Astrophysics Part 2 – Flashcards
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            Kepler's Third Law
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        Square of the period of any planet is proportional to the cube of the semi major axis of its orbit
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            Stellar Parallax
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        Created by orbital position. Max shift is when the earth is at opposite sides of the sun. Once angle found, distance is calculated via trigonometry.
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            Photosphere
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        Coolest part of the sun. Visible surface that emits all visible light.
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            Low mass star
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        < 8 solar masses
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            High mass star
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        > 8 solar masses
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            Low Mass Main sequence
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        Fusion of H begun, low mass spends 99% of lifetime here
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            Red giant
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        Inert He core shrinks down and then the star puffs up.
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            Helium Flash
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        He begins to fuse in red giant due to a temperature rise.
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            Asymptotic red giant
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        Occurs after helium flash. Carbon core.
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            Planetary Nebula
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        Material of star thrown off by winds, leaving a carbon core.
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            White dwarf
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        Dense and degenerate. No more fusion.
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            1.4 Solar Masses
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        White dwarf mass limit
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            Degeneracy pressure
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        When protons, neutrons and electrons are packed in as tightly as possible, exerting a quantum force
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            Nebula
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        Pre-star formation. Interstella medium collapses down.
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            High Mass main sequence
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        Massive and blue
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            Post main sequence high mass star
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        After H core of a high mass star exhausted, core shrinks and heats
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            Red supergiant
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        Hydrogen shell burning causing high mass star to expand
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            Beginning of He fusion in high mass star
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        T ~ 10^8K
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            Blue supergiant
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        Core has expanded after He fusion begins, slowing the fusion rate in a high mass star
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            Second Red giant phase
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        After He core exhausted, core shrinks are C fusion begins in core.
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            Iron core
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        Point at which star is doomed. Reactions from here onwards are endothermic
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            Core collapse supernova
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        Neutrons are packed so tight that they implode releasing heaps of energy.
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            Fusion of heavy elements
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        Type 2 supernovae powers...
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            Type 2 supernova
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        Core collapse supernova
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            Neutron core
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        Left by type 2 supernova
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            Neutron star
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        M < 3 Solar masses. Detected via pulse radiation or binary system.
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            Black hole
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        M > 3 Solar Masses
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            Pulse radiation
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        Use to detect neutron stars using their fast rotation due to conservation of angular momentum.
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            Pulsar
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        Neutron star spinning and releasing radio beams at a constant period
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            Neutron star accretion disk.
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        Sends of x-rays after getting hot due to friction of matter from a binary star being pulled into a neutron star.
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            Neutron degeneracy pressure limit
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        3 solar masses
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            Singularity
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        Single point of mass as neutron star collapses into a black hole
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            Schwarzchild Radius
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        where escape velocity is speed of light
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            Bright x-rays
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        What we look for when detecting black holes.
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            Detatched
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        Binary not transferring mass
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            Semi-attached
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        Binary with one roche lobe filled
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            Contact binary
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        Both roche lobes filled
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            Cataclysmic variable
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        White dwarf accreting off donor star via roche lobe overflow
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            Dwarf nova
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        Sudden large increase in brightness, then returns white dwarf to original state.
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            Direct imaging
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        Used in exceptional circumstances. Needs a large planet with wide separation from parent star.
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            Astrometry
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        Only useful for nearby stars as position shifts are very small and accuracy is important. Measures position of star and looks for wobbles
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            Wobbles small
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        Downside of astrometry
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            Radial velocity
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        Most sensitive to high mass planets close to the star
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            Inclination needed
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        Downside of radial velocity
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            Transit
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        Sensitive to smaller mass planets close to star. Dimming of light tells us about the planet.
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            area of star blocked / area of star
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        Fractional change in flux during transit given by:
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            Gravitational lensing
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        Sensitive to all masses, only large distances. Rare events.
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            Hot jupiter
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        Mostly H and He, close to parent star, larger, short orbital period and low density.
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            Rocky planets
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        More numerous than gas giants.
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            Temperature of planet
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        Flux at surface x cross-sectional area
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            Earth's biosignatures
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        Methane, liquid water and ozone
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            Spectrum of planet's light
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        Where to search for signs of life
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            Terrestrial
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        Small planet, with low mass, rocky and close to star
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            Jovian
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        Large, high mass, icy/gaseous and far out
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            Asteroids
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        Rocky bodies found in asteroid belt
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            Comets
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        Ice and rock, found in Kuiper belt
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            100,000 ly
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        Length of galaxy
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            Galactic bulge
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        Centre of the galaxy
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            Halo
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        Large region of low density around galaxy
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            Disk
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        Thin with spiral arms embedded within
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            Detection of atomic H
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        Atoms have different spins. When they have slightly more energy, they drop an energy state and release a photon
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            Molecular hydrogen
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        Doesn't have strong radiative transitions, hard to detect so we use other molecules to trace it.
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            H2 regions
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        Produced by young stars, looks like red glow. Young stars produce UV light that excites atoms.
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            Interstellar dust
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        Heated to high temperatures via starlight which is absorbed a reemitted in the IR
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            Blue light
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        Dust scatters this more easily
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            Scatters are absorbs
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        What does dust do to light?
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            Interstellar extinction
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        Light gets reddened and dimmed as light passes through a cloud.
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            Reddening
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        The difference in colour we observed to that expected for object, called colour excess
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            observed - intrinsic
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        colour excess given by...
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            Synchrotron Radiation
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        Non-thermal. High energy electrons are accelerated and spiral in magnetic fields causing this.
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            Jets from blackholes and supernova remnants
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        Most common source of synchrotron radiation due to very strong magnetic fields
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            Thermal radia emission
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        Also known as Free-free emission. From free electrons with free protons in a hot ionised gas, where the proton gets accelerated by electron and releases radiation.
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            Signals can't travel faster than the speed of light
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        What tells us that the size of Sgr A can't be more than a light hour in size.
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            Keplerin rotation curve
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        Mass concentrated in centre, with the rotation curve declining as distance increases
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            Observed rotation curve of the milky way
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        Speed stays roughly flat as distance increases after a big jump from zero.
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            Dark matter
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        Why the observed rotation curve for the solar system is mostly flat due to not uniform density.
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            Baryonic dark matter
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        Massive compact halo objects are a type of dark matter. Dead stars and brown dwarfs which are hard to see.
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            Non-baryonic dark matter
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        WIMPS - have mass and do not react in a way giving off radiation.
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            Star ags star cycle
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        Recycles gas from old stars into new stars. Each generation has heavier elements that previous stars. ISM steadily enriched
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            Hot bubbles
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        Ionsied gas. Caused by supernovae. Atomic hydrogen forms as gas cools and then molecular clouds.
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            star formation
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        after the molecular cloud stage in the star-gas-star cycle
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            nuclear fusion/heavy element formation
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        After star formation in star-gas-star cycle
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            Returning gas
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        Supernova and stellar winds do this after the nuclear fusion stage of the star-gas-star cycle
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            spiral arms
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        Where do new stars form in our galaxy?