Research Article

The Global Topography of Mars and Implications for Surface Evolution

See allHide authors and affiliations

Science  28 May 1999:
Vol. 284, Issue 5419, pp. 1495-1503
DOI: 10.1126/science.284.5419.1495

This article has a correction. Please see:

Abstract

Elevations measured by the Mars Orbiter Laser Altimeter have yielded a high-accuracy global map of the topography of Mars. Dominant features include the low northern hemisphere, the Tharsis province, and the Hellas impact basin. The northern hemisphere depression is primarily a long-wavelength effect that has been shaped by an internal mechanism. The topography of Tharsis consists of two broad rises. Material excavated from Hellas contributes to the high elevation of the southern hemisphere and to the scarp along the hemispheric boundary. The present topography has three major drainage centers, with the northern lowlands being the largest. The two polar cap volumes yield an upper limit of the present surface water inventory of 3.2 to 4.7 million cubic kilometers.

Long-wavelength topography (changes in topography over scales of hundreds to thousands of kilometers) reflects processes that have shaped Mars on a global scale and thus is of particular interest in the context of the planet's evolution. The Mars Orbiter Laser Altimeter (MOLA) (1), an instrument on the Mars Global Surveyor (MGS) spacecraft (2), recently acquired the first globally distributed, high-resolution measurements of the topography of Mars (3). A geodetically controlled topographic model derived from circum-Mars (Fig. 1) and northern hemisphere (4,5) profiles has enabled quantitative characterization of global-scale processes that have shaped the martian surface.

Figure 1

Global profile of Mars from MOLA crossing longitudes 52°E and 247°E. The north and south polar caps are at the top and bottom. The Pavonis Mons and Alba Patera volcanic shields, both located within the Tharsis province, appear at the upper left, and the Hellas impact basin is at the lower right. The contrast in elevation and regional topographic roughness between the northern and southern hemispheres is also apparent. The dichotomy boundary scarp can be seen at ∼50° east of north. Distributed points above the surface correspond to false returns caused by solar background at the laser wavelength and represent <0.5% of the transmitted pulses. Clustered returns above the surface near the south pole are from clouds. The vertical exaggeration is 100:1.

Before the MGS mission, models of martian topography were derived from Earth-based radar ranging (6), Mariner 9 and Viking 1 and 2 radio occultations (7), stereo and photoclinometric observations from Mariner 9 and Viking imagery (8), and the Mariner 9 ultraviolet and infrared spectrometers (9). Disparate measurement types were combined into digital terrain models (10) that were of variable spatial resolution and typically characterized by vertical errors of ∼1 to 3 km. The model from MOLA (Fig. 2) (11) has a spatial resolution of ∼1° (or ∼59 km separation at the equator) and an absolute accuracy of 13 m with respect to Mars' center of mass (COM) (12). The global topography of Mars is now known to greater accuracy than Earth's continents in a root mean square (rms) sense.

Figure 2

Maps of the global topography of Mars. The projections are Mercator to 70° latitude and stereographic at the poles with the south pole at left and north pole at right. Note the elevation difference between the northern and southern hemispheres. The Tharsis volcano-tectonic province is centered near the equator in the longitude range 220°E to 300°E and contains the vast east-west trending Valles Marineris canyon system and several major volcanic shields including Olympus Mons (18°N, 225°E), Alba Patera (42°N, 252°E), Ascraeus Mons (12°N, 248°E), Pavonis Mons (0°, 247°E), and Arsia Mons (9°S, 239°E). Regions and structures discussed in the text include Solis Planum (25°S, 270°E), Lunae Planum (10°N, 290°E), and Claritas Fossae (30°S, 255°E). Major impact basins include Hellas (45°S, 70°E), Argyre (50°S, 320°E), Isidis (12°N, 88°E), and Utopia (45°N, 110°E). This analysis uses an areocentric coordinate convention with east longitude positive. Note that color scale saturates at elevations above 8 km.

Global shape. The difference of ∼20 km between the polar and equatorial radii indicates that the largest contribution to shape is the planetary flattening (Table 1), which is due mostly to the rotation of Mars with a small contribution (∼5%) (13) from the vast volcano-tectonic Tharsis province (Fig. 2), situated near the equator. Subtraction of the gravitational potential or geoid (14) from radii measurements represents elevations in terms of topography and eliminates the contribution due to rotation, thus clarifying other long-wavelength components of the shape. Figure 2 illustrates that topography on Mars has a 30-km dynamic range, the largest of the terrestrial planets. The large topographic excursions are due to ancient impact basins, large shield volcanoes, and the ability of the planet's rigid outer shell (lithosphere) to support significant stresses associated with surface and subsurface loads (15).

Table 1

Mars geodetic parameters from MOLA.

View this table:

A useful representation of the planetary shape is the triaxial ellipsoid, for which the axes and orientation with respect to a coordinate system with origin at the COM of Mars are given in Table 1. The best fit ellipsoid (16) is dominated by a displacement from the COM by −2986 m along the z axis, which represents an offset between the COM and the planet's geometric center or center of figure (COF) along the polar axis. The sign of the offset indicates that the south pole has a higher elevation than the north pole by ∼6 km, which corresponds to a systematic south-to-north downward slope of 0.036°. The triaxial ellipsoid is also displaced by −1428 m along the y axis, in the general direction of the Tharsis topographic rise (Fig. 2).

Major features of topography. The dominant feature of the topography is the striking difference (∼5 km) in elevation between the low northern hemisphere and high southern hemisphere that represents one of the outstanding issues of martian evolution. This hemispheric dichotomy also has a distinctive expression in the surface geology of Mars. The surface of the crust in the southern hemisphere is old and heavily cratered, whereas that in the north is younger and more lightly cratered and was probably volcanically resurfaced early in Mars' history (17). The hemispheric difference is also manifest in surface roughness (Fig. 3) calculated from the MOLA topographic profile data (18). Most of the northern lowlands is composed of the Late Hesperian–aged (19) Vastitas Borealis Formation, which is flat and smooth (Fig. 2), even at a scale as short as 300 m (Fig. 3). The Amazonian-aged (19) Arcadia Formation, which overlies the Vastitas Borealis Formation, is also smooth at large and small scales, consistent with either a sedimentary (4, 20) or volcanic (21) origin for these plains. In the southern hemisphere Noachian-aged (19) ridged plains form locally flat intercrater deposits, whereas younger Hesperian-aged ridged plains dominate in some regions. All are characterized by a rougher topography than the northern plains. The boundary between the smooth northern hemisphere and the rough southern hemisphere is characterized by mesas, knobs, and intervening plains (22), as well as regional elevation changes of up to 4 km over distances of 300 to 1300 km (23). Where the regional elevation change is relatively steep, it is referred to as the dichotomy boundary scarp (compare Fig. 1).

Figure 3

Interquartile scale (IQS) surface roughness (18) of Mars calculated from MOLA profiles on a 330-m baseline in a 100-km running window. The projections are the same as inFig. 2.

The Tharsis province is a vast region of volcanism and deformation that appears to interrupt the global dichotomy boundary between the southern cratered highlands and northern lowland plains (24). In previous work the province was displayed as a broad topographic rise (10). However, Fig. 2 (see also Fig. 6) shows that topographically Tharsis actually consists of two broad rises. The larger southern rise is superposed on the highlands as a quasi-circular feature that extends from ∼220°E to ∼300°E and from ∼50°S to ∼20°N and spans about 107 km2 in area. The highest portion of the southern rise contains the Tharsis Montes (Ascraeus, Pavonis, and Arsia). Eastward of the highest terrain but still elevated are the ridged plains of Lunae Planum (Fig. 2). The smaller northern rise is superposed on the lowlands and covers approximately the same longitude band as the southern rise, but extends to ∼60°N. The northern rise is dominated by the massive volcanic construct of Alba Patera (compare Fig. 1). Hesperian-aged volcanic fans emanate radially from this shield into the northern lowlands for distances of more than 1000 km. The new data emphasize the distinctive nature of the Alba Patera structure as well as its connection to the Tharsis Montes region. In contrast, the massive Olympus Mons volcano appears to sit off the western edge of the Tharsis rise rather than on the flank, as previously mapped (10). By its spatial association, Olympus Mons is nonetheless likely to have had a genetic link to volcanism in Tharsis proper.

The new topographic data illuminate a long-standing debate over the dominant contributors to the high elevations of the Tharsis region. A prominent ridge (containing Claritas Fossae; Fig. 2) extends southward from the region of the Tharsis Montes, and then curves northeastward in a “scorpion tail” pattern. This arcuate ridge bounds Solis Planum, a plateau within the southern rise. The ridge contains an abundance of heavily cratered Noachian material that has presumably escaped resurfacing by younger Tharsis volcanic flows because of its high elevation. It has been suggested (25) that the termination of the ridge structure could have formed by lithospheric buckling, as could, by analogy, other ridge structures in the south Tharsis region. The southern rise (southward of ∼35°S) also contains exposures of heavily cratered Noachian units. These elevated ancient terrains are consistent with the view that the broad expanse of the southern rise (elevations >∼3 km; see Fig. 2) formed at least in part by structural uplift (26). Such a hypothesis is supported by the orientation of fractures and graben in Claritas Fossae (24), although it is also possible that there has been a contribution from lateral tectonic forces (25). The high elevations of the Tharsis Montes region as well as of the northern rise display major contributions from volcanic construction (27), although some structural uplift may have subsequently been masked by volcanism (28).

The Hellas impact basin has the deepest topography on Mars and is characterized by a total relief of more than 9 km (Fig. 4). Mountains and massifs previously identified as constituting the main basin ring of Hellas have a diameter of ∼2300 km (29) and are situated on the inner slopes of the topographic basin (Fig. 4). Basin ejecta material surrounding Hellas has not been mapped at the global scale; units that surround the basin are dominated by Noachian-aged heavily cratered plains (19). MOLA data reveal, however, a peak in the distinctive topographic annulus that surrounds Hellas at a diameter of ∼4000 km, lying ∼2 km above the main ring.

Figure 4

Regional topographic model of the Hellas basin. (Top) Azimuthally averaged radial topography used in the calculation of infilling the basin with surrounding material postulated to have been excavated from it. (Bottom) Color-coded topography plotted in an equal-area projection with the same scale as that in Fig. 2. The black lines correspond to zero-elevation contours.

In terms of size and morphology, Hellas has striking similarities to the South Pole–Aitken basin on the farside of the moon. These two impact structures have similar diameters and volumes (30), as well as distributions of surrounding excavated material, though the material encircling South Pole–Aitken is more asymmetric. Hellas represents a major topographic excursion that dominates much of Mars' southern hemisphere topography (compare Fig. 1). Previous researchers have noted the great depression, but no previous topographic model has resolved the expanse of Hellas' exterior topographic annulus, which is likely due to ejecta, but possibly includes contributions from impact melt, structural uplift, and admixed local material. This material represents a major redistribution of Mars' early crust. Figure 4 was used to determine that the volume of the topographic annulus, if “refilled” into the basin, would cause the basin and surroundings to have an elevation of ∼600 m with respect to the global reference. Material removed from Hellas thus accounts for a significant amount of the high-standing topography of Mars' southern hemisphere. The observed topographic annulus around Hellas is close to the position of the outermost mapped basin ring [diameter ∼4200 km (29)]. An alternative explanation for the topography is that this outermost ring might represent the highly degraded main basin rim, with additional ring structures lying lower within the basin.Figure 4 also shows that material from Hellas' topographic annulus contributes to the topographic expression along part of the dichotomy boundary.

Implications for evolution. The hemispheric dichotomy represents both an elevation difference and a difference in surface geology, and although these two defining aspects may be related, they do not necessarily share the same mechanism of formation. Hypotheses to explain the hemispheric dichotomy have included thinning of the northern hemisphere crust by mantle convection (31, 32), an early period of tectonic plate recycling (33), and one or more large impacts in the northern hemisphere (34–36).

A key issue is to determine how much of the hemispheric elevation difference is due to the long-wavelength planetary shape rather than the boundary scarp (23, 37); this issue can be explored from the global distribution of elevations and slopes (Fig. 5). As shown in Fig. 5, which plots histograms of elevations before and after removing the offset between the COM and COF along the polar axis, the z component of the COM-COF difference is largely equivalent to the hemispheric elevation difference. A histogram of the distribution of 100-km baseline slopes (38) calculated from the global topographic grid (Fig. 5C) peaks at ∼0.3° and is long-tailed, the latter feature a result of topographic excursions associated with volcanoes, impact basins, and tectonic features. The slope corresponding to the peak in the distribution is close to the average longitudinal slope associated with the COM-COF offset along the z axis and is partly a result of the offset. But the peak slope also contains contributions due to Tharsis and regional-scale features.

Figure 5

Histograms of (A) topography, (B) heights with respect to an ellipsoid shifted by −2.986 km along the z axis, and (C) 100-km baseline slopes. The histogram in (A) shows the distinct bimodal signature that represents the elevation difference between the northern and southern hemispheres. That in (B) shows elevations plotted with respect to an ellipsoid whose center is shifted so as to remove the effect of the COM-COF offset along the polar axis. The effect of the shift is to produce a unimodal distribution of elevations; that is, the hemispheric difference in elevation largely disappears.

Subtracting the COM-COF offset along the polar axis from the global topography model (Fig. 6) eliminates most of the hemispheric elevation difference, causing a large part of the southern hemisphere, away from Tharsis and Hellas, to display elevations as low as those over a significant fraction of the northern hemisphere. Together, Figs. 5 and 6 demonstrate that the COM-COF offset accounts for most of the elevation difference between the northern and southern hemispheres and indicate that the hemispheric elevation difference is primarily a long-wavelength effect.

Figure 6

Map of Mars' shape with zonal spherical harmonic degree 1 (COM-COF offset along the polar z axis) removed. The projection is rectangular to show topography from pole to pole. Note the general similarity in elevation between the northern and southern hemispheres. The figure highlights the two other significant components of martian topography: the Tharsis province and the Hellas impact basin. Here we have not removed shorter wavelength topographic features, including those composing the dichotomy boundary scarp.

A projection of the northern hemisphere topography from the pole to the equator (Fig. 7) further illustrates the nature of the northern hemisphere depression. Note the distinctive circular signature of the buried Utopia basin, originally proposed as an impact feature on the basis of geological evidence (35), but not observed in earlier topographic studies. The circular expression of Utopia is apparent despite its location within the area of northern hemisphere resurfacing (5, 39). However, even after accounting for the formation of the Tharsis rise, presumably subsequent to the process that produced the hemispheric elevation difference, the boundary of the northern hemisphere depression is clearly noncircular, and we see no compelling topographic evidence for a hemispheric-scale single impact such as previously proposed (34). Formation of the elevation difference by multiple smaller impacts has also been suggested (36). Beyond Utopia, however, no circular structures of comparable scale are apparent in the topography of the northern plains, although arguably such structures could have been masked by processes that occurred subsequent to formation.

Figure 7

(left). Lambert equal-area projection of pole-to-equator topography in the northern hemisphere. The Utopia basin is the circulardepression (in light blue) in the upper right.

MGS gravity data (40) provide additional perspective on crustal structure beneath the resurfaced northern hemisphere. Large (though smaller than hemispheric-scale) impacts such as Utopia and Hellas are marked by distinctive positive gravitational anomalies (40). However, no other anomalies of comparable spatial scale occur in association with regional topographic lows in the northern hemisphere, except for the previously known Isidis impact structure that sits on the dichotomy boundary. We thus suggest that the long-wavelength topographic expression of the northern hemisphere depression was shaped by an internal process or processes. The MOLA topography does not permit us to rule out the possibility of a focusing of internal activity in the vicinity of an early impact (36,41). However, if this focusing occurred, subsequent reworking of the northern crust by internal processes must have obliterated the record of basin circularity.

Distinguishing between internal mechanisms, mantle flow versus plate recycling, will require further study. Mantle convection calculations show that a deep-mantle phase transition would enable the development of hemispheric-scale (harmonic degree 1) convective instabilities on Mars (42), but additional analysis is required to understand how such a mantle flow scenario, coupled with its lithospheric response, could produce the observed long-wavelength topography. Recent observations by the MGS magnetometer experiment show magnetic anomalies of high magnitude that have been interpreted as evidence of an early, vigorous hydrodynamic dynamo in the martian core (43). The largest magnetic anomalies are confined to the southern highland crust, and because anomalies are generally absent near large southern hemisphere impact basins, a rapid decay in the strength of the dynamo and the global magnetic field in the first ∼500 million years of martian history is inferred (43). Either an early Noachian era of plate recycling (33, 43) or vigorous mantle convection would be consistent with an early core dynamo.

Important new constraints on the lithospheric thermal structure and heat flow in the southern hemisphere of Mars come from the high relief (Fig. 4) and gravity signature (40) of the Hellas basin and the amplitudes of the largest crustal magnetic anomalies (43). The 9 km of present relief displayed by Hellas implies that the mechanical lithosphere of Mars at the time of basin formation was at least locally of substantial thickness and long-term strength. The implied stress differences supported by martian lithospheric strength exceed those for the South Pole–Aitken basin on the moon (30) with its lower gravitational attraction, and would be larger still if the proposed ∼2 to 3 km thickness of Late Noachian to Amazonian units that blanket the floor of Hellas (44) were removed. If the basin is ∼90% isostatically compensated, as suggested from gravity data (40), then a basin relaxation model (45) indicates that the elastic lithosphere thickness at the time of Hellas' formation was ∼30 km. The thicknesses of coherently magnetized crustal blocks required to account for the observed magnetic anomalies with magnetizations no greater than for common terrestrial rocks also demand that temperatures were below the Curie temperature of the dominant magnetic minerals to significant depths before the Hellas impact event (43). The amplitudes of the magnetic anomalies yield a comparable elastic lithosphere thickness to that inferred from Hellas, but more detailed modeling of gravity, topography, and magnetics will ultimately be required to distinguish whether there existed any resolvable difference in lithospheric thermal structure between the time of Hellas basin formation and earlier.

The proposal that the hemispheric boundary scarp represents a primary structure associated with one or more major impacts (34–36) in the northern hemisphere does not receive strong support from the MOLA data, at least along those portions of the boundary not strongly affected by erosion (22). But the new topographic data do suggest that an impact in the southern hemisphere (Hellas) contributes to the boundary topography in its vicinity. The dichotomy boundary as manifest in surface geology and regional topography appears to contain three dominant contributions: (i) volcanic construction associated with Tharsis, (ii) major excavated deposits approximately circumferential to Hellas, with additional contributions from Isidis and probably Utopia ejecta, and (iii) modification of the intervening region by fluvial processes associated with the outflow channels that empty into Chryse Planitia. In addition, previously documented [for example, (35)] contributions from fracturing and resurfacing dictate that the boundary formed in response to multiple, complex mechanisms.

Polar caps and present surface volatile budget. The process that produced the low northern hemisphere occurred early in martian history. The resulting elevation difference must have dominated the transport of water on Mars throughout its history. The hemispheric elevation contrast also has played a role in the present distribution of surface volatiles, which can be quantified by the MOLA topographic model.

The largest present reservoirs of surface volatiles on Mars are the north and south polar caps (Fig. 2). Visually, the southern ice cap is smaller in extent than the northern, although the southern polar layered deposits extend farther from the ice cap and exhibit a more asymmetric distribution than their northern counterparts (19). Residual ice, which persists throughout the seasonal cycle, is much more limited in extent (an area with about one-third the diameter of the north polar cap) and is offset from the present rotational pole toward 35° to 40°E such that the pole does not fall within the residual ice deposit. The topography is highest in the south polar region within the residual ice deposits (87°S, ∼10°E), where a broad dome is present with more than 3 km of relief at one end of the cap (Fig. 8). The relief of the southern polar cap is comparable to that of the northern cap.

Figure 8

(right).Polar stereographic projection of topography from latitude 55°S to the pole.

The area of probable ice-rich material greatly exceeds the region of residual ice that is apparent from images. Support for this interpretation comes from the existence of distinctive plateau regions that correlate with layered terrain units (19), as would be expected if the layers were deposited on cratered terrain. In addition, impact craters within the plateaus share unusual geometric properties with counterparts in the north polar region (46) that are observed to have formed in an ice-rich substrate. This similarity suggests that significant portions of the south polar ice cap may be buried beneath mantling dust deposits. Third, profiles across the northern and southern caps (Fig. 9) show a striking correspondence in shape that argues for a similarity in composition and suggests that the southern cap may have a significant water ice component. The surface exposure of the residual south polar cap has been observed to display a CO2 composition (47), which led to the idea that CO2 is the dominant volatile in the southern cap. However, recent experiments on the rheology of solid CO2(48) combined with relative elevation measurements from stereo imaging (49) suggest that H2O is the more likely dominant volatile constituent of the southern cap (50), although the dust content in the deposits remains uncertain.

Figure 9

Comparison of topographic profiles of the southern (solid line) and northern (dotted line) residual ice caps across longitudes 0°E to 180°E. The gaps in the middle of the southern cap profile are due to lack of coverage poleward of 87°S. The northern profile is shifted 6.7 km upward and 1° in latitude, which makes the shapes of the two caps nearly coincident. The vertical exaggeration is 100:1.

By accounting for the possible contribution of flexure of the basal surface due to the layered deposit load (51, 52), we estimate that the south polar cap has a volume of 2 × 106 to 3 × 106 km3, and that it extends over an area of 1.44 × 106 km2(53). The average relief above the surroundings is ∼815 m. The uncertainty in the volume includes contributions from errors in the mapped surface and the interpolated polar gap, as well as in the depth of the estimated basal surface. The volume of the south polar cap load (ice plus layered deposits) is greater than that calculated for the northern cap (51). But because the thickness of dust that overlies much of the plateau cannot be determined from imaging or thermal inertia data (54), and because the amount of dust mixed with the ice cannot be distinguished from ice flow models unless the temperature of the ice is known well (55), the volatile content implied by the south polar volume must be considered only an upper limit. The correspondingly greater range of possible densities for the southern layered unit yields potentially larger deflections and flexural infill volumes than the northern cap models (51, 52), thus producing a larger uncertainty in the volume estimation (53). Combined with our previous volume estimate for the northern ice cap (51) (Table 1), we determine a total surface volatile inventory of up to 3.2 × 106to 4.7 × 106 km3, which is equivalent to a global layer of 22 to 33 m thickness. Even if it is assumed that both caps have a pure H2O composition, this range is at the low end of previous estimates of the amount of water believed to have been present early in Mars' history (56). However, the surface water may represent only a fraction of the water believed to be stored currently beneath the surface in the regolith (57). Much future work will be needed to reconcile the present surface volatile inventory with primordial estimates and with models of climatic cycling of water and mechanisms of volatile loss.

Implications for hydrological transport. The low northern hemisphere has been hypothesized as the site of an early martian ocean (58). One of the proposed “shorelines” corresponds approximately to an equipotential surface, consistent with that hypothesis (20), as is a correlation of low elevation with high topographic smoothness. Application of smoothness data to assess the possible hydrological origin of individual small occurrences of units elsewhere on Mars, however, must be done with caution and in combination with other data [see, for example, (20)]. Smoothness alone can be due to several sources, such as volcanism, as seen in the Amazonian lava flows on the southwestern flanks of Tharsis (Fig. 3).

The MOLA data reveal that there are at present, and probably for much of Mars' history, only three major closed basins that can act as sinks for the surficial flow of water or ice (Table 2); the low-lying northern plains are by far the largest of these. Its watershed, the basin along with the remaining area of the planet that would drain into it, constitutes three-quarters of Mars' surface area. The other basins are Hellas and Argyre/Solis Planum, both in the southern hemisphere.

Table 2

Mars global drainage basins.

View this table:

Hellas is much smaller in area than the northern plains, but its great depth gives it a volume that approaches that of the much shallower northern basin. Its floor has the lowest elevation on Mars. The highest closed contour is at 1250 m, at which level it breaches into the Isidis basin. However, Hellas' drainage area is relatively small. Two outflow channels empty into the basin from the east. These likely formed as a result of the interaction of groundwater or ground ice with several ancient southern hemisphere volcanic shields (19). The flat though rough (Fig. 3) nature of the basin floor can be consistent with fluvial, lacustrine, or aeolian deposition, all of which have been proposed on the basis of geological characterization of the deposits that fill central Hellas (44).

Argyre has a relatively small volume compared with Hellas but has a watershed that is just as large. The watershed breaches into Chryse Planitia through a well-developed set of flood-carved channels. The Solis Planum part of this watershed is unique in comparison with other southern hemisphere drainage centers in that it is apparently a tectonic structure rather than the result of a major impact. The Solis Planum drainage area is very shallow; the mean depth is only ∼500 m.

The COM-COF offset along the polar axis is responsible for the global-scale south-to-north transport of volatiles indicated by flow directions of outflow channels and valley networks (59), an observation supported by the global distribution of topographic gradients (Fig. 5C). Thus, if surface or near-surface water on Mars was once ubiquitous, much of it, even at high southern latitudes [such as would be liberated by basal melting (57) of an earlier and significantly thicker south polar cap], would have flowed to the northern plains. If the extended period of formation of the Tharsis province did not significantly modify regional slopes in the southern hemisphere, then Hellas and Argyre would each have collected water from about one-eighth of the planet. Hellas, with its great volume, would have been better able to absorb an influx, whereas Argyre may have breached and drained into the northern basin. Of course, water sources bear closely on the drainage. Recent images (60) indicate that many valley networks formed in response to subsurface sources rather than precipitation. The distribution of subsurface or surface sources would clearly control the water that would have been available to drain into any given area.

Some of the Valles Marineris canyons have been considered as source areas for outflow channels (61). Previous topography (62) was characterized by inconsistent gradients along the canyon floor, but these maps lacked geodetic control. MOLA topography (Fig. 10) now enables accurate calculation of floor slopes and their relation to the adjacent Chryse outflow channels. The canyon system is deepest (∼11 km) in Coprates Chasma at ∼300°E where the floor elevation is also lowest in an absolute sense (about −5 km). The increasing trough depths from the head of the canyon to Coprates superimposed on the flank of Tharsis result in a net eastward canyon-floor downward gradient of ∼0.3°. East of Coprates, however, the trough floors slope gently uphill by ∼0.03°, a gradient that is consistent over at least 1500 km. This uphill slope would present a barrier to surface water flow from Valles Marineris to the chaotic terrain and outflow channels to the northeast unless the water depth was sufficient to overcome the relief difference of ∼1 km. Local or regional tectonics (for example, rift deepening or large-scale tilting) as well as sediment infilling could explain the east-west floor gradients, and at least some of these processes could have postdated the outflow channels. However, the downhill floor gradient going westward from ∼330°E suggests that certain localized depressions could have served as source areas for water infilling of Valles Marineris.

Figure 10

Elevations within the floor of the Valles Marineris canyon system and the adjacent Chryse outflow channels. All areas not color contoured have elevations above −1.9 km.

  • * To whom correspondence should be addressed. E-mail: dsmith{at}tharsis.gsfc.nasa.gov

REFERENCES AND NOTES

View Abstract

Stay Connected to Science

Navigate This Article