Abstract
The origin of the sedimentary mound within Gale crater, the landing site for the Mars Science Laboratory rover Curiosity, remains enigmatic. Here we examine the total potential contribution of fluvial material by conducting a volume-based analysis. On the basis of these results, the mound can be divided into three zones: a lower, intermediate, and upper zone. The top boundary of the lowermost zone is defined by maximal contribution of water-lain sediments, which are ~13 to 20% of the total mound volume. The upper zone is defined by the elevation of the unbreached rim to the north (−2.46 km); sediments above this elevation cannot have been emplaced by flowing water. These volume balance calculations indicate that mechanisms other than flowing water are required to account for the overwhelming majority of the sediments transported into Gale crater. The most likely candidate process is settling from eolian suspension.
INTRODUCTION
The 154-km-diameter impact crater Gale was selected as the landing site for the Mars Science Laboratory (MSL) rover Curiosity in part because it presented an opportunity to explore the large central mound (Aeolis Mons, informally known as Mt. Sharp) (e.g., Grant et al., 2011; Golombek et al., 2012). Although there is clear evidence that the mound is sedimentary in origin, there remains uncertainty about the nature of the medium that transported and deposited those sediments, particularly whether the dominant transport agent was wind or water. A lacustrine origin was posited on the basis of observed channels and scarps interpreted as wave-cut terraces (Cabrol et al., 1999; Malin and Edgett, 2000). In contrast, an eolian-dominated formation scenario has been proposed on the basis of the inferred friability of material and lack of boulders (Irwin et al., 2004; Irwin et al., 2005) as well as outward-dipping bedding orientations (Kite et al., 2013). Results from the Curiosity rover indicate evidence for fluvial deposition of sediments on the crater floor (Williams et al., 2013; Grotzinger et al., 2014; Vaniman et al., 2014) and lower mound (e.g., Grotzinger et al., 2015; Fraeman et al., 2016; Fedo et al., 2017; Hurowitz et al., 2017; Rampe et al., 2017). But how much sediment in the central mound could have been contributed by fluvial processes? Here, we address this question with a mass-balance-type approach to compare the volume of the mound with the volume eroded from the catchment area by flowing water (Fig. 1). Specifically, we perform a source-to-sink analysis of the fluvially-transported sediment that was contributed to Gale crater. The ultimate source of fluvial sediment is the erosion of terrain within the catchment area.
On Mars, numerous authors have used a morphometric approach to infer the former flux of water in now-dry channels (e.g., Moore et al., 2003; Fassett and Head, 2005; Irwin et al., 2005; Burr et al., 2010), or estimate discharge from the volume of terminal deposits (e.g., Williams and Malin, 2008). Here, we consider two potential scenarios: one based on the current, modern topography, and another based on inferred paleotopograhy. The first scenario entails minimal assumed parameters and uses an estimate of the total eroded volume from the watershed area as a measure of the sediment supply. This approach is conceptually similar to the sediment budget analyses applied to catchment-fan systems where the volume of depositional fans is compared to the volume of inferred erosion in the catchment area (e.g., Jolivet et al., 2014; Palucis et al., 2014). In the second scenario, antecedent topography inferred from rover observation is included (e.g., Grotzinger et al., 2015).
METHODS
We used topography from the Mars Orbital Laser Altimeter (MOLA) instrument (Smith et al., 1999) and digital elevation models (DEMs) derived from High Resolution Stereo Camera (HRSC) images (Neukum and Jaumann, 2004) given in Fig. 1 (see also Table S1). As is evident in Fig. 1, only a portion of the exterior valley networks mapped by Hynek et al. (2010) lie within the boundaries of the HRSC DEMs. This subset of valley networks was measured and used to define median valley dimensions for the remainder of the contributing networks. Further details and uncertainty analyses are provided in the supplementary on-line materials (SOM) section.
MOUND VOLUME
The current mound volume was determined by measuring the difference in elevation between the mound surface and the inferred basal level, taken to be approximately −4.5 km in elevation. The resulting mound volume is 9.4±0.1×l03 km3. Following previous precedent (e.g., Grotzigner et al., 2015 SOM), we assume that the density of the eroded and deposited material is the same such that they can be directly compared. Volume changes due to the alteration of primary minerals are also not considered; the precipitation of secondary mineral phases in pore space is assumed to have no effect on the volume analysis considered here as it is inferred to be an isovolume process.
For context, this volume of sediment is significantly larger than the Eberswalde fan deposit (6–30 km3, e.g., Irwin et al., 2015), though smaller than the 1.5×l04 km3 layered mesa within the comparably-sized Henry crater (167.6 km in diameter) (Malin and Edgett, 2000). As discussed in the Supplementary Material, there is some uncertainty in the mound volume that results from the assumed base level and presence of a central peak (e.g., Gabasova and Kite, 2018). If one assumed the base is an inclined plane, for example, the mound volume would be reduced by one-third (i.e., to 6.1×l03 km3). In the second scenario considered here, the volume of the mound is inferred to have been ~1.8×l04 km3, which is roughly twice its present volume (see SOM and Grotzinger et al., 2015).
FLUVIAL ERODED SEDIMENT VOLUME
There are three components to consider in estimating the volume of sediment mobilized by water: the network of small interior channels, the valley network and large entrance breach in the south rim of Gale, and the eroded volume due to overland (i.e., non-channelized) flow.
Small Internal Channels
Gale crater exhibits numerous inward-draining channels but no outlet; evidence suggests it once hosted a lake (e.g., Grotzinger et al., 2015; Palucis et al., 2016), but it remained topographically closed. Numerous small inward-draining channels have been recognized, including 328 interior channel segments and 179 inverted channel segments (Le Deit et al., 2013), which have a total length of 1863 km (Fig. S1). Individual channel segments are typically 100–300 m in width and extend from a few km up to 35 km in length from the rim down to the crater floor. The lower portions of some of these channels stand in positive relief, indicating that a cementing agent has armored these former watercourses to form linear mesas due to later differential erosion (e.g., Pain et al., 2007). In prior measurements of terrestrial and martian inverted channels, the relative uniformity of inverted channel widths has been taken as evidence that these are approximately equal to the original widths of the channel fill deposits (Harris, 1980; Williams et al., 2009; Burr et al., 2010). Therefore, we estimate the total volume of missing material by summing the lengths of small negative-relief channels and valleys, adding the lengths of positive-relief inverted channels, and multiplying the total length by the typical third-order channel cross-sectional area (Table S3), to obtain a volume of roughly 200 km3 of sediment. For reference, the estimated volume of material removed due to channel incision in Peace Vallis is 0.8 km3, which is roughly equivalent to the volume of the Peace Vallis fan (0.9 km3) (Palucis et al., 2014). In the second scenario considered here that includes potential antecedent topography, early crater wall rim erosion is inferred to have contributed a vertical thickness of 0.5 to 0.6 km of material (after Grotzinger et al., 2015) that is deposited over the crater floor (see SOM for further details).
Valley Network System
Within the 1.20×l05 km2 watershed of Gale, 528 valley network segments have been identified (Hynek et al., 2010) and remapped using updated THEMIS mosaics (see SOM; Edwards et al., 2011; Fergason et al., 2013). Our goal is to quantify the eroded valley volume in order to bound the volume of sediment potentially available as Gale infill. We extracted topographic profiles orthogonal to the local downstream direction in order to measure 2D cross-sectional area. Fig. 2 gives a location plot of the 96 profiles (3 to 4 profiles per segment) with markers sized by cross-sectional area. Each valley network segment was assigned a stream order (Strahler, 1957).
For each segment, the eroded volume was determined by multiplying the cross-sectional area against the segment’s length. This calculation yields a volume of 109.5 km3 for the 434 km in the portion of the network included in HRSC DEM h1960_0000. As this represents only about 8% of the total length of the system of 5392 km, we grouped the area measurements by stream order to estimate the length-weighted median for each stream order (Table S3). Multiplying these areas by the total length of a given stream order yields a total cumulative volume of 8.1±12×l02 km3.
The confluence of the valley network system exterior to Gale is a single large channel, Farah Vallis, that incises the crater’s southwest rim (Greeley and Guest, 1987). Farah Vallis has a morphology consistent with other V-shaped martian valley networks (Williams and Phillips, 2001) and is a few km wide and ~100 m deep. The upstream morphology of Farah Vallis is partly buried by Gale ejecta, suggesting that the Gale impact disrupted it while it was active (Irwin et al., 2005),. If a significant fraction of the fluvial erosion occurred before the Gale impact, this would reduce our estimate of the sediment transported into Gale as this sediment would not be available for mound construction. In a similar manner, the routing of the valley network through a partially-filled, 46-km diameter crater (unnamed crater ‘A’ in Fig. 1) may also have reduced the sediment delivered to Gale (Irwin et al., 2005; Ehlmann and Buz, 2015), but the exact amount of this reduction depends on the timing of flow through the network. Since there is wide uncertainty in determining the magnitude of these effects, we took no further corrective action other than noting that our fluvially transported sediment volume estimate is at the upper end of the range of plausible values.
Overland Flow
In addition to channelized flow, landscape denudation in overland or non-channelized flow must also be considered. To the south, the 120,000 km2 Gale watershed terminates against the northern rim of the Herschel crater (Fig. 1). Average landscape denudation of 75 m throughout the watershed would yield a volume of sediment that matches the mound volume. However, while such a value might be plausible during the intense erosion in the Early Noachian (Hynek and Phillips, 2001), it is unreasonably high after this time, at least for most places on Mars. Estimates of post-Middle Noachian erosion rates are more than an order of magnitude lower (e.g., Golombek et al., 2006; Matsubara et al., 2018). For example, ~2 m of denudation was inferred in Milna crater watershed in the Margaritifer Sinus Quadrangle during a similar period of time (Buhler et al., 2014). We adopt this value as a representative erosion rate for this time period in Gale, yielding ~2.4 × 102 km3 of sediment from the Gale watershed. We acknowledge, however, that erosion rates on Mars vary widely in space and time. But even this value is likely an overestimate for denudation relevant to Gale given the minimal contribution of non-channelized erosion to the Peace Vallis fan (~12% of the channelized eroded volume) estimated previously (Palucis et al., 2014). Additionally, the presence of relatively unmodified Gale ejecta partially blanketing the valley network draining into Gale (Irwin et al., 2005) constrains the volume of material moved by overland flow to be minimal.
DISCUSSION
Based on the current topography, the total volume of material moved by flowing water into Gale is at most ~1.3×l03 km3, which is ~13 to 20% of the present volume of the mound (Table 1, Fig. S3). It is readily apparent that the volume of the present mound exceeds the volume of sediment from Gale’s catchment area mobilized by the contributory fluvial network and overland flow by a factor of 5 or more. Thus, mechanisms other than fluvial transport are needed to explain the remaining 80 to 87% of the mound’s sedimentary budget. Previously suggested transportation mechanisms include fluvial, lacustrine, eolian, and polar processes (niveo-eolian), or some combination of the above (e.g., Cabrol et al., 1999; Malin and Edgett, 2000; Irwin et al., 2005; Anderson and Bell, 2010; Milliken et al., 2010; Thomson et al., 2011; Kite et al., 2013). We will return to these options below after considering the topographic implications of these sediment volume estimates. If inferred paleotopography is included, the proportion of the mound moved by water is subject to greater uncertainty, but could be up to 37% (Table S5).
Table 1.
Volume [km3] | Source |
---|---|
2±1 × 102 | Interior channels |
8.1±13 × 102 | Exterior valley network (inc. Farah Vallis) |
≤ 2.4 × 102 | Overland flow |
9.4±0.1 × 103 | Mound volume |
Improved knowledge about the volume of fluvially-transported sediment provides constraints on the maximum elevation where one would expect this material to be found both on and within the mound. As previously noted (e.g., Malin and Edgett, 2000; Irwin et al., 2004; Irwin et al., 2005; Thomson et al., 2011), the mound of Gale rises to an elevation that is almost 3 km higher than the lowest point of the northern rim. Thus, formation of the entire mound in a lacustrine environment would necessitate filling of the northern plains (Fig. 3). There is no evidence of any scour or incision of commensurate scale with this volume of water either into or out of the northern rim of Gale. In this case, we interpret an absence of evidence as evidence of absence, i.e., the lack of a hydrological connection to the northern plains as consistent with such a connection never having formed (Irwin et al., 2004; Irwin et al., 2005). This (non-existent) spillway nevertheless provides a maximum elevation constraint, −2.46 km, above which a lacustrine origin is not tenable. Any putative northern ocean thus would need to either predate Gale, or have a maximum high stand less than approximately −2.46 km; in either case, an ocean could not have contributed to Gale’s sediment budget. One factor that contributes to the uncertainty associated with this elevation level is that the northern rim originally may have been slightly higher, although Irwin et al. (2004, 2005) noted that that a north-to-south asymmetry in the crater profile is to be expected given the crater’s formation on the regional slope of the dichotomy boundary.
Second, we can also place some constraints on the maximum elevation where one would expect fluvially-transported material to be found within the mound. In Fig. 3a, we have tabulated the cumulative volume of material present at or below a given elevation in the mound. Using the present mound topography, the volume of fluvially transported material (~1.3×l03 km3) corrEsponds to an elevation range of−4.21 km to 3.47 km, given choice of assumptions for the mound basal topography (Table S4). This elevation range is about 290 to 1000 m above the base elevation. We therefore propose that fluvial sediments should be located below an elevation of−3.47 km if they constitute mound-forming units (Curiosity crossed the −4.21 elevation in September of 2017 (Fig. 3c), and no abrupt transitions were noted). In the paleotopography scenario, the elevation of this lower boundary is estimated to be toward the upper end of this range (−3.7 to −3.3 km; Table S5).
Implications for the origin of the mound
The results help place constraints upon the origin of strata within three zones of the central mound in Gale. Fluvially-transported material could constitute the lower layers of the mound up to an elevation range of−4.21 km to −3.47 km (Fig. 3), consistent with rover observations (e.g., Grotzinger et al., 2015; Fraeman et al., 2016; Hurowitz et al., 2017). One caveat with this elevation constraint is that it assumes the present mound topography; in the paleotopography scenario, the elevation of this lower boundary is estimated to be −3.7 to −3.3 km. For the uppermost 3 km of the mound, a fluvial or lacustrine origin is not consistent as it lies above the northern rim elevation of −2.46 km (Irwin et al., 2004; Irwin et al., 2005). Here, eolian constructional processes are required given the lack of a northern rim breach.
In the intervening ~1 km, i.e., mound material at elevations >−3.47 km and <−2.46 km, it is also likely that the majority of sediment was delivered via the same eolian mechanism responsible for the upper mound. However, water-transported sediments are not precluded in this interval. If fluvial or lacustrine sediments are recognized in this intermediate elevation range (e.g., Dietrich et al., 2013; Le Deit et al., 2013; Fairén et al., 2014; Palucis et al., 2016), this necessitates that additional sources of sediment contributed to the volume of the mound when lakes fed by fluvial and potentially groundwater sources in Gale were operative. For example, wind-blown dust or ash may have contributed some fraction of the sediment during lacustrine phase(s) of evolution, a potential source that is unbounded in this current analysis. Despite these uncertainties, our results suggest that if fluvial or lacustrine deposits are found above an elevation of −3.47 km yet below −2.46 km, they either will be interleaved with other strata or present as mounddraping units that are bounded by basal unconformities depending on if the mound was partially or fully formed at the time of their deposition, respectively.
These results provide specific, testable constraints for the MSL rover. For layers identified via in situ analysis as having a fluvial-delatic or lacustrine origin, both their elevation and their stratigraphic context (i.e., whether they are present as mound-forming or mound-draping units) will help refine the geologic history of sedimentary deposition within Gale. Specifically, these characteristics will provide constraints upon the nature of and relative timing between the fluvial, lacustrine, and eolian processes that have contributed sediment to the Gale mound.
Supplementary Material
ACKNOWLEDGEMENTS
We greatly appreciate the work of four anonymous reviewers on an earlier version of the manuscript. This work was supported by NASA’s Mars Data Analysis Program (80NSSC17K0647). The raw data for this study are publically available in NASA’s Planetary Data System; the primary source for HRSC data is ESA’s Planetary Science Archive. Individual profile measurements underlying Figure 2 are included in the Supporting Information.
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