it will begin to form a ...
... the slightly later ultra compact (UC) H II region stage. It is unclear whether core hydrogen burning has begun in the MYSO phase, however their association with strong molecular outflows indicates accretion is going on. As the MYSO evolves and moves towards the main sequence, it will begin to form a ...
Beasts of the Southern Wild: Discovery of nine Ultra Faint satellites
... but could be approximately estimated from the source number counts in g, r, i filters. These number counts peak at magnitudes 23.7, 23.6, 22.9 in g, r, i correspondingly, indicating that the catalogues start to be significantly affected by incompleteness at somewhat brigher magnitudes g∼23.5, r∼23.4 ...
... but could be approximately estimated from the source number counts in g, r, i filters. These number counts peak at magnitudes 23.7, 23.6, 22.9 in g, r, i correspondingly, indicating that the catalogues start to be significantly affected by incompleteness at somewhat brigher magnitudes g∼23.5, r∼23.4 ...
Variability of young solar-type stars: Spot cycles, rotation
... akin to the 11 year spot cycle of the Sun, and other possible regularities present in the distribution of the starspots. Measurements of the chromospheric emission level by high resolution spectroscopy will furthermore directly provide useful estimates of the activity level of a star. Despite the fa ...
... akin to the 11 year spot cycle of the Sun, and other possible regularities present in the distribution of the starspots. Measurements of the chromospheric emission level by high resolution spectroscopy will furthermore directly provide useful estimates of the activity level of a star. Despite the fa ...
Molecular Cloud Evolution II. From cloud formation to the early
... more massive than its mean Jeans mass, and to begin undergoing global collapse. The turbulent, nonlinear density fluctuations induce numerous local and fast collapse events while the cloud is collapsing globally, converting most of its mass to stars. Since stellar energy feedback is not included, ou ...
... more massive than its mean Jeans mass, and to begin undergoing global collapse. The turbulent, nonlinear density fluctuations induce numerous local and fast collapse events while the cloud is collapsing globally, converting most of its mass to stars. Since stellar energy feedback is not included, ou ...
The electron temperature of the inner halo of the Planetary Nebula
... approximation (ISA) model atmosphere for the hydrogen deficient Wolf Rayet type central star of the planetary nebula (CSPN), and references to selected atomic parameters may be found in Hyung et al. (2000). We adopted the abundances from the core nebula, as described by Hyung et al. (2000). The resu ...
... approximation (ISA) model atmosphere for the hydrogen deficient Wolf Rayet type central star of the planetary nebula (CSPN), and references to selected atomic parameters may be found in Hyung et al. (2000). We adopted the abundances from the core nebula, as described by Hyung et al. (2000). The resu ...
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.