MSL FROST DETECTION CAMPAIGNS G.M. Martínez, Lunar and Planetary Institute/USRA, Houston, USA (gmartinez@lpi.usra.edu), R.V. Gough, CIRES and University of Colorado, Boulder, USA, W. Rapin, IRAP, CNRS-UPS, Toulouse, France, P.-Y. Meslin, IRAP, CNRS-UPS, Toulouse, France, O. Gasnault, IRAP, CNRS-UPS, Toulouse, France, S. Schröder, DLR, Berlin, Germany, T.H. McConnochie, Space Science Institute, USA, H. Savijärvi, Finnish Meteorological Institute, Helsinki, Finland, E. Fischer, University of Michigan, Ann Arbor, USA, S. Guzewich, NASA Goddard Spaceflight Center, Greenbelt, USA, C.E. Newman, Aeolis Research, USA, A. R. Vasavada, Jet Propulsion Laboratory, California Institute of Technology, Pasadena, USA, M. de la Torre-Juárez, Jet Propulsion Laboratory, California Institute of Technology, Pasadena, USA, R. Wiens, Purdue University, West Lafayette, USA, and N. Lanza, LANL, Los Alamos, USA., Introduction: We report results of the frost detection campaigns performed by the Curiosity rover during the first 3332 sols of the Mars Science Laboratory (MSL) mission. Also, we describe the observational strategy and target selection of these campaigns to support NASA’s Mars 2020 and future missions in the search for frost on Mars. We use environmental measurements from the Rover Environmental Monitoring Station (REMS) to predict frost formation, and ChemCam Laser Induced Breakdown Spectroscopy (LIBS) to detect enhanced hydration levels. Only when both instruments return positive results, we interpret that the formation of frost is likely. Out of 14 campaigns (Table 1), only on sol 2548 (Ls ~ 89°) in Martian Year (MY) 35 both REMS and ChemCam LIBS returned results consistent with frost formation. However, we note that these results were not unambiguous, and that future lab studies will improve our understanding of ChemCam sensitivity to frost. REMS and ChemCam Instruments: REMS is the weather station onboard MSL. It includes six sensors measuring atmospheric pressure, UV fluxes, wind velocity (which stopped working at around sol 1500), air temperature, ground temperature, and relative humidity [1–3]. The REMS sampling strategy consists of 5-min-long hourly samples at 1 Hz, with interspersed full hour sample periods at 1 Hz to cover every time of the sol over a period of a few sols. The LIBS instrument, part of the ChemCam instrument package, is able to perform remote and sensitive elemental analysis that includes the identification of submicron-thick frost layers [4–5]. Environmental Context: Fig. 1 shows REMS measurements of ground temperature (T g), relative humidity (RH), and water vapor volume mixing ratio (VMR) for the first 3332 sols of MSL mission. In every MY, the ground temperature shows the coldest annual values and the RH shows the highest annual values between late southern fall and early winter. Table 1. List of frost/hydration detection campaigns by the Curiosity rover during the first 3332 sols of the MSL mission. Only on sol 2548 in MY 35, both REMS and ChemCam returned results indicating the likely formation of frost on a soil patch informally named Kilpatrick. ‘Maybe’ indicates positive results without enough certainty. The nighttime VMR shows annual maximum values at Ls ~ 160°, when the water vapor column abundance at Gale is highest [5]. The RH reached saturation levels in MY 35, although fog has not been detected by the mission. VMR×P, where es is the saturation vapor pressure over ice [6], e is the water vapor pressure at 1.6 m, and P is the atmospheric pressure. In establishing this comparison, and due to the lack of humidity measurements at the ground, we implicitly assume that the water vapor content is constant in the first 1.6 m. Uncertainties derived from this assumption will be assessed as part of an ongoing manuscript. Fig. 2 shows the seasonal evolution of the maximum and minimum Tg (black), along with Tf values calculated when the RH at the ground (~e/es(Tg)) is highest (blue), which typically occurs right before sunset (LMST ~0500–06:00). Most frost events are predicted to occur seasonally within the Ls 90°–110° period, when the ground temperature falls below the frost point. We note that Tg measurements in the second half of MY 35 and in MY 36 are subjected to strong electronic noise at nighttime, and thus the uncertainty in minimum Tg values is larger. Figure 2. Seasonal evolution of the maximum and minimum ground temperature measured by REMS (black), and of the frost point calculated when the RH at the ground, RHg ~e/es(Tg), is highest (blue). The ground temperature falls below the frost point on several sols during fall and winter (mostly in the Ls 90°–110° period), and on a few sols during summer and spring, suggesting potential frost events. Figure 1. Interannual and seasonal evolution of the daily maximum, mean and minimum ground temperature (top), daily maximum RH (middle), and nighttime VMR (bottom). The daily maximum RH is generally achieved between 04:00 and 06:00 LMST, when the temperature is coldest. VMR values are obtained at the same time as the RH shown above. To predict frost events with REMS, we compare Tg with the frost point (Tf) calculated as es(Tf) = e = Target Selection: Three types of targets have been considered as part of our Frost Detection Campaigns: (1) soil/sand, (2) rocks, and (3) ventifacted rock fingers. Each type presents pros and cons for the potential formation of frost. Soil/sand has low thermal inertia, and therefore it can get colder overnight. However, this type of terrain is porous, and thus water vapor might diffuse to some depth before forming frost. Rocks are not porous but have high thermal inertia, and thus stay warmer overnight. Finally, ventifacted rock fingers have relatively low thermal inertia and are not porous, but it is challenging to estimate their temperature (the REMS ground temperature sensor has a field of view of a few m2, while the size of ventifacts is of the order of cm). Because frost at the Viking 2 landing site preferentially formed and persisted on soils as opposed to rocks (Fig. 3), it was decided to select this type of terrain in the campaigns of MYs 35 and 36 (Table 1). ing dawn vs daytime, suggesting there was no detectable change in water content overnight. Results for Kittybrewster, not shown, are similar to those of the Kinnordy target (i.e., no H enhancement). Figure 3. Color image by Viking Lander 2 camera showing frost preferentially on the soil. Credit: NASA/JPL. Observational Strategy of MSL Frost Campaign in MY 35: Three targets were analyzed by ChemCam LIBS during this campaign: Kilpatrick on sol 2548 at Ls = 89° (Fig. 4); Kinnordy on sol 2565 at Ls = 97°; and Kittybrewster on sol 2582 at Ls = 104°. All targets met the following selection criteria: (1) a fine-grained soil patch, (2) larger than 5 cm in size and (3) more than 3 m from the rover. This was decided to ensure thermal insulation from higher thermal inertia rocks, and to avoid thermal contamination from the rover. For each target, a ChemCam raster was collected a few minutes before sunrise (~05:50 LMST), when temperature is at its coldest and RH at its highest, and another was collected around 13:00, when temperature is at its warmest and RH at its lowest. Each raster consisted of 10 points spaced along a line (Fig. 4, top), with 10 shots on each point. The hydrogen emission peak at 656.6 nm is extracted from the spectra [5,7] and several signal normalizations are tested to compare day/dawn pairs of observations. Contemporaneously to ChemCam, REMS measurements of Tg, RH and P were collected to document the rapidly changing environmental conditions near sunrise. From these measurements, the frost point at the surface was determined assuming constant mixing ratio in the lower 1.6 m of atmosphere. Results of MSL Frost Campaign in MY 35: Fig. 5 shows the ground temperature (red) and frost point (blue) for Kilpatrick (top) and Kinnordy (bottom) on sols 2548 and 2565, respectively. For Kittybrewster, not shown, the diurnal evolution of both quantities was similar to that of Kinnordy. Only at Kilpatrick the environmental conditions were favorable for the formation of frost, where the ground temperature fell well below the frost point between 05:00 and 06:00 LMST. Fig. 6 shows ChemCam LIBS normalized H signals at Kilpatrick (top) and Kinnordy (bottom), both at daytime (left; ~13:00 LMST) and dawn (right; ~05:40 LMST). Only for Kilpatrick there was enhanced average H signal in shots at dawn relative to daytime, above point-to-point signal variability. For Kinnordy, there is no difference in the H signal dur- Figure 4. (Top) ChemCam Remote Micro-Imager image of Kilpatrick target on sol 2548. (Middle) Mastcam image of the surroundings. (Bottom) Navcam image with REMS’ field of view of ground temperature on sol 2548. Conclusions: Out of 14 frost detection campaigns performed along the MSL traverse, only on sol 2548 (Ls ~ 89°) in MY 35 both REMS and ChemCam LIBS returned results consistent with the Temperature (K) formation of frost. REMS observations suggested frost formation between 05:00 and 06:00 LMST and ChemCam LIBS showed enhanced average H signal in shots at dawn relative to daytime, above point-topoint signal variability. We interpret these results as likely frost formation. However, we are not able to determine the phase or distribution of this transient water, and adsorbed water layers on soil grains are also a possible cause. Point-to-point variability and signal normalization are the main limitations of these LIBS measurements. Future lab studies should improve our understanding of ChemCam sensitivity to frost. 270 260 250 240 230 220 210 200 190 180 170 160 Tg Tf Sol 2548 Kilpatrick Potential Frost Event 0 2 4 6 8 280 Temperature (K) Tg Tf Sol 2565 Kinnordy 260 10 12 14 16 18 20 22 24 LMST 240 220 200 180 160 140 0 2 4 6 8 10 12 14 16 18 20 22 24 LMST Figure 5. Diurnal evolution of ground temperature (red) and frost point temperature (blue) on sols 2548 (top) and 2565 (bottom). Between 05:00 and 06:00 LMST on sol 2548, the ground temperature fell well below the frost point, indicating favorable conditions for frost formation. Sunrise was ~05:50 LMST on both sols. Figure 6. Comparison of ChemCam LIBS hydrogen signal collected at targets Kilpatrick (a) and Kinnordy (b) during the day (left) and dawn (right). References: [1] Gómez‐ Elvira, Javier, et al. "Curiosity's rover environmental monitoring station: Overview of the first 100 sols." Journal of Geophysical Research: Planets 119.7 (2014): 1680-1688. [2] Martínez, G. M., et al. "The modern near-surface Martian climate: a review of in-situ meteorological data from Viking to Curiosity." Space Science Reviews 212.1 (2017): 295-338. [3] Newman, Claire E., et al. "MarsWRF convective vortex and dust devil predictions for Gale Crater over 3 Mars years and comparison with MSL‐ REMS observations." Journal of Geophysical Research: Planets 124.12 (2019): 3442-3468. [4] Meslin, P-Y., et al. "Soil diversity and hydration as observed by ChemCam at Gale Crater, Mars." Science 341.6153 (2013): 1238670. [5] Schröder, S., et al. "Hydrogen detection with ChemCam at Gale crater." Icarus 249 (2015): 43-61. [6] McConnochie, Timothy H., et al. "Retrieval of water vapor column abundance and aerosol properties from ChemCam passive sky spectroscopy." Icarus 307 (2018): 294-326. [7] Rapin, William, et al. "Quantification of water content by laser induced breakdown spectroscopy on Mars." Spectrochimica Acta Part B: Atomic Spectroscopy 130 (2017): 82-100.