Skip to content

Sojourner

Sojourner still latched to a Pathfinder lander petal on sol 1, imaged by the Imager for Mars Pathfinder. The six wheels, the flat solar panel that covers the whole deck and the deployment arrangement on the petal are visible, with a deflated airbag in the foreground NASA/JPL. Public domain (NASA / US government work).

Sojourner was delivered by the Mars Pathfinder lander on 4 July 1997, the first rover to operate on Mars [1]. Planned for seven sols, it returned data and images for 83 sols.

ParameterValueSource
Mass10.6 kg[1], [9]
Heightabout 30 cm[9]
Wheelssix, rocker-bogie suspension[1]
Instrumentsalpha proton X-ray spectrometer, three cameras[9]
ParameterValueSource
Launch4 December 1996 UTC, Cape Canaveral[9]
Landing4 July 1997, Ares Vallis[1], [9]
Planned missionseven sols[1]
Surface operations duration83 sols
Final data transmission from Pathfinder27 September 1997[9]
Linear distance traversedapproximately 100 m[1]
Surface area exploredapproximately 250 m2
Commanded rover maneuvers230
APXS in-situ elemental analyses16
Rover camera images550[1], [9]
Lander camera images16,500
Environmental measurementsapproximately 8.5 million[1]
Total mission data returnedapproximately 2.3 Gbit[1], [9]

The mission page counts more than 15 chemical analyses of rocks and soil [9] where the rover engineering report gives 16 APXS in-situ analyses [1].

Pathfinder entered the atmosphere directly, decelerated by heat shield, parachute and retrorockets, and landed inside an airbag cocoon [1]. Airbag landing is viable at this mass because the atmosphere, at a mean surface density near 0.020 kg/m3, decelerates a light entry vehicle adequately under a parachute alone [4].

The rover masses 10.6 kg on six wheels in a rocker-bogie suspension [1]. The Wheel Abrasion Experiment occupied the right center wheel of the six. The linkage keeps all six wheels loaded on uneven ground without springs or active levelling, distributing load passively as the terrain changes, and allows the vehicle to climb obstacles taller than its wheel diameter. The same geometry has been used on every subsequent NASA Mars rover.

Wheel surface speed during instrumented operation was 1 cm/s at approximately 1.2 rpm [1], a rate low enough that wheel-soil interaction is quasi-static and inertial effects in the soil do not enter. Wheel dig-in tests give the only direct in-situ measurement of surface bearing behavior from this mission: in softer soil the test wheel sank 0.6 to 0.7 cm in the first two revolutions and reached 0.8 to 1.2 cm after seven, while in harder material it reached 1.5 cm in two revolutions. Ground tests in analog soils produced depths over 3 cm [1]. The spread reflects the strength range of Martian surface materials, which run from sand at cohesion at or below 1 kPa to indurated soils near 11 kPa [3].

A solar array on the top surface supplies about 16 W, with non-rechargeable lithium batteries for short night operations [1]. Atmospheric opacity at the landing site was 0.5 during surface operations, with suspended particles of approximately 1 µm [1]. That opacity sits at the top of the background range for the aphelion half of the Martian year, so array output over the 83 sols was near its seasonal floor rather than depressed by a storm [4].

Hazard detection uses two binocular cameras and a laser ranging device [1]. Both sense geometry; neither senses soil strength, and cohesion across Martian surface types varies from at or below 1 kPa for sand to 11 kPa for indurated soil with no corresponding change in relief [3]. The rover has no direct Earth link; all communication relays through the Pathfinder lander over UHF, with telemetry at 40 bps. One-way Earth-Mars signal delay during the mission was at least ten minutes, which is what forces onboard hazard handling rather than direct teleoperation.

Operators sent waypoint goals rather than driving directly. Between waypoints the rover used laser stripe projection and a forward camera to detect and avoid hazards [1]. The dig-in results show why that is only a partial safeguard: the same seven wheel revolutions produced 0.8 to 1.2 cm of sinkage in one material and 1.5 cm in two revolutions in another, a difference in bearing behavior that no geometric sensor resolves [3]. The relay-only link also confined the rover to about 10 m from the lander.

The alpha proton X-ray spectrometer was placed against targets by backing the rover into them, returning the first in-situ measurements of Martian rock composition; 16 analyses were completed [1].

The WAE is the reason Sojourner produced a quantitative result about the abrasiveness of Martian surface material rather than only about its composition.

ParameterValue
Locationright center wheel
Substrateblack anodized, dye-impregnated aluminum strips, 25 x 120 x 0.25 mm
Metalsaluminum, nickel, platinum, resistively evaporation-deposited
Film thicknesses on one strip200, 300, 450, 700, 1000 Å
Brinell hardness of the three metalsAl 16, Pt 64, Ni 100
Sensorphotovoltaic reflectance detector
Typical run2 revolutions acquiring, 3 not, 2 acquiring; seven total
Readings per sample per revolutionfive, central reading taken as peak
Runs conducted11, totaling 39 wheel revolutions

Values from [1].

The metals bracket a hardness range: material that abrades aluminum but not nickel has a hardness between Brinell 16 and 100 [1]. In flight, aluminum wore most and wore inversely with film thickness, while platinum and nickel wore little. The limits placed on Martian dust are therefore harder than aluminum and softer than nickel.

Two experiment modes were run [1]. Rolling wear accumulated during normal driving. At intervals all wheels except the test wheel were locked to hold the rover stationary while the test wheel alone spun into the regolith, producing wear more severe than rolling and the dig-in depths quoted above.

The experiment returned a second result it was not designed for. Electrostatic charging of the wheels attracted dust onto the WAE wheel, which made reflectance interpretation problematic on many runs [1]. That the dust was attracted electrostatically constrains its grain size to somewhat smaller than 40 µm, and the observation is the first detection of electrostatic charging in the Martian environment.

ParameterValue
Detectorthree GaAs-on-Ge solar cells, 2 x 4 mm each
Package1 cm cube, 10 g mass budget
Design / actual operating temperature-50 C / -30 C
Load resistor1.26 kΩ at 0.1 percent, against a calculated maximum of 1.275 kΩ
Output voltage limit250 mV
Peak response5 pA·cm²/mW at 0 C
Short-circuit current at 40 mW/cm²196 pA
Isc temperature coefficient0.067 percent per C
Pointing tolerance±15 deg
Standoff, sample center to detector face19.2 mm
Imaged sample area1.5 x 2.5 cm
Landing load qualification60 g
Low temperature qualification-110 C, 1 h dwell
Bakeout110 C minimum, 50 h
Vacuum testbelow 1 torr, 24 h at 40 C

Values from [2].

Detector output feeds the reflectance record from which the metal film wear is read [1]. The load resistor is the design constraint that decides the whole measurement. Photocurrent at maximum illumination is 196 pA, so the resistor must be large enough to develop a readable voltage and small enough that the cell stays near short circuit; 1.26 kΩ against a calculated 1.275 kΩ maximum leaves no margin above, and the 250 mV output ceiling is what sets it [2]. Detector temperature was specified at -50 C and the flight units ran at -30 C, over which range the short-circuit current moves 0.067 percent per degree.

The detector was qualified to 60 g of landing load, to -110 C with a one hour dwell, and through a 110 C bakeout of at least 50 hours plus 24 h below 1 torr at 40 C [2]. Its viewing geometry is fixed at 19.2 mm standoff over a 1.5 by 2.5 cm sample area with a ±15 degree pointing tolerance, so alignment error translates directly into apparent reflectance change and had to be held mechanically rather than calibrated out.

QuantityValue
Mean atmospheric pressure6.7 mbar, varying 0.2 to 0.3 mbar daily
Atmospheric opacity0.5
Suspended dust particle sizeapproximately 1 µm
Precipitable water vapor0.01 mm
Maximum daytime / minimum night temperature-9 C / -76 C
Temperature sensor heights on the lander mast25, 50, 100 cm

Values from [1].

Winds were light and variable relative to the Viking sites: steady from the south at night, rotating clockwise south to west to north to east through the day [1]. Later compilation across all landed sites puts daytime wind maxima and a clockwise diurnal rotation of wind direction as the general low-latitude pattern, driven by convective mixing [4]. Dust devils were detected repeatedly from mid-morning through late afternoon, with marked temperature and pressure signatures as they passed the lander. Those figures sit inside the ranges later compiled across all landed sites, where measured air temperature spans 140 to 300 K and background column dust optical depth stays below 1 outside storm season [4].

Background column dust optical depth over the aphelion half of the Martian year sits below 1, and the opacity of 0.5 measured through these 83 sols is within that range rather than elevated by regional activity [4].

The mission returned 83 percent of a projected objective across 230 commanded maneuvers [1]. The command cycle was one uplinked plan per sol executed against onboard hazard handling, because the one-way light time exceeded ten minutes. Eleven Wheel Abrasion Experiments were run inside that cycle, each costing seven wheel revolutions and a stationary interval with five wheels locked, which is why the total across the mission is only 39 revolutions of instrumented wear [1].

The WAE strips carried five film thicknesses of each metal on one substrate, so a single run returns a wear-versus-thickness curve rather than a single wear datum, and the inverse relationship observed for aluminum is what identifies abrasion rather than contamination as the cause of the reflectance change [1].

Rocker-bogie mobility, onboard hazard avoidance from stereo plus laser ranging, and the sol-by-sol command cycle were all first flown here and are carried by every later Mars surface mission [1]. The dig-in depths it measured, 0.6 to 1.5 cm depending on material, are the earliest in-situ constraint on the bearing behavior later quantified as cohesion at or below 1 kPa for sand and up to 11 kPa for indurated soils [3].

The Wheel Abrasion Experiment established a method that has not been repeated: using the rover’s own wheel as a tribometer, with a graded set of metal films as the calibrated reference, to bracket the hardness of the surface material. It cost 10 g of detector and one modified wheel [2]. Its accidental detection of electrostatic charging, and the grain size limit that follows from it, is a result no imaging or spectroscopic instrument on the vehicle could have produced [1].

References

  1. Keith, T. G. and Siebert, M. W. (1998). Mars Pathfinder Wheel Abrasion Experiment Ground Test, and Mars Pathfinder Final Technical Report. NASA Lewis Research Center and Jet Propulsion Laboratory. Source
    BibTeX
    @techreport{keith1998mars,
      title = {Mars Pathfinder Wheel Abrasion Experiment Ground Test, and Mars Pathfinder Final Technical Report},
      author = {Keith, Theo G. and Siebert, Mark W.},
      institution = {NASA Lewis Research Center and Jet Propulsion Laboratory},
      year = {1998},
      url = {https://ntrs.nasa.gov/citations/19990013984}
    }
  2. Wilt, D. M., Ferguson, D. C. and Siebert, M. W. (1997). Photodetector Development for the Wheel Abrasion Experiment on the Sojourner Microrover of the Mars Pathfinder Mission. NASA Lewis Research Center, NASA TM-113123. Source
    BibTeX
    @inproceedings{wilt1997photodetector,
      title = {Photodetector Development for the Wheel Abrasion Experiment on the Sojourner Microrover of the Mars Pathfinder Mission},
      author = {Wilt, D. M. and Ferguson, D. C. and Siebert, M. W.},
      institution = {NASA Lewis Research Center},
      year = {1997},
      number = {NASA TM-113123},
      url = {https://ntrs.nasa.gov/citations/19980000043},
      booktitle = {IECEC-97 Proceedings of the Thirty-Second Intersociety Energy Conversion Engineering Conference (Cat. No.97CH6203)},
      doi = {10.1109/iecec.1997.659283},
      volume = {1},
      pages = {738-742}
    }
  3. Spohn, T., Hudson, T. L., Witte, L., Wippermann, T., Wisniewski, L., Kedziora, B., Vrettos, C., Lorenz, R. D., Golombek, M., Lichtenheldt, R., Grott, M., Knollenberg, J., Krause, C., Fantinati, C., Krueger, T. and Grygorczuk, J. (2022). The InSight-HP3 Mole on Mars: Lessons Learned from Attempts to Penetrate to Depth in the Martian Soil. Advances in Space Research, 8. Source
    BibTeX
    @article{spohn2022insight,
      title = {The InSight-HP3 Mole on Mars: Lessons Learned from Attempts to Penetrate to Depth in the Martian Soil},
      author = {Spohn, Tilman and Hudson, Troy L. and Witte, Lars and Wippermann, Torben and Wisniewski, Lukasz and Kedziora, Bartosz and Vrettos, Christos and Lorenz, Ralph D. and Golombek, Matthew and Lichtenheldt, Roy and Grott, Matthias and Knollenberg, Joerg and Krause, Christian and Fantinati, Cinzia and Krueger, Torsten and Grygorczuk, Jerzy},
      year = {2022},
      journal = {Advances in Space Research},
      volume = {69},
      number = {8},
      pages = {3140--3163},
      eprint = {2112.03234},
      url = {https://arxiv.org/abs/2112.03234},
      doi = {10.1016/j.asr.2022.02.009}
    }
  4. Martínez, G. M., Newman, C. N., De Vicente-Retortillo, A., Fischer, E., Renno, N. O., Richardson, M. I., Fairén, A. G., Genzer, M., Guzewich, S. D., Haberle, R. M., Harri, A.-M., Kemppinen, O., Lemmon, M. T., Smith, M. D., de la Torre-Juárez, M. and Vasavada, A. R. (2017). The Modern Near-Surface Martian Climate: A Review of In-situ Meteorological Data from Viking to Curiosity. Space Science Reviews. Source
    BibTeX
    @article{martinez2017modern,
      title = {The Modern Near-Surface Martian Climate: A Review of In-situ Meteorological Data from Viking to Curiosity},
      author = {Mart\'inez, G. M. and Newman, C. N. and De Vicente-Retortillo, A. and Fischer, E. and Renno, N. O. and Richardson, M. I. and Fair\'en, A. G. and Genzer, M. and Guzewich, S. D. and Haberle, R. M. and Harri, A.-M. and Kemppinen, O. and Lemmon, M. T. and Smith, M. D. and de la Torre-Ju\'arez, M. and Vasavada, A. R.},
      journal = {Space Science Reviews},
      volume = {212},
      pages = {295--338},
      year = {2017},
      doi = {10.1007/s11214-017-0360-x}
    }
  5. NASA. (2020). Cross-Program Design Specification for Natural Environments (DSNE), Revision G. NASA Marshall Space Flight Center. Source
    BibTeX
    @techreport{nasa2019cross,
      title = {Cross-Program Design Specification for Natural Environments (DSNE), Revision G},
      author = {NASA},
      year = {2020},
      institution = {NASA Marshall Space Flight Center},
      url = {https://ntrs.nasa.gov/citations/20200000867}
    }

Further reading

  • Cook, R. A. and Spear, A. J. (1997). Back to Mars: The Mars Pathfinder Mission. Acta Astronautica. Source
  • Bickler, D. (1997). The Mars Rover Mobility System. JPL Open Repository. Source
  • Lindemann, R., Reid, L. and Voorhees, C. (1999). Mobility Sub-System for the Exploration Technology Rover. JPL Open Repository. Source
  • (2026). NASA: Mars Pathfinder. science.nasa.gov/mission/mars-pathfinder
  • Justh, H. L., Burns, K. L., Dutta, S. and Hoffman, J. (2024). Mars Global Reference Atmospheric Model (Mars-GRAM) 2024: User Guide. NASA Marshall Space Flight Center. Source