Comparison of the HDO cycle in the LMD Mars GCM with ACS/TGO observations

Abstract

<p>HDO and the D/H ratio are important in order to understand Mars past and present climate, in particular regarding the evolution through ages of the Martian water cycle.&#160;</p>\n<p>We present simulations of the HDO cycle with the LMD Mars GCM and compare the retrieved cycle with observations provided by the Atmospheric Chemistry Suite (ACS) on board the ESA/Roscosmos Trace Gas Orbiter (TGO).&#160;&#160;</p>\n<p>This work is a companion study of Vals et al. presented in session TP12, which presents the evolutions of the model since Rossi et al, (2021), and explores the behaviour of the D/H ratio cycle when taking into account the microphysics and radiative effect of clouds, as well as the effect of kinetics on fractionation during condensation.&#160;</p>\n<p><strong>Introduction</strong></p>\n<p>Mars is known to have had a significant liquid water reservoir on the surface and the D/H ratio derived from the HDO/H₂O abundance ratio is a sensitive tool to constrain the primordial abundance of the water reservoir on Mars and its evolution with time. The current ratio is at least five times that of the Vienna Standard Mean Ocean Water (SMOW) (Owen et al. 1988 , Encrenaz et al. 2018, Krasnopolsky 2015, Villanueva et al. 2015).&#160;</p>\n<p>H and D atoms in the upper atmosphere come from H2O and HDO, their sole precursor in the lower atmosphere. The lower mass of H over D atoms and the fact that H₂O is preferentially photolysed over HDO (Cheng et al. 1999) explain the differential escape of these two elements. Also, the heavier isotope, HDO, has a lower vapor pressure than H₂O, which results in an enrichment of the deuterated isotope in the solid phase of water. This effect is known as the Vapor Pressure Isotope Effect (VPIE) and can reduce the D/H ratio above the condensation level to values as low as 10% of the D/H ratio near the surface (Bertaux et al. 2001, Fouchet et al. 2000).&#160; Fractionation should affect the amount of HDO depending on latitude, longitude, altitude and season (Montmessin et al. 2005, Rossi et al. 2021).&#160;</p>\n<p><strong>Modeling HDO</strong></p>\n<p>We present here the results from our (re)integration of the HDO cycle into the LMD Mars GCM, taking into account HDO in its vapour and ice phases in the atmosphere, and as surface ice. In Rossi et al. (2021), we presented first results with a dust annual scenario mimicking the dust seasonal and spatial evolution observed during Martian Year 34 (MY34) and including the occurrence of the Global Dust Storm (GDS).</p>\n<p>The simulations illustrated the effect of the dust on the temperature field, and therefore on the circulation and the cloud formation. Since clouds are forming at higher altitude (if at all), the deuterium is less constrained vertically and can extend to higher altitudes. A similar effect being observed for water vapour (Fedorova et al., 2020).</p>\n<p>In Rossi et al. (2021) we used a simplified cloud formation scheme, without condensation nuclei, and didn t include the radiative effect of clouds.</p>\n<p><img src= data:image/png;base64, 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