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ASTRONOMY 340 FALL 2007 27 September 2007 Class #8
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90 minutes of homework (for 6 th graders, but you can extrapolate to college…) 15 minutes looking for assignment 11 mins calling a friend for the assignment 23 mins explaining to parents why the teacher is mean and just doesn’t like children 8 mins in the bathroom 10 mins getting a snack 7 mins checking the TV guide 6 mins telling parents that the teacher never explained the homework 10 mins sitting at the kitchen table waiting for Mom to do the assignment
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Review CO molecule – Rayleigh-Jeans approximation substitute temperature for intensity in radiative transfer eqn. T b = ( λ 2 /2k)B λ T b (s) = T b (0)e - τ (s) +T(1-e - τ (s) ) Planetary Surfaces Processes at work: impact, weathering, atmosphere, geology (tectonics/volcanic Mercury: heavily cratered, no tectonics Venus: global resurfacing 300 Myr ago, no tectonics Mars: water, older volcanoes Earth: tectonics, water, weather
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Review Surface composition of terrestrial planets dominated by silicates SiO 2 (quartz), olivines, feldspars, etc. Tectonics – important on the Earth Sea-floor spreading, subduction zones, earthquakes, mountain chains, volcanic activity
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Geochronology Consider: at t=0, N=N 0 t=τ, N τ = N 0 – D τ, where D τ is the number of “daughter” atoms after time, τ. So, N 0 – D τ = N 0 exp(-λτ) τ = (1/λ)ln[1+(D τ /N τ )] (D τ /N τ ) can be easily measured. This is great as long as D only arises from radioactive decay of N.
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Volcanic Activity Key ingredient molten material Accretion (primordial heat) Impact triggered Tidal heating/stretching Radioactive decay
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Lunar Mare Lunar mare – resurfacing via some Impact that releases magma. Note low crater density.
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Volcanic Activity Key ingredient molten material Accretion (primordial heat) Impact triggered Tidal heating/stretching Radioactive decay ρ (magma)< ρ (rock) magma rises through “plumes” volcanoes sit atop plumes same physics on any planet/moon Magma acts to resurface Volcanic composition H 2 O, CO 2, SO 2 (recall that Io has SO 2 or S 2 gas)
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Olympus Mons Viking 1
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Venus’ Tectonic Activity? Smrekar & Stefan 1997 Science 277, 1289 Venus’ past Crater distribution is even & young no resurfacing over past 300-500 Myr (Price & Supper 1994 Nature 372 756) No global ridge system and a lack of significant upwellings (Solomon et al. Science 252 297) Why such a big difference compared with Earth? Catastrophic loss of H 2 O from mantle? no convection “coronae” are unique to Venus rising plumes of magma exert pressure on lithosphere less dense lithosphere deforms under pressure deformation of crust without tectonics
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Coronae on Venus – from Magellan radar imaging
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Martian Tectonic Activity Connerney et al ’99 Science 284 794 Mars Global Surveyor Detected E-W linear magnetization in southern highlands “quasi-parallel linear features with alternating polarity” Note: Earth’s global B-field is so much stronger it makes crustal sources hard to detect
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Martian Tectonic Activity Connerney et al ’99 Science 284 794 Mars Global Surveyor Detected E-W linear magnetization in southern highlands “quasi-parallel linear features with alternating polarity” Note: Earth’s global B-field is so much stronger it makes crustal sources hard to detect Mars has no global field so crustal field must be remnant (“frozen in time”) from crystallization
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Martian Crustal Magnetization Working model Collection of strips 200 km wide, 30 km deep Variation in polarization every few 100 km 3-5 reversals every 10 6 years (like seafloor spreading on Earth) Some evidence for plate tectonics…but crust is rigid Earth’s crust appears to be the only one that participates in convection
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Impacts and Cratering Dominates surface properties of most rocky bodies “Back of the envelope” calculation of the energy of an impact…
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Formation of Impact Craters Impactor unperturbed by atmosphere Impact velocity ~ escape velocity (11 km s -1 ) tens of meters in diameter Impact velocity > speed of sound in rocks impact forms a shock Pressures ~100 times stress levels of rock impact vaporizes rocks Shock velocity ~10 km s -1 much faster than local sound speed so shock imparts kinetic energy into vaporized rock
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Contact/Compression Projectile stops 1-2 diameters into surface kinetic energy goes into shock wave tremendous pressures P ~ (1/2) ρ 0 v 2 Peak shock pressures ~1000 kbar; pressure of vaporization ~600 kbar Shock loses energy Radial dilution (1/r 2 ) Heating/deformation of surface layer Velocity drops to local sound speed – seismic wave transmitted through surface Can get melting at impact point Shock wave reflected back through projectile and it also gets vaporized Total time ~ few seconds
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Excavation Shock wave imparts kinetic energy into vaporized debris excavation of both projectile and impact zone (defined as radius at which shock velocty ~ sound speed (meters per second) Timescale is just a dynamical/crossing time (t = (D/g) 1/2 Crater size? D goes as E 1/3 empirically, it looks like ~ 10 time diameter of projectile (but see equation 5.26b). Can get secondary craters from debris blown out by initial impact Large impacts multiring basins (Mars, Mercury, Moon)
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Craters 35m2m4yrSmall Earthquake 1km50m1600yrBarringer Meteor Crater 7km350m51,000yr9.6 mag earthquake 10km500m10 5 yrSweden 200km10km150 MyrLargest craters/KT impactor
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Crater Density See Figure 5.31 in your book number of craters km -2 vs diameter Saturation equilibrium – so many craters you just can’t tell…. Much of the lunar surface Almost all of Mercury Only Martian uplands Venus, Earth not even close note cut-off on Venus’ distribution Calibrate with lunar surface rocks 10 7 times more small craters (100m) as there are large craters (500-1000 km)
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Mercury South Pole
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Lavinia Planum Impact Craters Note ejecta surrounding crater
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“It’s the size of Texas, Mr. President” - from yet another bad movie Comets – small,rocky/icy things 10s of km Asteroids – small, rocky things a few to 10s of km the largest is the size of Texas (1000 km) 100-300 NEAs known Close encounters…. Tunguska River in Siberia 30-50m meteroid exploded above ground flattened huge swath of forest
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You make the catastrophe… Need high velocity max velocity ~ 70 km s -1 (combine Earth’s orbital velocity plus solar system escape velocity) Earth-asteroid encounters 25 km s -1 Eart-comet encounters 60 km s -1 Make it big…. E ~ mv 2 something 1000 km would wipe out the entire western hemisphere, but let’s be realistic and go for ~10m (10 21 J) or ~1 km (10 23 J) One impact imparts more energy in a few seconds than the Earth releases in a year via volcanism etc.
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