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43 Cards in this Set
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interstellar medium |
the gas and dust between the stars, is mostly concentrated near the plane of our Milky Way Galaxy and has an average density of about one atom per cubic centimeter |
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interstellar extinction |
or dimming, makes the distant stars look fainter than they should |
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interstellar reddening |
makes distant stars appear too red because dust particles in the interstellar medium scatter blue light more easily than red light. Dependence of this extinction on wavelength shows that scattering dust particles are very small. Dust made of carbon, silicates, iron, ice, and other common atoms and molecules |
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interstellar absorption lines |
made by interstellar gas that is cold and has very low density. Much narrower than the spectral lines produced in stars. Usually obvious in stellar spectra because they represent ions that cannot exist in the atmospheres of the stars. |
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interstellar emission lines |
produced at many wave lengths by low-density gas of the interstellar medium |
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21-cm radio line |
an emission line produced when the electron in hydrogen atoms change the direction of their spin and emit radio-wavelength photons. This radiation allows radio astronomers to map the distribution of neutral hydrogen gas in the interstellar medium |
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Composition of interstellar medium |
about 70% hydrogen gas 28% helium 2% is atoms heavier than helium this is approx the same composition as the sun and other stars
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interstellar dust |
makes up roughly 1% of the mass of the interstellar medium. The remaining 99% of the mass is gas |
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molecular clouds |
large, dense clouds of gas and dust; because they are so dense molecules can form inside them |
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giant molecular clouds |
largest o molecular clouds and the sites of star formation. Radio, infrared, and Xray telescopes have detected emission from over 150 molecules in the interstellar medium |
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nebula |
cloud of gas in space and an HII region also known as an emission nebula |
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HII region/ emission nebula |
produced when ultraviolet radiation from hot stars ionizes nearby gas, making it glow. The red, blue, and violet Balmer lines blend together to produce the characteristic pink-red color of ionized hydrogen |
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reflection nebula |
produced by gas and dust illuminated by a star that is hot enough to ionize the gas. Rather, the dust scatters the starlight to produce a reflection of the stellar absorption spectrum |
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Why does the daytime sky look blue |
because shorter wavelength photons scatter more easily than longer wavelength photons reflection nebula look blue |
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dark nebula |
cloud of gas and dust that is noticeable because it blocks the light of distant stars. Irregular shapes reveal the turbulence in interstellar medium |
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evidence that stars have formed recently |
existence of massive hot stars that cannot live very long, such as prominent stars of Orion |
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contraction of molecular clouds |
gravity makes them contract but is resisted by thermal every in the gas, and also by magnetic fields, rotation, and turbulence |
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shocks |
passing shock waves by which some clouds are compressed and star formation is triggered. Birth of massive stars can produce shock waves that trigger further star formation |
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bok globules |
small dark nebulae, some of which may be contracting to form stars |
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free-fall collapse |
when cold gas of interstellar space heats up as it contracts because atoms fall inward and pick up speed. When atoms collide, gravitational energy is converted into thermal energy |
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protostars |
collapsing clouds dense enough to be opaque slow their contraction |
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cocoons |
protostars form deep inside gas and dust cocoons and are not directly visible at visual wavelengths until the cocoons dissipate |
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Orion Nebula |
visible, small part of a much larger dusty molecular cloud. Ionization by ultraviolet photons from the hottest star is ionizing the gas, lighting up the nebula and making it glow brightly |
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infared observations |
reveal clear evidence of active star formation deeper in the molecular cloud just to the northwest of the Trapezium |
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birth line |
line in the H-R diagram where protostars become visible |
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T Tauri stars |
solar-mass objects that have just emerged from their cocoons and are located in the H-R diagram between the birth line and the main sequence |
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Young Stellar Objects |
stars that are nearing the main sequence stage |
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protostellar disks |
surrounds many protostars |
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bipolar flows |
jets of gas emitted along the axis of a spinning protostellar disk |
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Herbig-Haro objects |
nebulae formed where the jets push into the surrounding gas |
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Associations: T associations/ OB associations |
groups of stars born together but not bound to each other by their mutual gravity. The presence of these associations in the area is evidence of recent star formation |
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principle of hydrostatic equilibrium |
says the weight pressing down on a layer of gas in a star must be balanced by the pressure in the gas for the star to be stable. That shows that the inner layers of stars must be hotter because they must support more weight |
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law of energy transport |
states that energy must flow from hot regions such as the core of the sun to relatively cool regions such as the surface of the sun (conduction, radiation, or convection) |
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opacity of a gas |
its resistance to the flow of radiation. Regions where opacity of gas does not permit radiation to carry away enough energy the gas can churn in convection |
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why is convection important in stellar evolution |
it can mix material between inner and outer parts of stars (conduction is less efficient that radiation or convection except in few rare types of stars with very high densities) |
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how do stars make energy |
the same way the sun does, using the proton-proton chain, operates only at temperatures above 4million K needed to overcome the Coulomb barrier of electrical repulsion between positively charged atomic nuclei |
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CNO cycle |
more efficient than proton-proton chain but requires a higher temperature because of the larger repulsion by carbon and other nuclei (both processes combine 4 hydrogen nuclei to make 1 helium nucleus plus energy) |
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pressure-temperature thermostat |
relationship between pressure and temperature, ensures that the star generates just enough energy to support itself |
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stellar models |
astronomers can study the interiors of stars and the way they change overtime by calculating detailed stellar models. (based on 4 previous laws) |
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why can the mass-luminosity relation among main sequence stars not be understood from stellar models |
more massive stars have more weight to support so that makes them more luminous |
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why does the main sequence have a lower end; what objects are seen there |
because stars less massive than .08 solar mass cannot get hot enough to begin hydrogen fusion; brown dwarfs |
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zero-age main sequence (ZAMS) |
where a star is located on the H-R diagram when it first begins fusing hydrogen into helium. As hydrogen is converted to helium the total number of nuclei in the stars core declines, slowly contracting the core, the outer layers expand, moves up and to the right across the band of the main sequence |
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how long can a star remain on the main sequence |
depends on its mass; more massive the faster it uses hydrogen fuel. 25-solar-mass will die in 7 million years, sun expected to last for 10 billion |