Thermal Studies of Martian Channels and Valleys Using Termoskan Data
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JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 99, NO. El, PAGES 1983-1996, JANUARY 25, 1994 Thermal studiesof Martian channelsand valleys using Termoskan data BruceH. Betts andBruce C. Murray Divisionof Geologicaland PlanetarySciences, California Institute of Technology,Pasadena The Tennoskaninstrument on boardthe Phobos '88 spacecraftacquired the highestspatial resolution thermal infraredemission data ever obtained for Mars. Included in thethermal images are 2 km/pixel,midday observations of severalmajor channel and valley systems including significant portions of Shalbatana,Ravi, A1-Qahira,and Ma'adimValles, the channelconnecting Vailes Marineris with HydraotesChaos, and channelmaterial in Eos Chasma.Tennoskan also observed small portions of thesouthern beginnings of Simud,Tiu, andAres Vailes and somechannel material in GangisChasma. Simultaneousbroadband visible reflectance data were obtainedfor all but Ma'adimVallis. We find thatmost of the channelsand valleys have higher thermal inertias than their surroundings,consistent with previousthermal studies. We show for the first time that the thermal inertia boundariesclosely match flat channelfloor boundaries.Also, butteswithin channelshave inertiassimilar to the plainssurrounding the channels,suggesting the buttesare remnants of a contiguousplains surface. Lower bounds ontypical channel thermal inertias range from 8.4 to 12.5(10 -3 cal cm-2 s-1/2 K-I) (352to 523 in SI unitsof J m-2 s-l/2K-l). Lowerbounds on inertia differences with the surrounding heavily cratered plains range from 1.1 to 3.5 (46 to 147 sr). Atmosphericand geometriceffects are not sufficientto causethe observedchannel inertia enhancements.We favornonaeolian explanations of the overall channel inertia enhancements based primarily upon the channelfloors' thermal homogeneity and the strongcorrelation of thermalboundaries with floor boundaries. However,localized, dark regions within some channels are likely aeolian in natureas reported previously. Most channelswith increasedinertias have fretted morphologies such as flat floorswith steepwalls. EasternRavi and southernAres Vailes, the only major channel sections observed that have obvious catastrophic flood bedforms, do nothave enhanced inertias. Therefore, we favorfretting processes over catastrophic flooding for explainingthe inertiaenhancements. We postulatethat the inertia enhancements were caused either by the original fretting process or by a processinvolving the bondingof finesdue to an increasedavailability of water,either initially or secondarily. INTRODUCTION missions.The term channelhas beenwidely used for Mars, Enormouschannels and valleys are some of Mars' most althoughit is somewhaterroneous in itsusage [Sharp and Malin, intriguingfeatures. Most, includingthose studied here, are now 1975;Carr, 1981]. For simplicity,we usethe termchannel to generallyaccepted to have been cut by water or ice related refer collectivelyto featurespreviously classed as channelsor processes[Carr, 1981;Baker, 1982;Baker et al., 1992]. These valleys. processesprobably included catastrophic flooding and sapping processes.Studies of Martian channelsurface properties and BACKGROUND morphologiesyield importantimplications for Mars' geologic, hydrologic,and climatic history. The Termoskan Instrument and Data The SovietPhobos '88 Termoskaninstrument provided the In Februaryand March 1989 the Termoskaninstrument on highestspatial resolution thermal data obtainedso far for Mars boardthe Phobos'88 spacecraftof the USSR acquireda limited [Selivanovet al., 1989; Murray et al., 1991; Betts, 1993], set of very high spatial resolutionsimultaneous observations of includingobservations of severallarge equatorial channels and reflected solar flux and emitted thermal flux from Mars' valleys.Here we presentthe results of thefirst detailed study of equatorialregion. Theseimage panoramas cover a largeportion channelsusing the Termoskan data. We includea descriptionof of the equatorialregion from 30øS to 6øN latitude. Termoskan theinstrument and the observations, a description of thechannels was an optical-mechanicalscanning radiometer with one visible observed,a review of geologicclassifications and previous channel(0.5-1.0 g,m) and one thermal infrared channel (8.5-12.0 thermalstudies, qualitative results and implications, quantitative gm). Theinstrument was fixed to thespacecraft, pointing in the thermal inertia determinationsand implications,critiques of antisolardirection. Thus, all observationsare at 0ø phaseangle possiblehypotheses, and proposedtests using future Mars andonly daytime observations were acquired. More complete descriptionsof the Termoskaninstrument and data appearin Murray et al. [1991] andBetts [1993]. 1Nowat the San Juan Capistrano Research Institute, San Juan Capistrano, California. Termoskan'sbest resolution per pixel was 1.8 km for threeof the panoramasacquired and 300 m for the remainingpanorama Copyright1994 by the AmericanGeophysical Union. [Selivanovet al., 1989;Murray et al., 1991]. Theseresolutions are much better than thoseobtained by the Viking infrared Paper number93JE03173. thermalmapper (IRTM) (approximately5 to 170 km/pixel,with 0148-0227/94/93 JE03173505.00 onlya smallfraction of the datanear 5 km/pixel,and a typical 1983 1984 BETTS AND MURRAY: THERMAL STUDIES OF MARTIAN CHANNELS valueof 30 [Christensen,1986]). Termoskan'sspatial resolution In addition to Ravi Vallis, several other channels lead either is also better than the 3 km/pixel that was expectedfor Mars into or out of HydraoresChaos (see Figure 1). A large, flat Observer'sthermal emission spectrometer (TES), althoughTES channelenters Hydraores Chaos from Valles Marineris to the observationswould have providedglobal 1400 and 0200 local south. We will refer to this channelby the unofficial name, time(LT) spectralcoverage. HydraoresChannel. Regionsof chaoticterrain occur both to the Thermal inertia, a bulk measure of the resistance of a unit southand to the northof this channel. Anotherflat, steepwalled surfacearea to changesin temperature,is commonlyused to channel at the northwestcomer of HydraoresChaos begins characterizethe insulatingproperties of planetarysurfaces. It is Simud Vallis. Only approximately75 km of this channelwere definedasI = (kpcp)112,where kis the thermal conductivity, pis observed north of the chaos. At the northeast corner of thedensity, and c3 is thespecific heat. Low-inertia materials Hydraores Chaos, Termoskanobserved about 150 km of a exhibit the largestday-to-night temperature variation and the channel(here called Tiu West) that splitsaround a large butte. smallestthermal skin depths. We use the units for thermal This channelthen meets anotherobserved channel (here called inertia often usedfor the Martian surface[e.g., Kieffer et al., Tiu East) comingfrom HydaspisChaos to the east. When these 1977]:10 '3 calcm '2 K'1 s'it2. Thermalinertias in SI units(J m'2 setsof channelsmeet north of the Termoskancoverage area, they K'1 s '1/2) can be obtained bymultiplying by41.86. form Tiu Vallis proper. Smallportions of the headwardreaches of AresVallis were alsoobserved. Most of thispart of Aresdoes ChannelDescriptions and Geographic and Geologic Settings not show flat floors, but rather appearsscoured and is locally Termoskanobserved several large channelsnear the eastern anastomofic[Sharp and Malin, 1975]. Simud, Tiu, and Ares, end of Valles Marineris including significantportions of like ShalbatanaVallis, all debouchinto ChrysePlanifia several hundred kilometers downstream. ShalbatanaVallis, Ravi Vallis, the channelconnecting Valles Channel materials were also observed in two of the eastern Marineriswith HydraotesChaos, and channelmaterial in Eos Chasma. In the sameregion, Termoskan also observed small Valles MarinerisChasma: Eos andGangis (see Figure 1). Flow portionsof the southernbeginnings of Simud,Tiu, and Ares from theseregions presumably headed to the eastand eventually Valles as well as channelmaterial in the northernportions of northeastin the directionof HydraoresChannel and Chaos. Only GangisChasma. On the otherside of the planet,Termoskan the northernmostpart of Gangis was observed. A separate observedtwo majorvalleys in the AeolisQuadrangle: A1-Qahira Termoskanpanorama shows most of EosChasma. Both chasma Vallis and Ma'adim Vallis (see Table 1). All the channel contain flat, smooth appearingareas classifiedby Scott and sectionsobserved by Termoskancut throughancient cratered Tanaka [1986] as Hesperianchannel materials. The channel terrainof Noachianage [Scottand Tanaka,1986; Greeleyand materialsare situatednext to steepwalls, buttes,and at leastin Guest, 1987]. EosChasma, between regions of chaoticterrain. ShalbatanaVallis (see Figure 1) appearsto emanatefrom a Termoskan also observedMa'adim Vallis and A1-Qahira zone of chaotic terrain at 0øN, 46øW and heads northward.It Vallis, two isolated channels in the Aeolis qua&angle. narrowsto a low-sinuositychannel with a reasonablyuniform Termoskanobserved the northernmost(distal) 350 km of the 700 width of approximately10 km. It eventuallysplits into two km long,gently winding, 15- to 25-km-wideMa'adim Vallis. It distributaries. In all, it extendsover 1000 km. Termoskan headsnorthward until hookingnorthwest after breachinga 30-km observedapproximately the southern400 km of the channel. crater. It debouches into another 30-km crater. Ma'adim is Just to the east of Shalbatanais the 300-km-longRavi Vallis, unusuallyold for a large channel[Baker, 1982; Masurskyet al., whichalso emanates from a regionof chaoticterrain (Aromatum