
revealing star formation processes in the nearby universe
... • UV & FIR light are subject to assumptions about extinction and reprocessing of light • Radio recombination lines provide a direct measure of the ionized gas ...
... • UV & FIR light are subject to assumptions about extinction and reprocessing of light • Radio recombination lines provide a direct measure of the ionized gas ...
Magnetized Gravitational Collapse & Star Formation
... Note trapping of field at origin produces split monopole with long lever arm for magnetic braking. ...
... Note trapping of field at origin produces split monopole with long lever arm for magnetic braking. ...
The Relative Ages of M5 and Pal 4/Eridanus from their
... “none of the above” category; neither spiral nor elliptical appear white & dusty with ISM • have more in common with the disk component of spirals distant galaxies are more likely to be irregular • they were more common when the Universe was young ...
... “none of the above” category; neither spiral nor elliptical appear white & dusty with ISM • have more in common with the disk component of spirals distant galaxies are more likely to be irregular • they were more common when the Universe was young ...
Stellar Mass Assembly History
... of galaxies to high redshift; reliability depends on having spectroscopic redshifts and long wavelength data • It is now clear that mass assembly since z~2 does not proceed hierarchically; growth is suppressed in high mass systems at early times continuing in low mass systems to z~0 (`downsizing’) • ...
... of galaxies to high redshift; reliability depends on having spectroscopic redshifts and long wavelength data • It is now clear that mass assembly since z~2 does not proceed hierarchically; growth is suppressed in high mass systems at early times continuing in low mass systems to z~0 (`downsizing’) • ...
The Milky Way
... • The gravitational field of the density wave causes stars and gas to slow down near the arm • This compresses the interstellar clouds, triggering the formation of stars. • New stars appear on the “downstream” side of the densest part of the spiral arms. • The entire arm pattern rotates around the M ...
... • The gravitational field of the density wave causes stars and gas to slow down near the arm • This compresses the interstellar clouds, triggering the formation of stars. • New stars appear on the “downstream” side of the densest part of the spiral arms. • The entire arm pattern rotates around the M ...
Bright Stars and Faint Stars: the stellar magnitude system
... • Apparent magnitude is the brightness of an object as it appears to you • System due to Hipparchos (2nd century BC) • Nowadays system made more precise • Magnitude changes are “logarithmic”, each magnitude means factor of 2.512 in brightness • See Table 16.2 ...
... • Apparent magnitude is the brightness of an object as it appears to you • System due to Hipparchos (2nd century BC) • Nowadays system made more precise • Magnitude changes are “logarithmic”, each magnitude means factor of 2.512 in brightness • See Table 16.2 ...
Folie 1
... If molecular clouds are the sites of star formation what conditions must exist for collapse to occur? • James Jeans investigated this with simplified assumptions, considering the effects of small deviations from hydrostatic equilibrium with spherical symmetric collapse and neglecting the effects due ...
... If molecular clouds are the sites of star formation what conditions must exist for collapse to occur? • James Jeans investigated this with simplified assumptions, considering the effects of small deviations from hydrostatic equilibrium with spherical symmetric collapse and neglecting the effects due ...
(Relative) Distances from the HST Snapshot Database
... central He burning lifetime, one expects that atomic diffusion becomes more and more efficent in decreasing the envelope He abundance, implying the quenching of the HeII convection. At the same time, larger effective temperatures should enhance radiative levitation, producing a change in the surface ...
... central He burning lifetime, one expects that atomic diffusion becomes more and more efficent in decreasing the envelope He abundance, implying the quenching of the HeII convection. At the same time, larger effective temperatures should enhance radiative levitation, producing a change in the surface ...
Measuring the Distances to the Stars: Parallax What sets the parallax limit? 1
... • In concept, solve for R0 = 7.94 ± 0.38 kpc • (actually, it comes out of orbit fit) ...
... • In concept, solve for R0 = 7.94 ± 0.38 kpc • (actually, it comes out of orbit fit) ...
GAIA A Stereoscopic Census of our Galaxy
... – ~1600 Earth-crossers >1 km predicted (100 currently known) – detection limit: 260–590 m at 1 AU, depending on albedo ...
... – ~1600 Earth-crossers >1 km predicted (100 currently known) – detection limit: 260–590 m at 1 AU, depending on albedo ...
What you need to know
... Is there a star that is in an unobservable position? When a star travels from being below the observer’s horizon to being above the observer’s horizon, is that star rising or ...
... Is there a star that is in an unobservable position? When a star travels from being below the observer’s horizon to being above the observer’s horizon, is that star rising or ...
Report for European Helioseismology and Asteroseismology Network
... artificial timeseries data that mimic observations made by Kepler. The first release of artificial timeseries data was made on three artificial stars (named Pancho, Boris and Katrina). This release comprised multiple datasets on each artificial star, to cover a range of different apparent visual mag ...
... artificial timeseries data that mimic observations made by Kepler. The first release of artificial timeseries data was made on three artificial stars (named Pancho, Boris and Katrina). This release comprised multiple datasets on each artificial star, to cover a range of different apparent visual mag ...
Document
... In addition, because the strange quark mass is close to u and d quarks, the “soup” may contain u, d, and s. Quark/hybrid stars: typically refer to a NS whose cores contain a mixed phase of confined and deconfined matter. These stars are bound by gravity. Strange stars: refer to stars that have only ...
... In addition, because the strange quark mass is close to u and d quarks, the “soup” may contain u, d, and s. Quark/hybrid stars: typically refer to a NS whose cores contain a mixed phase of confined and deconfined matter. These stars are bound by gravity. Strange stars: refer to stars that have only ...
Stellar Winds and Supernova Remnants: Interaction with the ISM
... V-band image of IRC+10216 showing shell-like structures in the circumstellar envelope (90''x 90'') Mauron & Huggins (2010) ...
... V-band image of IRC+10216 showing shell-like structures in the circumstellar envelope (90''x 90'') Mauron & Huggins (2010) ...
Collisions and close encounters involving massive main
... of the stars. The fits of the three-dimensional SPH models to the one-dimensional ATON model are clearly very good. Note that none of the 9 M models has a mass of exactly 9 M . The mass of the ATON model star is 8.85 M , of the high-resolution SPH model is 8.75 M and of the low-resolution model ...
... of the stars. The fits of the three-dimensional SPH models to the one-dimensional ATON model are clearly very good. Note that none of the 9 M models has a mass of exactly 9 M . The mass of the ATON model star is 8.85 M , of the high-resolution SPH model is 8.75 M and of the low-resolution model ...
IEEE 2 Column Format
... The masses of MPMs can be determined by comparing their observed magnitudes with those predicted by a stellar evolutionary model (For known age, reddening, distance and metallicity). The MF values are given in Table 2 by considering the negligible effect of field star contamination. Fig. 2 shows the ...
... The masses of MPMs can be determined by comparing their observed magnitudes with those predicted by a stellar evolutionary model (For known age, reddening, distance and metallicity). The MF values are given in Table 2 by considering the negligible effect of field star contamination. Fig. 2 shows the ...
A Collection of Curricula for the STARLAB Hindu Mythology Cylinder
... The four corners of a celestial bed. ...
... The four corners of a celestial bed. ...
A Collection of Curricula for the STARLAB Hindu Mythology Cylinder
... The four corners of a celestial bed. ...
... The four corners of a celestial bed. ...
protostellar disks under the influence of winds and uv radiation
... during his visit to the Max-Planck-Institut für Astrophysik in Munich. (Our paths may have crossed before this, but I just don’t remember.) As a recent post-doc at MPIA I had just added an ionization/recombination module to the Yorke & Krügel (1977) code to calculate more realistically the formati ...
... during his visit to the Max-Planck-Institut für Astrophysik in Munich. (Our paths may have crossed before this, but I just don’t remember.) As a recent post-doc at MPIA I had just added an ionization/recombination module to the Yorke & Krügel (1977) code to calculate more realistically the formati ...
SS_L2 - TCD Maths
... There are two main circumstances under which 2.19 will fail. 1.In the centre of main-sequence stars, the radiation flux l/4r2 can become very large, whilst remains small. Thus the temperature gradient dlnT/dlnP required for radiative equilibrium becomes large, and the material becomes convective ...
... There are two main circumstances under which 2.19 will fail. 1.In the centre of main-sequence stars, the radiation flux l/4r2 can become very large, whilst remains small. Thus the temperature gradient dlnT/dlnP required for radiative equilibrium becomes large, and the material becomes convective ...
Mass-radius Relations for Helium White Dwarfs
... In this paper, we give the first results of our white dwarf models including neutrino emission, that is M-R relations of the fully degenerate helium WDs for masses greater than 0.4 M are presented. Figure 1. shows the M-R relations for helium WDs calculated by Hamada and Salpeter [5], Althaus and B ...
... In this paper, we give the first results of our white dwarf models including neutrino emission, that is M-R relations of the fully degenerate helium WDs for masses greater than 0.4 M are presented. Figure 1. shows the M-R relations for helium WDs calculated by Hamada and Salpeter [5], Althaus and B ...
ch 15 notes
... The brightness of a star depends on both its size and its temperature. It can be described in two ways: Apparent brightness: Brightness as seen from Earth (i.e. the sun is the brightest star to us only because it’s so close). Absolute brightness: Brightness the star would have if it were at a standa ...
... The brightness of a star depends on both its size and its temperature. It can be described in two ways: Apparent brightness: Brightness as seen from Earth (i.e. the sun is the brightest star to us only because it’s so close). Absolute brightness: Brightness the star would have if it were at a standa ...
Chapter 15 Stars, Galaxies, and Universe Galaxies
... The brightness of a star depends on both its size and its temperature. It can be described in two ways: Apparent brightness: Brightness as seen from Earth (i.e. the sun is the brightest star to us only because it’s so close). Absolute brightness: Brightness the star would have if it were at a standa ...
... The brightness of a star depends on both its size and its temperature. It can be described in two ways: Apparent brightness: Brightness as seen from Earth (i.e. the sun is the brightest star to us only because it’s so close). Absolute brightness: Brightness the star would have if it were at a standa ...
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.