NASA JSC Active Response Gravity Offload System
ARGOS is the gravity offload facility at NASA JSC: an overhead bridge crane carrying a motor-driven cable that holds a constant upward force on a test article while following it through the workspace, so the article moves as though it weighed a lunar, Martian or microgravity fraction of its Earth weight [1][4]. Three translational axes are actively driven, which is the difference between it and the earlier Pogo rig described on the reduced gravity testing page, and the reason it can be used for walking rather than only for standing tasks [2].
It offloads at one point. Everything the following sections say about fidelity follows from that: the cable knows the total weight it is holding, and nothing about how the mass is distributed across the limbs beneath it [3].
Every number in the capability table is the operator’s stated specification. Nothing published reports a measured offload force accuracy, a bandwidth, a residual horizontal force or a cable angle error against an independent reference [1][4].
Laboratory data
Section titled “Laboratory data”| Parameter | Value |
|---|---|
| Operator | NASA JSC [4] |
| Location | Houston, Texas, United States [4] |
| Commissioned | Third iteration of the system as described in 2017; earlier dates not published [1] |
| Type | Active cable gravity offload rig, human rated and two fault tolerant [1] |
| Floor area | Bridge crane structure 41 x 24 x 25 ft (12.5 x 7.3 x 7.6 m) [4] |
| Capabilities | Offload envelope, gimbals |
| Simulant or terrain | None installed. Terrain is brought in by the test [1] |
| Instrumentation | Displacement and force sensing on X, Y and Z; AIBEL motion tracking [4] |
| Ground truth | Not published. No independent verification of delivered offload is reported [1][4] |
| Fidelity limits | Single attachment point; limbs stay at 1 g; three rotations passive [2][3] |
| Access | Test support offered through the JSC analogs and mockups program; no lead time published [4] |
| Cited by | Robonaut 2 [5] |
Capabilities
Section titled “Capabilities”Offload envelope
Section titled “Offload envelope”| Parameter | Value |
|---|---|
| Working volume | Over 340 m3: 11.0 m Y, 5.8 m X, 5.5 m working height [1] |
| Test article limits | 340 kg (750 lb) payload [1][4] |
| Vacuum | None. Ambient pressure in a high bay [1] |
| Temperature | Not controlled. Breathing air and suit cooling water are supplied [4] |
| Illumination | Not published. No solar simulator |
| Slope | Not applicable. Terrain is whatever the test brings in |
| Gravity offload | Vertical, at one point, set in software from 1 g to microgravity [1][4] |
| Instrumentation | Redundant sensors, real-time safety model, independent overspeed detection [1] |
Speed and acceleration trade against payload mass: 3.3 m/s and 24.4 m/s2 at 140 kg, falling to 1.4 m/s and 10.2 m/s2 at 340 kg [1]. A separate horizontal-system maximum of 2.0 m/s and 6.1 m/s2 is quoted alongside those figures without being reconciled with them [1]. The operator’s own catalog gives the limits in the form a test director needs, as tracking rates by configuration: 4 ft/s vertical and 6.5 ft/s horizontal with a suited subject, 11 ft/s vertical and 6.5 ft/s horizontal unsuited [4]. Motion faster than that is outside the offload envelope, which is a constraint on the task, not on the rig.
Vertical offload load sensitivity is quoted as below 0.0005 kg, and horizontal tracking sensitivity as under 0.1 degree of cable angle, both without a bandwidth, a condition or a measurement method [1]. Safety faults are detected in under 20 ms with two fault tolerance, and a lifting cable device limits the shock load into the payload during a high-speed stop [1].
The two published descriptions disagree on the workspace. The 2017 description gives 11.0 by 5.8 m at 5.5 m height, over 340 m3 [1]; the operator’s catalog gives 13 by 30 by 15 ft, about 4.0 by 9.1 by 4.6 m or 167 m3, inside the 41 by 24 by 25 ft crane structure [4]. Neither states which convention it uses, and the difference is a factor of two in usable volume, so a test that needs the full run length should confirm it with the facility rather than from either number here.
Gimbals
Section titled “Gimbals”| Parameter | Value |
|---|---|
| Working volume | Not applicable. The gimbal is the payload interface |
| Test article limits | Suited, unsuited and unmanned interfaces available [4] |
| Actively controlled axes | Three translations. The three rotations are passive [2] |
| Instrumentation | Center of gravity board with four-corner force transducers, for pivot setup [3] |
Roll is limited to about 30 degrees by the parallelogram linkage and pitch by interference with the subject [2]. Gimbal mass is a facility variable with a measurable effect: replacing the 105 lb all-metal claw gimbal with a 53 lb gimbal adapted from EMU and MkIII suit hardware measurably improved subject-rated simulation quality, the lower mass and inertia being the stated cause [2].
What it does not reproduce
Section titled “What it does not reproduce”The limbs. The gimbal attaches at a single point on the portable life support system mockup, so arms and legs move against full 1 g. It is worst in prone postures, where the entire lower torso lies outside the offloading cable region [3]. Any result about limb effort in a suited task at ARGOS is a 1 g limb result. This is a fidelity limit stated by the operators, not a measurement of the error it causes, and no published source quantifies it.
Gait timing. Suited walking at 1/6 g offload gave a 50/50 swing and stance split, the same as 1 g unsuited ground walking, but the mid-swing point occurred 10 percent earlier and the cause was not established [2]. Different subjects were used in the two environments, so the comparison is not paired.
A pivot point that does not have to be tuned. Across 68 configurations and 14 xEMU subjects of 175.1 +/- 8.4 cm stature in lunar offload, the functional zone for the gimbal pivot is 2.5 to 6.4 cm above and 1.3 to 2.5 cm aft of the system center of gravity [3]. Suited subjects notice fore-aft shifts as small as 0.6 cm, while up-down shifts of 2.5 cm produce minimal performance difference [3]. A simulation run without that tuning is measuring the rig. Setup uses a center of gravity board with four-corner force transducers and the hard upper torso hatch angle: standing neutral came out at 58 to 62 degrees from vertical, standing tip-over at 47 to 52 degrees, one-knee kneeling tip-over at 15 to 27 degrees, with a standing sway range of 0.5 to 8.5 in and a static center of pressure offset of 3 to 3.5 in [3].
Soil. The rig offloads the test article. The ground beneath it stays at 1 g, so a mobility or excavation result taken here inherits terrain stronger than the destination’s [1]. The reasoning is on the reduced gravity testing page.
Duration is the thing it does reproduce. Against a parabolic aircraft, which gives the highest offload fidelity of the analogs but only about 30 s per parabola in a constrained cabin volume, ARGOS trades fidelity for unlimited run time [2]. Against Pogo, which drove only two axes and carried significant overhead inertia from the lifting mechanism, it trades mechanism complexity for a third driven axis [2].
Campaigns run there
Section titled “Campaigns run there”Robonaut 2 with climbing legs, 2014. A nearly 300 kg two-legged Robonaut 2 configuration placed its end effector to under 1 cm of error over a reach of more than 1 m, with both legs stiff at a natural frequency of 20 and a damping ratio of 1.2, base leg joint torque limited to 100 and reaching leg to 20 in units the source does not state, and the embedded impedance loop integrator enabled [5]. The result carries the facility’s own limit: only the base leg was effectively offloaded, so the reaching leg worked against 1 g [5].
xEMU pivot point characterization, reported 2023 [3]. The 68-configuration study above is a campaign about the facility rather than about a test article, and it is an unusual thing for an offload rig to publish. One dedicated run tested 10 pivot settings on a single experienced subject in a day [3].
Suited lunar gait measurement, reported 2020. Inertial measurement units mounted on the exterior of a Mark III suit recorded the swing and stance split at 1/6 g offload [2].
References
- Valle, P. S. (2017). Reduced Gravity Testing of Robots (and Humans) Using the Active Response Gravity Offload System
. Institute of Electrical and Electronics Engineers. ntrs.nasa.gov/citations/20170008856
BibTeX
@misc{valle2017reduced, title = {Reduced Gravity Testing of Robots (and Humans) Using the Active Response Gravity Offload System}, author = {Valle, Paul Steinar}, journal = {Institute of Electrical and Electronics Engineers}, year = {2017}, url = {https://ntrs.nasa.gov/citations/20170008856}, abstract = {No abstract available} } - Bekdash, O. S., Valle, P. S., Kim, K. J., Jarvis, S. L., Dunn, J. T., Norcross, J. R. and Abercromby, A. F. J. (2020). Development and Evaluation of the Active Response Gravity Offload System as a Lunar and Martian EVA Simulation Environment
. International Conference on Environmental Systems, 20205003610. Source
BibTeX
@inproceedings{bekdash2020development, title = {Development and Evaluation of the Active Response Gravity Offload System as a Lunar and Martian EVA Simulation Environment}, author = {Bekdash, Omar S. and Valle, Paul S. and Kim, Kyoung Jae and Jarvis, Sarah L. and Dunn, Jocelyn T. and Norcross, Jason R. and Abercromby, Andrew F. J.}, booktitle = {International Conference on Environmental Systems}, number = {20205003610}, institution = {NASA}, year = {2020}, url = {https://ntrs.nasa.gov/citations/20205003610}, abstract = {In preparation for future exploration missions, NASA seeks the ability to simulate partial-gravity operations for use in ground-based research, crew training, and engineering design evaluations. The Active Response Gravity Offload System (ARGOS) at the Johnson Space Center (JSC) is designed to simulate reduced gravity environments, such as lunar, Martian, or microgravity, using a robotic system similar to an overhead bridge crane. ARGOS continuously offloads a portion of a suited human’s weight during all dynamic motions within the test facility, which can include basic functional movements such as walking, running, and jumping, as well as a wide range of planetary surface activities. This system will be used as part of a metabolic-rate task characterization study to determine the workload associated with partial-gravity extravehicular activity (EVA). Pilot testing was conducted using the MKIII prototype planetary space suit and two gimbal designs to determine the ability of the ARGOS test environment to simulate planetary EVA operations. This paper will describe the lessons learned from the feasibility testing, simulation-environment mockup design, and the results from the pilot tests and their influence into the final study design. Being able to effectively simulate partial-gravity environments and characterize the performance of crewmembers will have an impact on multiple domains including suit design, task design, thermal models, and life-support-system capacity verification plans, among others.} } - Jarvis, S. L., Vu, L. Q., Gupta, G., Benson, E., Kim, K. H., Rhodes, R. and Rajulu, S. L. (2023). Development of ARGOS (Active Response Gravity Offload System) Offloading Assessments and Methodology for Lunar EVA Simulations
. International Conference on Environmental Systems, 20230002430. Source
BibTeX
@inproceedings{jarvis2023development, title = {Development of ARGOS (Active Response Gravity Offload System) Offloading Assessments and Methodology for Lunar EVA Simulations}, author = {Jarvis, Sarah L. and Vu, Linh Q. and Gupta, Garima and Benson, Elizabeth and Kim, K. Han and Rhodes, Richard and Rajulu, Sudhakar L.}, booktitle = {International Conference on Environmental Systems}, number = {20230002430}, institution = {NASA}, address = {Calgary}, year = {2023}, url = {https://ntrs.nasa.gov/citations/20230002430}, abstract = {The Active Response Gravity Offload System (ARGOS) at NASA Johnson Space Center (JSC) is an analog environment that can offload pressurized suited subjects for various reduced gravity simulations. The suit is suspended from a robotic overhead crane by a cable connected to the suit via a gimbal with an adjustable pivot point (i.e. offload attachment). There has been increased interest in providing planetary pressurized suited training at ARGOS in preparation for lunar missions. Determination of the appropriate gimbal pivot point location for a given subject is vital for a high-fidelity functional lunar simulation. Interactions between the pivot point location and human-spacesuit center of gravity (CG) can result in righting moments that may lead to artificially stable or unrealistically challenging configurations. Changing the pivot point location is time consuming and repeated adjustment can result in loss of valuable pressurized suited time. This paper aims to share knowledge obtained from the offloading characterization efforts during pressurized suited testing at ARGOS and document the ongoing process to define an appropriate pivot point location through iterative quantitative and qualitative assessments. Human-spacesuit CG locations for the ARGOS lunar simulation were estimated using a 3D body scan and density model combined with spacesuit hardware CAD and specifications. Early pilot testing of the gimbal revealed that setting the pivot point coincident with the modeled CG location was not always possible due to the current gimbal design, and small pivot point shifts had noticeable effects on subject stability. Fourteen subjects performed a series of CG-related tasks in the Exploration Extravehicular Mobility Unit (xEMU) to assess simulation characteristics. Through iterative testing, this task list evolved to streamline the process needed to efficiently identify a suitable pivot point for a given subject. The developed methodology will be critical for pivot point selection during astronaut training in the ARGOS environment.} } - NASA Johnson Space Center. (2024). JSC Analogs and Mockups. nasa.gov/reference/jsc-analogs-mockups
BibTeX
@misc{nasajscanalogs, title = {JSC Analogs and Mockups}, author = {{NASA Johnson Space Center}}, organization = {nasa.gov}, year = {2024}, url = {https://www.nasa.gov/reference/jsc-analogs-mockups/} } - Badger, J. M., Hulse, A. M., Taylor, R. C., Curtis, A. W., Gooding, D. R. and Thackston, A. (2014). Model-based Robotic Dynamic Motion Control for the Robonaut 2 Humanoid Robot
. IEEE-RAS International Conference on Humanoid Robots, 20140000410. Source
BibTeX
@inproceedings{badger2014model, title = {Model-based Robotic Dynamic Motion Control for the Robonaut 2 Humanoid Robot}, author = {Badger, Julia M. and Hulse, Aaron M. and Taylor, Ross C. and Curtis, Andrew W. and Gooding, Dustin R. and Thackston, Allison}, booktitle = {IEEE-RAS International Conference on Humanoid Robots}, number = {20140000410}, pages = {62-67}, institution = {NASA}, year = {2014}, doi = {10.1109/humanoids.2013.7029956}, abstract = {Robonaut 2 (R2), an upper-body dexterous humanoid robot, has been undergoing experimental trials on board the International Space Station (ISS) for more than a year. R2 will soon be upgraded with two climbing appendages, or legs, as well as a new integrated model-based control system. This control system satisfies two important requirements; first, that the robot can allow humans to enter its workspace during operation and second, that the robot can move its large inertia with enough precision to attach to handrails and seat track while climbing around the ISS. This is achieved by a novel control architecture that features a joint-level embedded impedance control law which is tightly interfaced with a kinematic and dynamic coordinated control system that resides on centralized processors. This paper presents the integrated control algorithm as well as several test results that illustrate R2's safety features and performance.} }