Abstract:Response of the Martian upper thermosphere to the lower atmospheric dust activity is studied using unique observations made together by the Mars Orbiter Mission (MOM) and the Mars Atmosphere and Volatile Evolution (MAVEN) spacecraft. The Mars Exospheric Neutral Composition Analyzer (MENCA)/MOM and the Neutral Gas and Ion Mass Spectrometer (NGIMS)/MAVEN have simultaneously (on the same day) measured the neutral densities in the Martian thermosphere on 5, 8, 10, 13, 16, and 29 June 2018. The measurement period f… Show more
“…The NGIMS measurements constitute the longest data of the Mars thermospheric neutral densities. These data were obtained during the medium to low solar activity period and when the Mars lower atmosphere witnessed the global and regional dust storms that perturbed the thermosphere significantly (Elrod et al 2020;Jain et al 2020;Venkateswara Rao et al 2020). The main results of our study are as follows:…”
In this study, we extracted the amplitudes of the gravity waves (GWs) from the neutral densities measured in situ by the neutral gas and ion mass spectrometer aboard the Mars Atmosphere and Volatile Evolution mission. The spatial and temporal variabilities of the GWs show that solar activity (the F10.7 cm solar flux corrected for a heliocentric distance of 1.66 au), solar insolation, and the lower atmospheric dust are the dominant drivers of the GW variability in the thermosphere. We developed a methodology in which a linear regression analysis has been used to disentangle the complex variabilities of the GWs. The three dominant drivers could account for most of the variability in the GW amplitudes. Variability caused by the sources of GWs and the effects of winds and the global circulation in the mesosphere and lower thermosphere are the other factors that could not be addressed. The results of the present study show that for every 100 sfu increase in the solar activity, the GW amplitudes in the thermosphere decrease by ∼9%. Solar insolation drives the diurnal, seasonal, and latitudinal variations of ∼9%, ∼4%, and ∼6%, respectively. Using the historical data of the dust opacity and solar activity, we estimated the GW amplitudes of the Martian thermosphere from MY 24 to MY 35. The GW amplitudes were significantly reduced during the maximum of solar cycle 23 and were highest in the solar minimum. The global dust storms of MY 25, 28, and 34 lead to significant enhancements in the GW amplitudes.
“…The NGIMS measurements constitute the longest data of the Mars thermospheric neutral densities. These data were obtained during the medium to low solar activity period and when the Mars lower atmosphere witnessed the global and regional dust storms that perturbed the thermosphere significantly (Elrod et al 2020;Jain et al 2020;Venkateswara Rao et al 2020). The main results of our study are as follows:…”
In this study, we extracted the amplitudes of the gravity waves (GWs) from the neutral densities measured in situ by the neutral gas and ion mass spectrometer aboard the Mars Atmosphere and Volatile Evolution mission. The spatial and temporal variabilities of the GWs show that solar activity (the F10.7 cm solar flux corrected for a heliocentric distance of 1.66 au), solar insolation, and the lower atmospheric dust are the dominant drivers of the GW variability in the thermosphere. We developed a methodology in which a linear regression analysis has been used to disentangle the complex variabilities of the GWs. The three dominant drivers could account for most of the variability in the GW amplitudes. Variability caused by the sources of GWs and the effects of winds and the global circulation in the mesosphere and lower thermosphere are the other factors that could not be addressed. The results of the present study show that for every 100 sfu increase in the solar activity, the GW amplitudes in the thermosphere decrease by ∼9%. Solar insolation drives the diurnal, seasonal, and latitudinal variations of ∼9%, ∼4%, and ∼6%, respectively. Using the historical data of the dust opacity and solar activity, we estimated the GW amplitudes of the Martian thermosphere from MY 24 to MY 35. The GW amplitudes were significantly reduced during the maximum of solar cycle 23 and were highest in the solar minimum. The global dust storms of MY 25, 28, and 34 lead to significant enhancements in the GW amplitudes.
“…Because of this diurnal asymmetry in enhancement, the diurnal pattern in GW activity ceases. It is known that during lower atmospheric dust storms, the thermosphere expands, and hence at any given altitude, the neutral densities are enhanced (e.g., Elrod et al., 2019; Jain et al., 2020; Liu et al., 2018; Venkateswara Rao et al., 2020). Thus, the thermosphere is hotter during PEDE‐2018 than normal times.…”
Understanding the structure and dynamics of the Martian thermosphere (100-220 km) is extremely important as this region, in particular the upper thermosphere, acts as a buffer zone between the reservoir of atmospheric species down below and the exosphere above from where the gaseous escape happens (e.g., Bougher, Cravens, et al., 2015). From this view point, the exobase acts as a lid on top of the thermosphere and the gaseous escape is regulated by the amount of energy, particles, and fields (both electric and magnetic) that reach the upper thermosphere. Thermospheric neutral densities, in general, decrease exponentially with an increase in altitude. Superimposed on this, there are perturbations of various scales that are due to forcings from above and below. Forcings from below include the planetary waves, thermal tides, and gravity
“…In addition to heating and cooling, persistent forcing by gravity waves (England et al, 2017;Fritts et al, 2006;Mahaffy et al, 2015;Medvedev & Yiğit, 2012;Terada et al, 2017;Williamson et al, 2019), thermal tides (Lee et al, 2009;Liu et al, 2017;Wilson, 2002), planetary waves (Hinson et al, 2003;Moudden & Forbes, 2010), seasonal inflation and contraction of the lower atmosphere (e.g., Bougher, Pawlowski, et al, 2015) and episodic forcings such as planet-encircling dust events (Elrod et al, 2020;Jain et al, 2020;Kuroda et al, 2020;Leelavathi et al, 2020;Liu et al, 2018;Venkateswara Rao et al, 2020) also play a key role in the energy redistribution and compositional changes in the Mars upper atmosphere. These forcings are indicative of energy transfer from the lower atmosphere to the thermosphere and hence coupling between the two regions (e.g., Bougher, Cravens et al, 2015).…”
The Mars thermosphere extends from the top of the mesopause (∼100 km) to the exobase (∼220 km) and its composition is dominated by CO 2 with O, O 2 , Ar, N 2 , CO, NO, C, He, and N being the other important neutral species (e.g., Bougher, Jakosky, et al., 2015). O becomes the dominant neutral species above somewhere between 180 and 270 km in the upper thermosphere and exosphere (e.g.,
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