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Zhurong beside the Tianwen-1 landing platform in Utopia Planitia, photographed by the deployable remote camera the rover placed on the ground and then drove away from. The six wheels, the four deployable solar panels and the mast are visible, as is the ramp the rover descended from the platform CNSA, via China News Service.

Zhurong is China’s first Mars rover, delivered to Utopia Planitia by the Tianwen-1 entry module and released onto the surface on 22 May 2021 [1]. Rock coverage at the Martian surface is about twice that of the Moon, which set the obstacle-clearing requirement the rover’s designers worked against. Its answer, unlike the passive rocker-bogie carried by every American Mars rover, is an active suspension that can change its own geometry on command: a main and auxiliary rocker arm linkage with a clutch that, once released, lifts a sunk wheel or contracts the whole chassis rather than relying only on wheel torque to climb out of trouble [1]. The rover operated about a year against a 90 day planned life and entered hibernation on 18 May 2022 without waking again [11].

ParameterValue
Dimensionsapproximately 3.3 x 3.2 x 1.85 m
Power sourcesolar, four deployable panels
Suspensionactive, main and auxiliary rocker arms with a releasable clutch
Payloadsix instruments

Specifications from [1]. Rover mass is not published.

ParameterValueSource
Landing15 May 2021, Utopia Planitia
Rover egress from the platform22 May 2021
Planned mission90 Martian days, completed 15 August 2021[11]
Odometer traverse to 5 May 20221921 m over 347 Martian days[11]
Reconstructed true-path traverse2009 m over 206 site operations, 360 sols[2]
Data returned by rover and orbiter to 5 May 2022about 940 gigabytes[11]
Relay test with ESA Mars ExpressNovember 2021[11]
First solar conjunction outagemid September to late October 2021[11]
Statusdid not wake from hibernation, 18 May 2022

Landing, egress and status from [1]. The 88 m gap between the 2009 m of true path reconstructed from site imagery and the 1921 m odometer reading is attributed to forward wheel slip on a generally downslope, southward traverse [2].

The suspension’s clutch, once released, converts a normally passive linkage into a commandable mechanism with four functions: controlled lifting, controlled lowering, wheel lifting, and suspension contraction [1]. That is a deliberate departure from the JPL rocker-bogie lineage, which excludes springs and active joints altogether because an elastic or actuated link raises the normal force on a climbing wheel while unloading the others, exactly wrong for obstacle climbing on a passive chassis [12]. That design was tuned against six or seven modeled obstacle positions, where six wheels climb an axle-high vertical face at a friction coefficient near 0.8 against 0.78 to 1.4 for four wheels depending on which end meets the wall, a fixed-geometry optimum Zhurong’s clutch trades away [12]. Zhurong trades that climbing optimality for a self-extraction capability the passive linkage cannot offer.

Failure conditionRecovery action
Single wheel sunklift that wheel
All wheels caughtcontract the suspension
Body in contact with a rockraise the suspension to clear it

Recovery actions from [1].

Suspension contraction with sequential wheel lifting produces a walking gait that extracts the vehicle from soft ground by changing which wheels carry load rather than by increasing drawbar pull. That addresses slip-sinkage directly: a wheel that is unloaded and repositioned does not have to develop thrust against soil whose shear strength has already been exceeded, the same failure mode a rigid rocker-bogie has no recourse against beyond driving through it [12]. Terrain along the traverse at Utopia Planitia is flat, covered by reddish soils and dust, with dark-toned material exposed where wheels or wind removed the dust layer [3].

Localization during the traverse combined onboard dead reckoning with cross-site visual matching: dead reckoning against a HiRISE-visible rover track carried an error of 3.11 percent of traverse length, cross-site Affine-SIFT visual localization reduced that to 1.75 percent, and matching site imagery to orbital imagery at four waypoints reduced it further to 0.50 percent [2]. Site digital elevation and orthophoto models were built at 0.02 m grid spacing out to 15 m range, with total stereo measurement error of 0.108 m at that range [2].

Solar radiation intensity at Mars orbit is approximately 43 percent of that near Earth [1]. Atmospheric dust adds to that deficit: background column optical depth over the aphelion half of the year sits below 1, and dust storm activity recurs seasonally, so array output carries a seasonal floor independent of surface deposition on the panels themselves [7], [8]. Two measures respond to the combined problem. Maximum power point tracking improves conversion efficiency from the cells, and an ultra-thin solar film with an anti-dust coating gives a dust removal efficiency over 86 percent, addressing deposition rather than the seasonal atmospheric floor [1].

A dormancy and wake-up mode covers the range of surface lighting conditions. On the onset of a dust storm the rover powers off to prevent battery drain and remains asleep until generated power and temperature reach their thresholds simultaneously, a coupling that makes the mode a survival state rather than a low-power state [1]. During a global dust storm, column optical depth reaches a global mean near 4 with local values of 5 to 10, so a storm subtracts from generation at the same time as it adds to deposition on the arrays [8]. The dust climatology behind that figure was itself validated against independent measurements from CRISM in orbit and from PanCam and Mini-TES on the ground, which is why it is used as the dust forcing in the Mars Climate Database [8].

Surface temperature below -100 C sets the design case [1]. Measured air temperature at landed Mars sites spans roughly 140 to 300 K depending on season and latitude, with a diurnal range large enough that a surface vehicle crosses most of that span every sol [7]. At Gale crater, the diurnal amplitude of the ground temperature cycle runs on a thermal inertia of roughly 170 to 550 SI units depending on terrain, the same site-dependence that makes any fixed thermal design a compromise across a traverse [7]. The architecture combines active and passive control.

ElementFunction
Solar windowcollects heat during the day, raises cabin temperature at night
Aerogel plus CO2 isolationpassive insulation: reduces conduction, isolates radiative leakage, eliminates in-cabin convection
Active heating at nightbrings in-cabin equipment to its required ambient temperature
Active control on external equipmentnavigation and obstacle avoidance cameras, multispectral cameras

Thermal elements and their functions from [1].

The passive layer is what makes the active budget affordable: with limited active thermal resources, leakage is attacked on all three transfer paths at once rather than compensated by heater power [1]. That approach to the cold is not the only one flown to Mars: the InSight HP3 mole, a hammering probe rather than a thermally isolated cabin, failed to reach its planned depth because the cohesive duricrust at its site gave no lateral soil pressure and therefore no hull friction to react the hammer’s recoil, a soil-mechanical failure mode with no counterpart in Zhurong’s cabin-insulation design [9].

LinkParameterValue
X-band directRover-to-Earth visible arcapproximately M04:30 to M16:00 each sol
X-band directUplink rate to the omnidirectional antennaas low as 7.8125 bps
UHF relayArchitectureloop relay mode, two-way, through the Tianwen-1 orbiter
UHF relayNear-Mars arc pass around noonapproximately 10 min
UHF relayMartian night passapproximately 5 h
UHF relayNear-Mars arc rateMbps class

Link parameters from [1]. The 7.8125 bps direct uplink is a command channel, not a data path, so the relay carries everything of volume: telemetry, images and instrument data, all within the same near-Mars pass. The orbiter’s own magnetometer, MOMAG, continued returning solar wind and interplanetary magnetic field data through the relay period, cataloging two coronal mass ejections and three stream interaction regions at Mars between November and December 2021 in coordination with NASA’s MAVEN [10]. Each event’s magnetic field measurements were compared directly between the two spacecraft rather than merged, since Tianwen-1 orbits Mars while MAVEN samples the solar wind further out, and the two records agree on timing even where local field magnitude differs [10].

The rover is in standby by default, with computers on and other equipment operating intermittently against a mission cycle template run onboard [1]. Standby rather than sleep is affordable because the passive thermal stack holds cabin temperature without continuous heater draw.

IntervalAction
Martian afternoon, approx 10 hX-band omnidirectional receiver on, holding a basic uplink channel
Martian noon, approx 1 hUHF receiver on for the near-Mars arc
Martian night, approx 5 hUHF receiver on for the remote arc
M11:00 to M15:00primary work period, ambient temperature highest and no additional heating needed

Daily template from [1].

Scheduling the work period against temperature rather than against illumination is a direct consequence of the thermal budget: heating an actuator costs energy the arrays would otherwise deliver to the activity itself.

Delayed instructions are uplinked each Martian morning via the orbiter, relayed to the rover by UHF around noon for execution, and telemetry is returned through the orbiter by UHF during the Martian night [1]. The cycle is therefore one command load per sol with a single execution window and a single return window, rather than the multiple tactical passes available to the NASA rovers through the Mars Relay Network [2].

Six instruments are carried [1]. Four measure the environment rather than the rover’s own state, and the meteorology package is the Chinese counterpart to REMS and MEDA [7].

InstrumentMeasurementSource
Navigation camerasurface morphology, driving
Multispectral cameramineral and rock types, material distribution
Subsurface detection radarsoil structure and stratification, water and ice content
Surface composition detector (MarSCoDe)LIBS for quantitative chemistry, short-wave infrared spectroscopy for mineralogy[5]
Magnetic field detectormagnetic field intensity, variation, ionospheric current
Meteorological instrumentstemperature, pressure, wind speed and direction, sound

Instrument list from [1] unless noted.

MarSCoDe’s laser is a passively Q-switched 1064 nm unit at 23 mJ per 4.5 ns pulse, firing at 1 to 3 Hz with fixed energy, feeding a 106 mm Ritchey-Chretien telescope that both focuses the beam and collects the plasma emission, pointed by a worm-gear mechanism driven by two stepping motors [5]. Emission is dispersed across three LIBS channels covering 240 to 340, 340 to 540 and 540 to 850 nm, while a short-wave infrared channel covers 850 to 2400 nm [5]. Because the rover is solar powered and cannot keep the spectrometer at a constant temperature, its spectra drift with Martian temperature; the instrument carries an onboard titanium calibration target, and an elastic particle swarm optimization algorithm matches the shifted spectral lines against a standard wavelength set established in a Mars simulation chamber before launch, cutting the residual wavelength error after correction to under 0.006 nm at the ultraviolet channel’s coldest tested point of -40 C [6]. That correction was validated in a Mars simulation environment chamber holding Earth-lab pressure near 1 percent of Earth’s own and temperatures from -40 to 30 C, using standard element lamps for the initial calibration and the onboard target for the temperature-shift correction itself [6].

MarSCoDe measured LIBS and short-wave infrared spectra of six Vastitas Borealis Formation targets, soils, an outcrop and a coherent rock, in the rover’s first 300 sols, and the result reads as a low-alteration mix of igneous minerals with clay-like alteration phases formed under limited or ephemeral water and cold conditions [3]. The magnetometer campaign returned vector measurements at 16 sites along a 1089 m track; the field measured, under 10 nT over most of the track, is far weaker than the roughly 81 nT that downward-continued orbital models had predicted for the site, though InSight measured about 2000 nT at Elysium Planitia, so the discrepancy is a local rather than a universal one [4]. Separating that faint ambient field from the roughly 10,000 nT generated by a permanent magnet inside the rover’s own mast-mounted camera required rotating the mast and the whole rover to isolate sensor-frame, rover-frame and Mars-frame components of the reading [4].

Zhurong entered hibernation on 18 May 2022 and did not re-establish contact [2]. Dust accumulation on the arrays is the assumed cause, against an 86 percent dust removal efficiency demonstrated for the coating and a wake logic requiring both power and temperature thresholds to be met at once [1]. Removal of deposited dust by wind requires a surface shear stress at or above the saltation threshold, which is not a schedulable event, and the storm conditions that would generate that stress are the same conditions that raise column optical depth and cut array output at the same time [8].

The active suspension is the one mobility capability on Mars that no NASA rover has carried. Its value is not obstacle clearance, which a passive rocker-bogie already provides by design [12], but a recovery mode that does not depend on developing more thrust: lifting a sunk wheel, or contracting the whole suspension, changes the load distribution instead of demanding more shear from soil that has already failed. The thermal architecture pairs a passive stack that attacks conduction, radiation and convection simultaneously with a solar window that stores daytime heat for night use, converting part of the survival heating load from an electrical draw into a thermal one. MarSCoDe’s onboard particle-swarm wavelength recalibration is a narrower but transferable lesson: an instrument that cannot be thermally stabilized on a solar-powered platform can still hold calibration by matching against a known target rather than by controlling its own temperature [6].

Rover mass, the exact panel count beyond what is visible in imagery, and a definitive account of the wake failure, dust accumulation versus a hardware fault, remain unpublished. The magnetometer discrepancy between ground and orbital field estimates is attributed to demagnetization at either the scale of the whole Utopia Basin or of the smaller ghost crater the rover landed in, and neither is ruled out [4].

References

  1. Tian, H., Zhang, T., Jia, Y., Peng, S. and Yan, C. (2021). Zhurong: Features and mission of China's first Mars rover . The Innovation, 3. Source
    BibTeX
    @article{tian2021zhurong,
      title = {Zhurong: Features and mission of China's first Mars rover},
      author = {Tian, He and Zhang, Tianyi and Jia, Yang and Peng, Song and Yan, Chuliang},
      journal = {The Innovation},
      volume = {2},
      number = {3},
      pages = {100121},
      year = {2021},
      doi = {10.1016/j.xinn.2021.100121},
      abstract = {On May 22, 2021, at 10:40 am (Beijing Time), China’s Zhurong rover successfully reached the Mars surface and began its exploration. China is only the second nation to have conducted a successful soft landing and exploration of the red planet. The Mars probe consists of an orbiter and landing rover. The spacecraft includes an entry module consisting of a back shell, landing platform, and outsole, as well as a rover (Figure 1). Before release, the orbiter, which carries the landing rover, completed the Earth–Mars orbital transfer and an orbit reduction maneuver.}
    }
  2. Wan, W., Wang, J., Liu, Z., Di, K., Peng, M., Wang, Y., Liu, B., Hu, G., Han, S., Li, X., Yu, T., Li, L. and Liu, C. (2025). Visual Localization and Topographic Mapping for Zhurong Rover in Tianwen-1 Mars Mission . IEEE Journal of Selected Topics in Applied Earth Observations and Remote Sensing. Source
    BibTeX
    @article{wan2025visual,
      title = {Visual Localization and Topographic Mapping for Zhurong Rover in Tianwen-1 Mars Mission},
      author = {Wan, Wenhui and Wang, Jia and Liu, Zhaoqin and Di, Kaichang and Peng, Man and Wang, Yexin and Liu, Bin and Hu, Guolin and Han, Shaojin and Li, Xin and Yu, Tianyi and Li, Lichun and Liu, Chuankai},
      journal = {IEEE Journal of Selected Topics in Applied Earth Observations and Remote Sensing},
      volume = {18},
      pages = {6393--6408},
      year = {2025},
      doi = {10.1109/jstars.2025.3540377},
      abstract = {This article presents the methods, results, and applications of visual localization and topographic mapping for the Zhurong rover in China's Tianwen-1 Mars mission. New techniques, namely vignette correction and online camera mast calibration, were developed for the images captured by the rover's navigation and terrain cameras (NaTeCam) to enhance the mapping qualities. During surface operations, photogrammetric techniques were routinely applied at the traveling waypoints. The NaTeCam images were obtained to generate 3-D topographic mapping products at the centimeter level to support obstacle analysis and rover path planning. Cross-site visual localization at adjacent waypoints was conducted to reduce the accumulated position errors in the onboard dead-reckoning result. Visual localization refinement was also employed by matching the digital orthophoto map (DOM) from the rover images and the orbital basemap at waypoints where distinct terrain features were available to further eliminate the localization errors. Compared with the reference rover traverse extracted from a high-resolution imaging science experimental image in which the actual rover track is visible, the accuracies of the rover traverses generated from cross-site visual localization and DOM matching refinement are estimated to be 1.75% and 0.50% of the traverse length. The actual total traverse length is 2009 m, which is 88 m longer than 1921 m from the odometer reading, revealing a forward wheel slipping caused by the downslope trend of the southward traverse. The visual localization and topographic mapping results of the Zhurong rover have greatly supported the surface exploration planning, object approaching, and scientific investigations in the mission.}
    }
  3. Liu, Y., Wu, X., Zhao, Y.-Y. S., Pan, L., Wang, C., Liu, J., Zhao, Z., Zhou, X., Zhang, C., Wu, Y., Wan, W. and Zou, Y. (2022). Aqueous alteration of the Vastitas Borealis Formation at the Tianwen-1 landing site . Communications Earth & Environment, 280. Source
    BibTeX
    @article{liu2022aqueous,
      title = {Aqueous alteration of the Vastitas Borealis Formation at the Tianwen-1 landing site},
      author = {Liu, Y. and Wu, Xiaofeng and Zhao, Y.-Y. S. and Pan, Lu and Wang, C. and Liu, J. and Zhao, Zhiyuan and Zhou, X. and Zhang, Chi and Wu, Y. and Wan, Wenhui and Zou, Yongliao},
      journal = {Communications Earth & Environment},
      volume = {3},
      number = {280},
      year = {2022},
      doi = {10.1038/s43247-022-00614-3},
      abstract = {Abstract The Vastitas Borealis Formation is a Hesperian-aged sedimentary unit that mainly covers the Martian northern plains. Its environment of formation is uncertain but may be related to an ancient Martian ocean, outflow channel deposits, compaction and drainage activities, or subsurface ice-related processes. Here we investigate the geological evolution of the Vastitas Borealis Formation using geochemical and mineralogical data acquired by the Mars Surface Composition Detector on board the Zhurong rover at the Tianwen-1 landing site. We find that the fine-grained soil is very similar to the ubiquitous surface dust at other landing sites on Mars but mixed with calcium-rich and magnesium-poor local materials. These materials are mostly igneous minerals mixed with allophane and imogolite/opal and appear to have a low degree of chemical alteration. We suggest that these deposits likely formed by alteration of extensive volcaniclastic soils in limited or ephemeral water under cold conditions, which largely supports the hypotheses of a frozen ocean and sublimation.}
    }
  4. Du, A., Ge, Y., Wang, H., Li, H., Zhang, Y., Luo, H., Huang, C., Shan, L., Han, F., Liu, Y., Zou, Y., Wang, C., Pan, Y., Liu, Q., Mitchell, R. N., Jia, Y., Chen, B., Jin, S., Jiang, Y., Zhang, T., Zhu, R., Gubbins, D. and Zhang, K. (2023). Ground magnetic survey on Mars from the Zhurong rover . Nature. Source
    BibTeX
    @article{du2023ground,
      title = {Ground magnetic survey on Mars from the Zhurong rover},
      author = {Du, Aimin and Ge, Yasong and Wang, Huapei and Li, Haiying and Zhang, Ying and Luo, Hao and Huang, Can and Shan, Lican and Han, Fei and Liu, Yang and Zou, Yongliao and Wang, Chi and Pan, Yongxin and Liu, Qingsong and Mitchell, Ross N. and Jia, Yang and Chen, Baichao and Jin, Shengyi and Jiang, Yi and Zhang, Tielong and Zhu, Rixiang and Gubbins, David and Zhang, Keke},
      journal = {Nature},
      volume = {7},
      pages = {1037--1047},
      year = {2023},
      doi = {10.1038/s41550-023-02008-7},
      abstract = {Abstract Mars’ magnetic field has been measured at large scale by orbiting spacecraft and at very small scale via Martian meteorites. Here we report on a ground magnetic survey on metre to kilometre scales. The Zhurong rover made vector measurements at 16 sites along a 1,089 m track in the Utopia Basin on Mars. It recorded an extremely weak magnetic field, with an order of the average intensity less than that inferred from orbit, in contrast to the large magnetic field in Elysium Planitia measured by InSight. A spacecraft measurement samples an area with radius comparable to its altitude, while a ground measurement samples an area with radius comparable to the depth of the magnetized body. The weak magnetic field measured by Zhurong indicates no magnetization anomalies for a depth of many kilometres around and below the rover’s traverse. We suggest two possible explanations for the weak magnetic field: the entire Utopia Basin may have remained unmagnetized since its formation about 4 billion years ago or that the 5-km-radius ghost crater where Zhurong landed may have been been demagnetized by impact.}
    }
  5. Wan, X., Li, C., Wang, H., Xu, W., Jia, J., Xin, Y., Ma, H., Fang, P. and Ling, Z. (2021). Design, Function, and Implementation of China's First LIBS Instrument (MarSCoDe) on the Zhurong Mars Rover . Atomic Spectroscopy, 6. Source
    BibTeX
    @article{wan2021design,
      title = {Design, Function, and Implementation of China's First LIBS Instrument (MarSCoDe) on the Zhurong Mars Rover},
      author = {Wan, Xiong and Li, Chenhong and Wang, Hongpeng and Xu, Weiming and Jia, Jianjun and Xin, Yingjian and Ma, Huanzhen and Fang, Peipei and Ling, Zongcheng},
      journal = {Atomic Spectroscopy},
      volume = {42},
      number = {6},
      pages = {292--299},
      year = {2021},
      doi = {10.46770/as.2021.608}
    }
  6. Wan, X., Yuan, R., Wang, H., Cheng, Y., Jia, J., Shu, R., Xu, W., Li, C., Xin, Y., Ma, H., Fang, P. and Ling, Z. (2021). Elastic Particle Swarm Optimization for MarSCoDe Spectral Calibration on Tianwen-1 Mars Rover . Journal of Guidance, Control, and Dynamics, 22. Source
    BibTeX
    @article{wan2021elastic,
      title = {Elastic Particle Swarm Optimization for MarSCoDe Spectral Calibration on Tianwen-1 Mars Rover},
      author = {Wan, Xiong and Yuan, Rujun and Wang, Hongpeng and Cheng, Yulong and Jia, Jianjun and Shu, Rong and Xu, Weiming and Li, Chenhong and Xin, Yingjian and Ma, Huanzhen and Fang, Peipei and Ling, Zongcheng},
      journal = {Journal of Guidance, Control, and Dynamics},
      volume = {93},
      number = {22},
      pages = {7970-7977},
      publisher = {American Chemical Society (ACS)},
      year = {2021},
      doi = {10.1021/acs.analchem.1c00832}
    }
  7. 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 = {Martínez, G. M. and Newman, C. N. and De Vicente-Retortillo, A. and Fischer, Erik and Renno, N. O. and Richardson, Mark I. and Fairén, A. G. and Genzer, Maria and Guzewich, Scott D. and Haberle, R. M. and Harri, Ari-Matti and Kemppinen, Osku and Lemmon, Mark T. and Smith, Michael D. and de la Torre-Juárez, M. and Vasavada, Ashwin R.},
      journal = {Space Science Reviews},
      volume = {212},
      pages = {295--338},
      year = {2017},
      doi = {10.1007/s11214-017-0360-x},
      abstract = {We analyze the complete set of in-situ meteorological data obtained from the Viking landers in the 1970s to today’s Curiosity rover to review our understanding of the modern near-surface climate of Mars, with focus on the dust, CO 2 and H 2 O cycles and their impact on the radiative and thermodynamic conditions near the surface. In particular, we provide values of the highest confidence possible for atmospheric opacity, atmospheric pressure, near-surface air temperature, ground temperature, near-surface wind speed and direction, and near-surface air relative humidity and water vapor content. Then, we study the diurnal, seasonal and interannual variability of these quantities over a span of more than twenty Martian years. Finally, we propose measurements to improve our understanding of the Martian dust and H 2 O cycles, and discuss the potential for liquid water formation under Mars’ present day conditions and its implications for future Mars missions. Understanding the modern Martian climate is important to determine if Mars could have the conditions to support life and to prepare for future human exploration.}
    }
  8. Montabone, L., Forget, F., Millour, E., Wilson, R. J., Lewis, S. R., Cantor, B. A., Kass, D., Kleinböhl, A., Lemmon, M. T., Smith, M. D. and Wolff, M. J. (2015). Eight-year Climatology of Dust Optical Depth on Mars . Icarus. Source
    BibTeX
    @article{montabone2015eight,
      title = {Eight-year Climatology of Dust Optical Depth on Mars},
      author = {Montabone, L. and Forget, Francois and Millour, Ehouarn and Wilson, R. J. and Lewis, Stephen R. and Cantor, B. A. and Kass, D. and Kleinböhl, A. and Lemmon, Mark T. and Smith, Michael D. and Wolff, M. J.},
      journal = {Icarus},
      volume = {251},
      pages = {65--95},
      year = {2015},
      doi = {10.1016/j.icarus.2014.12.034}
    }
  9. 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},
      journal = {Advances in Space Research},
      volume = {69},
      number = {8},
      pages = {3140--3163},
      year = {2022},
      doi = {10.1016/j.asr.2022.02.009},
      abstract = {The NASA InSight lander mission to Mars payload includes the Heat Flow and Physical Properties Package HP3 to measure the surface heat flow. The package was designed to use a small penetrator - nicknamed the mole - to implement a vertical string of temperature sensors in the soil to a depth of 5 m. The mole itself is equipped with sensors to measure a thermal conductivity-depth profile as it proceeds to depth. The heat flow is calculated from the product of the temperature gradient and the thermal conductivity. To avoid the perturbation caused by annual surface temperature variations, the measurements need to be taken at a depth between 3 m and 5 m. The mole is designed to penetrate cohesionless soil similar in rheology to quartz sand which is expected to provide a good analogue material for Martian sand. The sand would provide friction to the buried mole hull to balance the remaining recoil of the mole hammer mechanism that drives the mole forward. Unfortunately, the mole did not penetrate more than 40 cm, roughly a mole length. The failure to penetrate deeper is largely due to a cohesive duricrust of a few tens of centimeter thickness that failed to provide the required friction. Although a suppressor mass and spring as part of the mole hammer mechanism absorb much of the recoil, the available mass did not allow designing a system that fully eliminated the recoil. The mole penetrated to 40 cm depth benefiting from friction provided by springs in the support structure from which it was deployed and from friction and direct support provided by the InSight Instrument Deployment Arm. In addition, the Martian soil provided unexpected levels of penetration resistance that would have motivated designing a more powerful mole. The low weight of the mole support structure was not sufficient to guide the mole penetrating vertically. Roughly doubling the overall mass of the instrument package would have allowed to design a more robust system with little or no recoil, more energy of the mole hammer mechanism and a more massive support structure. In addition, to cope with duricrust a mechanism to support the mole to a depth of about two mole lengths should be considered.}
    }
  10. Chi, Y., Shen, C., Cheng, L., Yu, B., Miao, B., Wang, Y., Zhang, T., Zou, Z., Xu, M., Pan, Z., Su, Z., Guo, J., Mao, D., Zhong, Z., Zhang, Z., Liu, J., Wang, C., Wu, Z., Wang, G., Xiao, S., Liu, K., Hao, X., Li, Y., Chen, M. and Du, Y. (2023). Interplanetary Coronal Mass Ejections and Stream Interaction Regions observed by Tianwen-1 and Maven at Mars . The Astrophysical Journal Supplement Series. Source
    BibTeX
    @article{chi2023interplanetary,
      title = {Interplanetary Coronal Mass Ejections and Stream Interaction Regions observed by Tianwen-1 and Maven at Mars},
      author = {Chi, Yutian and Shen, Chenglong and Cheng, Long and Yu, Bingkun and Miao, Bin and Wang, Yuming and Zhang, Tielong and Zou, Zhuxuan and Xu, Mengjiao and Pan, Zonghao and Su, Zhenpeng and Guo, Jingnan and Mao, Dongwei and Zhong, Zhihui and Zhang, Zhiyong and Liu, Junyan and Wang, Can and Wu, Zhiyong and Wang, Guoqiang and Xiao, Sudong and Liu, Kai and Hao, Xinjun and Li, Yiren and Chen, Manming and Du, Yang},
      journal = {The Astrophysical Journal Supplement Series},
      volume = {267},
      pages = {3},
      year = {2023},
      doi = {10.3847/1538-4365/acd191},
      abstract = {Abstract The Tianwen-1 spacecraft is China's first Mars exploration mission. The Mars Orbiter Magnetometer (MOMAG) is a scientific instrument on board the Tianwen-1 mission that is designed to study magnetic fields at Mars, including the solar wind to the magnetosheath and the ionosphere. Using the first Tianwen-1/MOMAG data that is publicly available, we present an interplanetary coronal mass ejection (ICME) and stream interaction region (SIR) list based on in situ observations at Mars between 2021 November 16 and 2021 December 31. We compared the magnetic field intensity and vector magnetic field measurements from Tianwen-1/MOMAG and Mars Atmospheric Volatile EvolutioN (MAVEN)/Magnetometer (MAG) during the ICME and SIR interval and found a generally good consistency between them. Due to MAVEN's orbital adjustment since 2019, the Tianwen-1/MOMAG instrument is almost unique in its status as an interplanetary magnetic field monitor currently at Mars. The observations indicate that the MOMAG instrument on Tianwen-1 is performing well and can provide accurate measurements of the vector magnetic field in the near-Mars solar wind space. The multipoint observations combining MOMAG, MINPA, and MEPA on board Tianwen-1 with MAG, SWIA, and STATIC on board MAVEN will help develop systematic studies of the characteristics of ICMEs and SIRs at Mars, and their influences on the Martian atmosphere and ionosphere.}
    }
  11. (2026). CNSA: Tianwen-1 mission marks 1st year on Mars. cnsa.gov.cn/english/n6465652/n6465653/c6840321/content.html
    BibTeX
    @misc{cnsatianwen,
      title = {CNSA: Tianwen-1 mission marks 1st year on Mars},
      organization = {cnsa.gov.cn},
      year = {2026},
      url = {https://www.cnsa.gov.cn/english/n6465652/n6465653/c6840321/content.html}
    }
  12. Bickler, D. B. (1997). The Mars Rover Mobility System . JPL Open Repository. Source
    BibTeX
    @inproceedings{bickler1997mars,
      title = {The Mars Rover Mobility System},
      author = {Bickler, Donald B.},
      publisher = {JPL Open Repository},
      year = {1997},
      url = {https://dataverse.jpl.nasa.gov/dataset.xhtml?persistentId=hdl:2014/18908}
    }

Further reading