Origin of Earth s s Oceans. Karen Meech, Session #29 Tues 1/18/05
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1 Origin of Earth s s Oceans Karen Meech, Session #29 Tues 1/18/05
2 D/H Units Translation Absolute abundances harder to measure Measure relative to a standard S.M.O.W. for D/H = x 10-6 Definition δ = D/H sample D/H D/H SMOW Example: D/H SMOW LL3 meteorites: D/H = x 10-6 δd SMOW = -512 oo /o to oo /o X 1000 per mil
3 Most impt debate / controversy in SS form Oceans are enriched in Deuterium Comets brought some (10-30%) Isotopic Tracers D/H Earth ~ 16 x10-5 Solar System ~ 2.5x10-5 Comets ~ 30 x10-5 Origin of Earth s Water
4 Iceland Hawaii The D/H ratio in comets is not well established The reference to Earth is SMOW how does this relate to the primordial water?
5 D/H Issues Original D/H set in big bang Formation of molecules in cold clouds Isotopic enrichment in cold interstellar clouds Ion-Molecule reactions Planetesimal formation fractionation Comet formation scenarios Planetesimal delivery to Earth Sources of Water D/H comet measurements Fractionation processes on Earth...? Deep Mantle Water? Measurements & Instrumentation
6 The Interstellar Medium Element Formation H, He form in big bang Heavier elements dust processed inside stars Cold clouds hot cores T ~ K n ~ 3 x 10 4 cm cm -3 Grains sites of molecule formation Collisions sticking Mobility of D and H is key
7 D/H Measurements in Diffuse ISM Lyman α absorption toward several stars Local value D/H avg ~ 1.6 x 10-5 Range: x 10-5 [δd = oo /o] Protosolar Value D/H = 2.5 x 10-5 [δd = -839 oo /o] D/H at time of SS form 3 He/ 4 He in solar wind + D 3 He models Giant planets + models
8 C 2 H 6 CH 3 CHO CH 3 COOH CO CO 2 CH 4 C 2 H 3 COCH 3 HCOOH H 2 O CH 3 OH H 2 S C 2 H 2 C 2 H 5 OH H 2 CO NH 3 C 2 H 4 Many molecules Chemical models Can t t decouple simple molecules ISM D/H Fractionation Ion Molecule Reactions Gas phase reactions D & H slight mass difference Closer E levels D favored in kinetics 1322 reactions / 107 species Energy levels not known for polyatomic molecules Reaction rates strongly T dependent time dependent
9 D Enrichment Primary Gas Phase Deuterium Reactions Certain reverse reactions in isotopic exchange are strongly inhibited at low T Results in preference for formation of certain deuterated species Rate coefficients, k cm 3 s -1 Reaction H HD H 2 D + + H 2 H 2 D + + H 2 H HD Gas-Grain Reactions 10K 1.7(-09) 3.6(-18) 30K 1.5(-09) 8.8(-12) 50K 1.5(-09) 9.3(-11) 70K 1.4(-09) 2.0(-10) Through accretion, D-molecules not destroyed as fast This leads to large deuterated molecule enhancement
10 ISM Core Measurements W33a D/H ~ (40-150) x 10-5 [δd= oo /o] Hot cores E barriers inhibiting reverse reactions overcome Accretion/surface chemistry Evaporation of grain mantles Preserved for ~ 10 4 yr Deuteration much stronger in low mass stars Orders of magnitude higher
11 Planetesimal formation Collapse of interstellar cloud Center collapses faster flattened disk Grain infall passes shock front sublimation, recondense Turbulent mixing of gas / solids radial transport Eventual gravitational clumping planet building Comets: how much ISM material is preserved is the diff between SP and LP comets important for D/H?
12 Comets: Archaeological Remnants Kuiper Belt & Oort Cloud reservoir Perturbations close to sun Activity develops Km-scale nucleus Coma ~ 10 5 km Tail ~ km
13 ISM Alteration in Nebula? Re-equilibration of D/H Need heat k(t) ) drops 5 orders mag from T= K Need reservoir of Hydrogen gas No isotopic exchange between gas / solids Radial mixing of gas Reset D/H only in warm inner nebula How far out did turbulence extend?
14 Evidence for Radial Mixing Chemical heterogeneities H 2 CO in 1P/Halley Crystalline silicates Requires high T (> 800K) KBO dynamics planet migration
15 Comet Isotopic Measurements GHz High dry site: Mauna Kea Relate line strength to amt Excitation models Collisional excitation & LTE Fluorescence balance between excitation & vibrational-rotation decay Measure gas temperature Measure Q H2 O separately IR ro-vibrational bands UV (IUE) OH + models Ground narrow band OH Lyman α (SOHO) + models
16 D/H in Comets Comet Halley Halley Hyakutake Hale Bopp Tempel 1 Wirtanen Ion mass spec Neutral mass spec Sub-mm Sub-mm Sub-mm Method Rosetta in situ Value x / / / /- 8 TBD TBD All measured so far are from Oort cloud Prediction: KBO more enriched (less mixing in nebula) Sub-mm measurements very indirect
17 D/H Preserved During Sublimation? Sublimation of HDO and H 2 O from separate fronts Nucleus is porous Vapor pressures are equal (lab meas) ρ HDO < ρ H2 O HDO front moves inward faster HDO flux decreases faster Steady state eventually reached D/H meas = D/H nucleus Far from steady state D/H can be a factor of 2 high Steady state near q, different if far from q
18 Meteorite D/H Measurements Meteorites Water-rich minerals in some Form within 1-2 Myr of SS form Evidence for heating & aqueous alteration D/H Measurements Chondrules in LL3 D-rich meteorites: (7-45) x 10-5 [δd = oo Earth /o] Chondrites (12-30) x 10-5 [δd = oo /o] D/H x 10-5
19 Mars SNC Meteorites Atmospheric water: D/H = 81 x 10-5 (δd=+4200 oo /o) May be enriched because of preferential H atm escape Jeans Escape High E tail of Maxwell v distn escapes Mars D/H fractionation Loss of 2.7x10 8 cm -2 s -1 on Earth, small compared to reservoir Loss on Mars of 2.4x10 8 cm -2 s -1 Reservoir unknown Log of water in Mars crust today (H 1 ) versus early Mars, (H o ) for D/H ratios wrt SMOW of 2.6 & 5.2
20 Dynamical Delivery of Meteoritic Material Dynamical models (Morbidelli( Morbidelli) delivery in few impacts (small number statistics) Secular resonances & planet migration + gas drag: delivers H 2 O-rich asteroids to Earth Models show only 2-20% of cometary bodies were delivered to Earth Problem with Nobel gas abundances Earth has too much Ne to come from asteroids, but maybe not comets
21 Summary of D/H Measurements SMOW Comets Source Diffuse ISM Protosolar Nebula Meteorites Molecular clouds / hot cores [δd oo oo /o] > D/H x x x x x 10-5 > x 10-5
22 Status of D/H Measurements?? We don t t really know comet D/H for more than one type Meteorite measurements have wide range Dynamics of delivery? Nobel gas abundances? Does SMOW represent the primordial water on Earth?
23 Earth s s Juvenile Water? Are there sources of Deep Mantle primordial water? What are fractionation processes on Earth for D/H? Lack of re-equilibration: no source of H How to assess contamination in mantle water measurements? If water is delivered during impact is the D/H reset?
24 How to Access Primordial Water? Glacier & Geothermal systems Gas phase measurements? Take Advantage of drilling High T rock phases surviving transport Olivine, pyroxene, diamond 3 He/ 4 He in phenocrysts Xenoliths: δd = -40 to -95 oo oo /o
25 Fractionation Processes on Earth Evaporation / condense Light molecules enriched in vapor phase Kinetic effects Rate of chemical reaction related to mass Diffusion Light isotopes more mobile Pressure Hydrous minerals D/H fractionation Chemical composition Nature of chemical bonds high vibration f prefer heavier isotopes Crystal structure Heavy isotopes concentrate in more closely packed structures MORB water Homogeneous wrt % water Remixed into source or uniform degassing Hot spots and xenoliths significant hydration in mantle Upper mantle *may* contain primordial H 2 O Hydrosphere UV photochemistry Impact degassing subduction
26 Deep Drilling Projects HSDP Hilo 4 km (ongoing) Isotopic data vs time: plume geochemistry IDDP Iceland 5 km (start 11/04) Extraction of Energy & chemicals o C Instruments Small down-hole mass spec Boreholes 4 4 diam
27 Hawaii Scientific Drilling Project Continuous samples from MKO flows Learn how mantle plumes originate & magma to surface Drill from ,000 yr (20,000 ft) Zoned plume Core from deep mantle
28 Iceland Deep Drilling Project Plan (economic) Depth of geothermal resources 5 km well in Rekjanes peninsula (2007-8) 3 wells, 15 yr Krepla Problems for primordial water search Rocks are very permeable Fluid origins seawater? Water-rock exchange? Permeability at depth unknown Suggested tactics Gas inclusions in phenocrists Sampling new volcanic plumes Gas samples disappear quickly
29 Grimsvotn Eruption Nov 2004
30 Does a Habitable World Require an Asteroid Belt? Implications for terrestrial planet H 2 O in other SS require an asteroid belt? Oort cloud?
31 Discussion Nordic Ctr for Volcanology: Karl Gronvold, Niels Oskarsson Look for D/H in high T phases H released from deep sources from breakdown of hydrides Interaction with C CH 4 At high T (1500K) no fractionation Gases trapped in inclusion in spinels, olivines,, diamonds Measurements H with ion beams (SIMS) H measurement tricky (need clean system) D very challenging 3 He/ 4 He anomalies in Iceland and Hawaii Questions Timescale for planetary chemical fractionation & core formation?
32 Discussion Nordic Ctr for Volcanology: Karl Gronvold, Niels Oskarsson Surtsey gas analysis Rare gas work Probably recycled seawater Helium work Primordial He high in NW & central Iceland Geothermal water Isotopic work Iceland Mostly meteoric Except Reykjanes peninsula (δd=-20%)( Rocks very permeable
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