Implications of K, Cu and Zn isotopes for the formation of tektites

1,2,3Yun Jiang,3Heng Chen,3Bruce Fegley Jr.,3Katharina Lodders,4Weibiao Hsu,5Stein B.Jacobsen,3,5KunWang(王昆)
Geochimica et Cosmochimica Acta (in Press) Link to Article [https://doi.org/10.1016/j.gca.2019.06.003]
1CAS Key Laboratory of Planetary Sciences, Purple Mountain Observatory, Chinese Academy of Sciences, Nanjing 210008, China
2CAS Center for Excellence in Comparative Planetology, China
3Department of Earth and Planetary Sciences and McDonnell Center for the Space Sciences, Washington University in St. Louis, One Brookings Drive, St. Louis, MO 63130, USA
4Space Science Institute, Macau University of Science and Technology, Macau
5Department of Earth and Planetary Sciences, Harvard University, 20 Oxford Street, Cambridge, MA 02138, USA
Copyright Elsevier

Tektites are mm to cm sized glassy objects generated through high-energy meteoroid impacts on the surface of the Earth under high temperature and pressure, and reducing conditions. They are the products of large-scale catastrophic events in Earth’s history and can be used to understand the behavior of moderately volatile elements (e.g., K and Zn) during impact vaporization events. Here, we report bulk K isotopic compositions of tektites from three different strewn fields and “in-situ” profile analysis of both K and Zn isotopes in one complete tektite. All tektites span a narrow range in their K isotopic compositions (δ41KBSE: −0.10 ± 0.03‰ to 0.16 ± 0.04‰), revealing no discernible K isotopic fractionation from the Bulk Silicate Earth (BSE) and upper continental crust materials, which is consistent with previous results. In contrast, Zn isotopes show a large variation (δ66Zn: −0.39 ± 0.02‰ to 2.38 ± 0.03‰) even within one specimen. In order to provide a coherent explanation for the different behavior of moderately volatile elements (K, Zn and Cu), we have conducted thermochemical calculations to compute the partial vapor pressures of Cu2O, K2O, and ZnO dissolved in silicate melts as a function of temperature, pressure, oxygen and chlorine fugacities. In a large range of the parameter space, the calculations show that Cu and Zn can be vaporized much easier than K and thus produce large isotopic fractionation. In contrast, the lithophile element K is more prone to remain in the silicate melt because of its very low activity coefficient in the melt, and thus the K isotopes remain unfractionated. This study provides new constraints on the formation of tektites and is consistent with a “bubble-stripping” model to explain the extreme water and volatiles depletion in tektites.

Effects of pH2O, pH2 and fO2 on the diffusion of h-bearing species in lunar basaltic liquid and an iron-free basaltic analog at 1 atm

1,2,3M.E.Newcombe, 1J.R.Beckett,1M.B.Baker, 4S.Newman,1Y.Guan,1J.M.Eiler1E.M.Stolper
Geochmica et Cosmochimica Acta (in Press) Link to Article [https://doi.org/10.1016/j.gca.2019.05.033]
1Division of Geological and Planetary Sciences, California Institute of Technology, Pasadena, CA 91125, USA
2Lamont Doherty Earth Observatory, 61 Route 9W, Palisades, NY 10964, USA
3Department of Terrestrial Magnetism, Carnegie Institution of Washington, 5241 Broad Branch Road NW, Washington, DC 20015
4Bay Area Air Quality District, 375 Beale St., Suite 600, San Francisco, CA 94105
Copyright Elsevier

We have experimentally determined the diffusivity of water in a representative lunar basaltic liquid composition (LG) and in an iron-free analog of a basaltic liquid (AD) at the low water concentrations and low oxygen fugacities (fO2) relevant to the eruption of lunar basalts. Experiments were conducted at 1 atm and 1350 °C over a range of pH2/pH2O from near zero to ∼10 and a range in fO2 spanning ∼9 orders of magnitude (from 2.2 log units below the iron-wüstite buffer, IW–2.2, to IW+6.7). The water concentrations measured in our quenched experimental glasses by secondary ion mass spectrometry (SIMS) and Fourier transform infrared spectroscopy (FTIR) vary from a few ppm to ∼430 ppm. Water concentration gradients in the majority of our AD experiments are well described by models in which the diffusivity of water (Dwater∗ ) has a constant value of ∼2×10–10 m2/s, while our LG results indicate that Dwater∗ in LG melt has a constant value of ∼6×10–10 m2/s under the conditions of our experiments. Water concentration gradients in hydration and dehydration experiments that were run simultaneously in H2/CO2 gas mixtures are well described by the same Dwater∗ , and water concentrations measured near the melt-vapor interfaces of these experiment pairs are approximately the same. These observations strongly support an equilibrium boundary condition for our experiments containing >70 ppm H2O. However, dehydration experiments into nominally anhydrous CO2, N2, and CO/CO2 gas mixtures leave some scope for the importance of kinetics during dehydration of melts containing less than a few 10’s of ppm H2O. Comparison of our results with the modified speciation model (Ni et al., 2013) in which both molecular water and hydroxyl are allowed to diffuse suggests that we have resolved the diffusivity of hydroxyl (DOH ) in AD and LG melts. Our results support a positive correlation between DOH and melt depolymerization. Best-fit values of Dwater∗ for our LG experiments vary within a factor of ∼2 over a range of pH2/pH2O from 0.007 to 9.7 and a range of logfO2 from IW–2.2 to IW+4.9. The relative insensitivity of our best-fit values of Dwater∗ to variations in pH2 suggests that H2 diffusion did not control the rate of degassing of H-bearing species from the lunar glasses of Saal et al. (2008); however, we cannot rule out a role for molecular H2 diffusion under lower-temperature and/or higher-pressure conditions than explored in our experiments. The value of Dwater∗ chosen by Saal et al. (2008) for modeling the diffusive degassing of the lunar volcanic glasses is within a factor of ∼2 of our measured value in LG melt at 1350 °C. By coupling our LG results at 1350 °C with an activation energy of 220 kJ/mol (Zhang et al. 2017), we obtain the following Arrhenius relationship, which can be used to model syneruptive diffusive water loss from lunar melt beads:

Dwater∗(m2/s)=7.2×10-3exp-2.6×104T(K) .

Indigenous Organic-Oxidized Fluid Interactions in the Tissint Mars Meteorite

1,2Jaramillo, E.A.,3Royle, S.H.,4,5Claire, M.W.,1,3Kounaves, S.P.,3Sephton, M.A.
Geophysical Research Letters 46, 3090-3098 Link to Article [DOI: 10.1029/2018GL081335]
1Department of Chemistry, Tufts University, Medford, MA, United States
2Jet Propulsion Laboratory, California Institute of Technology, Pasadena, CA, United States
3Department of Earth Science and Engineering, Imperial College London, London, United Kingdom
4School of Earth and Environmental Sciences and Centre for Exoplanet Science, University of St. Andrews, Saint Andrews, United Kingdom
5Blue Marble Space Institute of Science, Seattle, WA, United States

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An extremely heavy chlorine reservoir in the Moon: Insights from the apatite in lunar meteorites

1,2,3Wang, Y.,2,3Hsu, W.,4Guan, Y.
Scientific Reports 9, 5727 Link to Article [DOI: 10.1038/s41598-019-42224-8]
1Key Laboratory of Planetary Sciences, Purple Mountain Observatory, Chinese Academy of Sciences, Nanjing, 210034, China
2The State Key Laboratory of Lunar and Planetary Science/Space Science Institute, Macau University of Science and Technology, Taipa, China
3CAS Center for Excellence in Comparative Planetology, Purple Mountain Observatory, Nanjing, 210034, China
4Division of Geological and Planetary Sciences, California Institute of Technology, Pasadena, CA 91125, United States

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Application of instrumental methods in the Morasko Meteorite investigations [Zastosowanie metod instrumentalnych w badaniach meteorytu Morasko]

1Duczmal-Czernikiewicz, A.,1Muszynski, A.,2Runka, T.,3Golebiewska, B.,1Michalska, D.,
4Karwowski, L.
Przeglad Geologiczny 67, 156-158 Link to Article [DOI: 10.7306/2019.6]
1Instytut Geologii, Uniwersytet Im. Adama Mickiewicza W Poznaniu, ul.Bogumila Krygowskiego 12, Poznan, 61-680, Poland
2Instytut Badan Matcrialowych I Inzynierii Kwantowcj, Politechnika Poznanska, ul. Piotrowo 2, Poznan, 61-138, Poland
3AGH Akademia Gorniczo-Hutnicza, Katedra Mineralogii, Geochemii Petrografii i Geochemii, al. Mickiewicza 30, Krakow, 30-059, Poland
4Uniwersytet and Slaski, Katedra Geochemii, Mineralogii i Petrografii, ul. Bqdzinska 60, Sosnowiec, 41-205, Poland

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Titanium local coordination environments in Cretaceous–Paleogene and Devonian–Carboniferous boundary sediments as a possible marker for large meteorite impact

1,2,3Tobase, T.,1Yoshiasa, A.,1Komatsu, T.,1Maekawa, T.,1Hongu, H.,4Okube, M.,4Arima, H.,4Sugiyama, K.
Physics and Chemistry of Minerals (in Press) Link to Article [DOI: 10.1007/s00269-019-01030-4]
1Graduate School of Science and Technology, Kumamoto University, Kumamoto, 860-8555, Japan
2Université de Lorraine, CRM2, UMR 7036, Vandoeuvre-les-Nancy, 54506, France
3CNRS, CRM2, UMR 7036, Vandoeuvre-les-Nancy, 54506, France
4Institute for Materials Research, Tohoku University, Sendai, 980-8577, Japan

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Multiple Outbursts of Asteroid (6478) Gault*

Quanzhi Ye (叶泉志)1,2 et al. (>10)
Astrophysical Journal Letters 874, L16 Link to Article [DOI: 10.3847/2041-8213/ab0f3c]
1Division of Physics, Mathematics and Astronomy, California Institute of Technology, Pasadena, CA 91125, USA
2Infrared Processing and Analysis Center, California Institute of Technology, Pasadena, CA 91125, USA

Main-belt asteroid (6478) Gault unexpectedly sprouted two tails in late 2018 and early 2019, identifying it as a new active asteroid. Here we present observations obtained by the 1.2 m Zwicky Transient Facility survey telescope that provide detailed time-series coverage of the onset and evolution of Gault’s activity. Gault exhibited two brightening events, with the first one starting on 2018 October 18 ± 5 days and a second one starting on 2018 December 24 ± 1 days. The amounts of mass released are 2 × 107 kg and 1 × 106 kg, respectively. Based on photometric measurements, each event persisted for about a month. Gault’s color has not changed appreciably over time, with a pre-outburst color of g PS1 − r PS1 = 0.50 ± 0.04 and g PS1 − r PS1 = 0.46 ± 0.04 during the two outbursts. Simulations of dust dynamics shows that the ejecta consists of dust grains of up to 10 μm in size that are ejected at low velocities below $1\,{\rm{m}}\,{{\rm{s}}}^{-1}$ regardless of particle sizes. This is consistent with non-sublimation-driven ejection events. The size distribution of the dust exhibits a broken power law, with particles at 10–20 μm following a power law of −2.5 to −3.0, while larger particles follow a steeper slope of −4.0. The derived properties can be explained by either rotational excitation of the nucleus or a merger of a near-contact binary, with the latter scenario to be statistically more likely.

The Sporadic Activity of (6478) Gault: A YORP-driven Event?

Jan T. Kleyna1 et al. (>10)
Astrophysical Journal Letters 874, L20 Link to Article [DOI: 10.3847/2041-8213/ab0f40]
1Institute for Astronomy, University of Hawaii, 2680 Woodlawn Drive, Honolulu, HI 96822, USA

On 2019 January 5 a streamer associated with the 4–10 km main belt asteroid (6478) Gault was detected by the ATLAS sky survey, a rare discovery of activity around a main belt asteroid. Archival data from ATLAS and Pan-STARRS1 show the trail in early 2018 December, but not between 2010 and 2018 January. The feature has significantly changed over one month, perfectly matching predictions of pure dust dynamical evolution and changes in the observing geometry for a short release of dust around 2018 October 28. Follow-up observations with the Hubble Space Telescope(HST) show a second narrow trail corresponding to a brief release of dust on 2018 December 30. Both releases occurred with negligible velocity. We find the dust grains to be fairly large, with power-law size distributions in the 10−5−10−3 m range and power-law indices of ~−1.5. Three runs of ground-based data find a signature of ~2 hr rotation, close to the rotational limit, suggesting that the activity is the result of landslides or reconfigurations after Yarkovsky–O’Keefe–Radzievskii–Paddack (YORP) spin-up.

Earth’s volatile element depletion pattern inherited from a carbonaceous chondrite-like source

1,2Ninja Braukmüller,1,2Frank Wombacher,1,2Claudia Funk,1,2Carsten Münker
Nature Geoscience (in Press) Link to Article [https://doi.org/10.1038/s41561-019-0375-x]
1Institut für Geologie und Mineralogie, Universität zu Köln, Köln, Germany
2Steinmann Institut für Geologie, Mineralogie und Paläontologie, Universität Bonn, Poppelsdorfer Schloss, Bonn, Germany

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Episodically Active Asteroid 6478 Gault

David Jewitt1,2, Yoonyoung Kim3, Jane Luu4, Jayadev Rajagopal5, Ralf Kotulla6, Susan Ridgway5, and Wilson Liu5
Astrophysical Journal Letters 876, L19 Link to Article [DOI: 10.3847/2041-8213/ab1be8]
1Department of Earth, Planetary and Space Sciences, UCLA, 595 Charles Young Drive East, Los Angeles, CA 90095-1567, USA
2Dept. of Physics and Astronomy, UCLA, 430 Portola Plaza, Box 951547, Los Angeles, CA 90095-1547, USA
3Max Planck Institute for Solar System Research, Justus-von-Liebig-Weg 3, D-37077 Göttingen, Germany
4Department of Physics and Technology, Arctic University of Tromso, Tromso, Norway
5NOAO, 950 North Cherry Avenue, Tucson, AZ 85719, USA
6Department of Astronomy, University of Wisconsin-Madison, 475 N. Charter St., Madison, WI 53706, USA

We present imaging and spectroscopic observations of 6478 Gault, a ~6 km diameter inner main-belt asteroid currently exhibiting strong, comet-like characteristics. Three distinct tails indicate that ultra-slow dust (ejection speed 0.15 ± 0.05 m s−1) was emitted from Gault in separate episodes beginning UT 2018 October 28 ± 5 (Tail A), UT 2018 December 31 ± 5 (Tail B), and UT 2019 February 10 ± 7 (Tail C), with durations of ΔT ~ 10–20 days. With a mean particle radius $\overline{a}\,\sim $ 200 μm, the estimated masses of the tails are M A  ~ 4 × 107 kg, M B  ~ 6 × 106 kg, and M C  ~ 6 × 105 kg, respectively, and the mass-loss rates from the nucleus are 20–40 kg s−1 for Tail A, 4–6 kg s−1 for Tail B, and ~0.4 kg s−1for Tail C. In its optical colors Gault is more similar to C-type asteroids than to S-types, even though the latter are numerically dominant in the inner asteroid belt. A spectroscopic upper limit to the production of gas is set at 1 kg s−1. Discrete emission in three protracted episodes effectively rules out an impact origin for the observed activity. Sublimation driven activity is unlikely given the inner-belt orbit and the absence of detectable gas. In any case, sublimation would not easily account for the observed multiple ejections. The closest similarity is between Gault and active asteroid 311P/(2013 P5), an object showing repeated but aperiodic ejections of dust over a 9 month period. While Gault is 10 times larger than 311P/(2013 P5), and the relevant timescale for spin-up by radiation torques is ~100 times longer, its properties are likewise most consistent with episodic emission from a body rotating near breakup.