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Mars Atmospheric Evolution : What Can Dynamical Models Tell Us?. Stephen W. Bougher Jared M. Bell (University of Michigan). Jane L. Fox (Wright State University). Martian Atmospheric Regions and Escape Processes.
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Mars Atmospheric Evolution :What Can Dynamical Models Tell Us? Stephen W. Bougher Jared M. Bell (University of Michigan) Jane L. Fox (Wright State University)
Summary of Mars Volatile Escape Mechanisms • Thermal (Jean’s) escape : e.g. H • Non-thermal escape: • Photochemical escape : DR of O2+, N2+, CO+… forming energetic (hot) neutrals (O, N, C …). (2) Pick-up ion escape : ions produced in the corona and exosphere are dragged along by solar B-field lines to partially escape in the SW (O+, H+, C+…). (3) Ionospheric outflows: planetary ions are accelerated by the SW convection E-field and partially lost (e.g. O2+). (4) Ion sputtering : a portion of pick-up ions re-impact the neutral atmosphere with enough energy to eject neutral atmospheric particles (e.g. CO2, N2, CO, O, N, C...).
Requirements for Evolution Models of Mars Volatile Escape • Model for the early solar EUV fluxes (Ayres, 1997). ~3 x EUV at ~2.5 GYA. • Model for the history of the solar wind properties (Newkirk, 1981; Wood et al., 2002). • Models for the ancient upper atmosphere neutral densities and temperatures (Zhang et al., 1993; Bougher and Fox, 1996; this work). • An assumed history of the planetary magnetic field; Mars turn-off ~3.7 GYA (Acuna et al., 1998).
MTGCM Input Parameters, Fields, and Domain • Domain : ~70-300 km; 33-levels; 5x5 ° resolution • Major Fields and Species : T, U, V, W, CO2, CO, O, N2 • Minor Species : O2, He, Ar, N(4S) • Ions (PCE) : CO2+, O2+, O+, NO+, CO+, N2+ (<180 km) • Homopause Kzz ~ 1 x 107 cm2/s (at ~125 km) • Prescribed Heating efficiencies : EUV and FUV (22%) • Fast NLTE 15-µm cooling and IR heating schemes from M. Valverde 1-D NLTE code (Spain). • Ko-co2 = 3.0 x 10-12 cm3/s at 300K (Lopez-Puertas et al., 1992). • Simplified ion-neutral chemistry (Fox and Sung, 2001) • Scaled benchmark Ti and Te based upon Viking (Fox).
MGCM-MTGCM Simulation: Coupling Configuration • Separate but coupled NASA Ames MGCM (0-90 km) and NCAR/Michigan MTGCM (70-300 km) codes, linked across an interface at 1.32-microbars on 5x5 ° grid. • Fields passed upward at interface (T, U, V, Z) on 2-min time-step intervals. No downward coupling enabled. • MGCM-MTGCM captures upward propagating migrating and non-migrating tidal oscillations, as well as in-situ driven solar EUV-UV migrating tides.
Current vs. Ancient Model Inputs and Parameters • Both : Ls = 270 (perihelion, S. Summer, TES dust) • Current(today): --F10.7-cm= 130 solar EUV/FUV fluxes --1.0 solar IR fluxes. • Ancient (2.5 GYA) : --F10.7-cm = 390 solar EUV/FUV fluxes (Ayres, 1997) --0.79 current solar IR fluxes (Gough, 1981).
Thermal Structure Exobase Altitude : ~215 km (C) ~250 km (A)
Heat Balances Solid = cond Dash = adia D.Dash = heat 3D.Dash = CO2 Dotted = adv
Neutral Composition Solid = CO2 3D-Dash = O D-Dash = N2 Dash = CO Dotted = Ar
O/CO2 Ratios(Current vs. Ancient) At 135 km: O/CO2 = 1.75% (C) O/CO2 = 3.75% (A)
Electron Densities Ionospheric peak : 1.94 x 105 cm-3 (C) 2.90 x 105 cm-3 (A)
Summary and Conclusions • Enhanced solar EUV-UV fluxes drive a warmer (290 to 430 K) ancient Mars dayside exobase, faster global winds, and a lower thermosphere more abundant in O (1.75 to 3.75% near 135 km). • Dayside (upwelling) winds have a significant impact upon adiabatic cooling, strongly regulating dayside temperatures. Advection of O is enhanced. • A strong dayside thermostat also results from enhanced CO2 cooling, due to more abundant atomic-O. Similar to present day Venus. • Exobase rises (on average) from ~195 to 230 km. Enhanced O and CO2 densities at these heights.