Constraints on mantle plumes on Venus: Implications for volatile history

Abstract The analysis of Venus’ gravity field and topography suggests the presence of a small number of deep mantle plumes (∼9). This study predicts the number of plumes formed at the core–mantle boundary, their characteristics, and the production of partial melt from adiabatic decompression. Numerical simulations are performed using a 3D spherical code that includes large viscosity variations and internal heating. This study investigates the effect of several parameters including the core–mantle boundary temperature, the amount of internal heating, and the mantle viscosity. The smallest number of plumes is achieved when no internal heating is present. However, scaling Earth’s radiogenic heating to Venus suggests a value of ∼16 TW. Cases with internal heating produce more realistic lid thickness and partial melting, but produce either too many plumes or no plumes if a high mantle temperature precludes the formation of a hot thermal boundary layer. Mantle viscosity must be reduced to at least 10 20  Pa s in order to include significant internal heating and still produce hot plumes. In all cases that predict melting, melting occurs throughout the upper mantle. Only cases with high core temperature (>1700 K) produce dry melting. Over time the upper mantle may have lost significant volatiles. Depending on the water content of the lower mantle, deep plumes may contribute to present-day atmospheric water via volcanic outgassing. Assuming 50 ppm water in mantle, 10 plumes with a buoyancy flux of 500 kg/s continuously erupting for 4 myr will outgas an amount of water on the order of that in the lower atmosphere. A higher level of internal heating than achieved to date, as well as relatively low mantle viscosity, may be required to achieve simulations with ∼10 plumes and a thinner lid. Alternatively, if the mantle is heating up due to the stagnant lid, the effect is equivalent to having lower rates of internal heating. A temperature increase of 110 K/byr is equivalent to −13 TW. This value along with the internal heating of 3 TW used in this study may represent the approximate heat budget of Venus’ mantle.

[1]  E. Engdahl,et al.  Finite-Frequency Tomography Reveals a Variety of Plumes in the Mantle , 2004, Science.

[2]  H. Keppler,et al.  Water Solubility in Aluminous Orthopyroxene and the Origin of Earth's Asthenosphere , 2007, Science.

[3]  A. Galsa,et al.  Quantitative investigation of physical properties of mantle plumes in three-dimensional numerical models , 2007 .

[4]  R. Phillips,et al.  Venusian highlands: Geoid to topography ratios and their implications: Earth and Planetary Science L , 1991 .

[5]  B. Hager,et al.  Geoid anomalies and dynamic topography from convection in cylindrical geometry - Applications to mantle plumes on earth and Venus , 1992 .

[6]  G. Jarvis,et al.  Geometrical effects of curvature in axisymmetric spherical models of mantle convection , 1994 .

[7]  J. Hunen,et al.  New evidence for dislocation creep from 3-D geodynamic modeling of the Pacific upper mantle structure , 2005 .

[8]  H. Keppler,et al.  Water partitioning at 660 km depth and evidence for very low water solubility in magnesium silicate perovskite , 2003 .

[9]  David N. Barnett,et al.  Elastic Thickness Estimates for Venus Using Line of Sight Accelerations from Magellan Cycle 5 , 2000 .

[10]  Sean C. Solomon,et al.  Localization of gravity and topography: constraints on the tectonics and mantle dynamics of Venus , 1997 .

[11]  Frédéric Hourdin,et al.  Superrotation of Venus' atmosphere analyzed with a full general circulation model , 2010 .

[12]  J. Pollack,et al.  H2O-H2SO4 system in Venus' clouds and OCS, CO, and H2SO4 profiles in Venus' troposphere. , 1994, Icarus.

[13]  R. Hékinian,et al.  Carbon and hydrogen isotope constraints on degassing of CO2 and H2O in submarine lavas from the Pitcairn hotspot (South Pacific) , 2006 .

[14]  Louis-Noel Moresi,et al.  Non-Newtonian Stagnant Lid Convection and Magmatic Resur facing on Venus☆ , 1999 .

[15]  A. Davaille,et al.  Transient high-Rayleigh-number thermal convection with large viscosity variations , 1993, Journal of Fluid Mechanics.

[16]  Alexander S. Konopliv,et al.  Venusian k2 tidal Love number from Magellan and PVO tracking data , 1996 .

[17]  G. Choblet Modelling thermal convection with large viscosity gradients in one block of the 'cubed sphere' , 2005 .

[18]  G. Schubert,et al.  Subsolidus convective cooling histories of terrestrial planets , 1979 .

[19]  F. Guyot,et al.  Comparison of carbon, nitrogen and water budgets on Venus and the Earth , 2000 .

[20]  Giuseppe Piccioni,et al.  Venus surface thermal emission at 1 μm in VIRTIS imaging observations: Evidence for variation of crust and mantle differentiation conditions , 2008 .

[21]  T. Spohn,et al.  Water, Life, and Planetary Geodynamical Evolution , 2007 .

[22]  P. C. Hess,et al.  Chemical dieferentiation of a convecting planetary interior: Consequences for a one plate planet such as Venus , 1992 .

[23]  Giuseppe Piccioni,et al.  Surface brightness variations seen by VIRTIS on Venus Express and implications for the evolution of the Lada Terra region, Venus , 2008 .

[24]  T. Kondo,et al.  Water solubility in Mg-perovskites and water storage capacity in the lower mantle , 2003 .

[25]  Greg Hirth,et al.  Water in the oceanic upper mantle: implications for rheology , 1996 .

[26]  G. Davies Dynamic Earth: Plates, Plumes and Mantle Convection , 2000 .

[27]  Louis Moresi,et al.  Mantle convection with a brittle lithosphere: thoughts on the global tectonic styles of the Earth and Venus , 1998 .

[28]  K. Fischer,et al.  A mechanism for low‐extent melts at the lithosphere‐asthenosphere boundary , 2010 .

[29]  C. Sotin,et al.  Three-dimensional thermal convection in an iso-viscous, infinite Prandtl number fluid heated from within and from below: applications to the transfer of heat through planetary mantles , 1999 .

[30]  W. M. Kaula Constraints on Venus Evolution from Radiogenic Argon , 1999 .

[31]  P. Tackley,et al.  Generation of mega‐plumes from the core‐mantle boundary in a compressible mantle with temperature‐dependent viscosity , 1998 .

[32]  Raymond E. Arvidson,et al.  Impact craters and Venus resurfacing history , 1992 .

[33]  F. Nimmo,et al.  VOLCANISM AND TECTONICS ON VENUS , 1998 .

[34]  Shijie Zhong,et al.  Dynamics of thermal plumes in three‐dimensional isoviscous thermal convection , 2005 .

[35]  S. Smrekar,et al.  Origin of Corona-Dominated Topographic Rises on Venus , 1999 .

[36]  Angioletta Coradini,et al.  Scientific goals for the observation of Venus by VIRTIS on ESA/Venus Express mission , 2007 .

[37]  James H. Roberts,et al.  Degree-1 convection in the Martian mantle and the origin of the hemispheric dichotomy , 2006 .

[38]  C. Sotin,et al.  Inversion of two‐dimensional numerical convection experiments for a fluid with a strongly temperature‐dependent viscosity , 2000 .

[39]  J. Arkani‐Hamed Effects of the core cooling on the internal dynamics and thermal evolution of terrestrial planets , 1994 .

[40]  D. Yuen,et al.  Seismic implications of mantle wedge plumes , 2006 .

[41]  M. Doin,et al.  Heat transport in stagnant lid convection with temperature‐ and pressure‐dependent Newtonian or non‐Newtonian rheology , 1999 .

[42]  G. Davies,et al.  Ocean bathymetry and mantle convection: 1. Large‐scale flow and hotspots , 1988 .

[43]  L. Stixrude,et al.  Mineralogy and elasticity of the oceanic upper mantle: Origin of the low‐velocity zone , 2005 .

[44]  B. Hager,et al.  Long-wavelength variations in Earth’s geoid: physical models and dynamical implications , 1989, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[45]  Basaltic Volcanism Study Basaltic volcanism on the terrestrial planets , 1981 .

[46]  B. Hager,et al.  A mantle plume model for the equatorial highlands of Venus , 1991 .

[47]  Patrick Wu,et al.  Rheology of the Upper Mantle: A Synthesis , 1993, Science.

[48]  S. Smrekar,et al.  The interaction of mantle plumes with surface thermal and chemical boundary layers: Applications to hotspots on Venus , 1996 .

[49]  W. Leng,et al.  Controls on plume heat flux and plume excess temperature , 2008 .

[50]  Gary A. Glatzmaier,et al.  Three-dimensional convection of an infinite-Prandtl-number compressible fluid in a basally heated spherical shell , 1992, Journal of Fluid Mechanics.

[51]  V. L. Barsukov,et al.  Venus geology, geochemistry, and geophysics. Research results from the USSR. , 1992 .

[52]  P. Tackley,et al.  Evolution of Helium and Argon Isotopes in a Convecting Mantle: Physics of the Earth and Planetary In , 2004 .

[53]  Louis Moresi,et al.  Scaling of time‐dependent stagnant lid convection: Application to small‐scale convection on Earth and other terrestrial planets , 2000 .

[54]  D. Senske,et al.  Large Topographic Rises on Venus: Implications for Mantle , 1995 .

[55]  H. Bunge,et al.  Convection in a spherical shell heated by an isothermal core and internal sources: Implications for the thermal state of planetary mantles , 2008 .

[56]  Louis Moresi,et al.  Numerical investigation of 2D convection with extremely large viscosity variations , 1995 .

[57]  Olivier Grasset,et al.  Thermal convection in a volumetrically heated, infinite Prandtl number fluid with strongly temperature‐dependent viscosity: Implications for planetary thermal evolution , 1998 .

[58]  Mark A. Bullock,et al.  The Recent Evolution of Climate on Venus , 2001 .

[59]  R. Phillips,et al.  Ejecta correlations with spatial crater density and Venus resurfacing history , 1995 .

[60]  Suzanne E. Smrekar,et al.  Global mapping of crustal and lithospheric thickness on Venus , 2006 .

[61]  V. L. Barsukov Venusian igneous rocks. , 1992 .

[62]  C. Dumoulin,et al.  ŒDIPUS: a new tool to study the dynamics of planetary interiors , 2007 .

[63]  U. Christensen,et al.  The excess temperature of plumes rising from the core‐mantle boundary , 1996 .

[64]  S. Karato,et al.  Water, partial melting and the origin of the seismic low velocity and high attenuation zone in the upper mantle , 1998 .

[65]  Giuseppe Piccioni,et al.  Water vapor abundance near the surface of Venus from Venus Express/VIRTIS observations , 2009 .

[66]  Larry W. Esposito SAGE New Frontiers Mission to Venus , 2011 .

[67]  C. Sotin,et al.  Three-dimensional numerical experiments on thermal convection in a very viscous fluid: Implications for the dynamics of a thermal boundary layer at high Rayleigh number , 2000 .

[68]  Norman H. Sleep,et al.  Hotspots and Mantle Plumes' Some Phenomenology , 1990 .

[69]  P. Drossart,et al.  Recent Hotspot Volcanism on Venus from VIRTIS Emissivity Data , 2010, Science.

[70]  J. P. Dubois,et al.  A warm layer in Venus' cryosphere and high-altitude measurements of HF, HCl, H2O and HDO , 2007, Nature.