JAXA Space Exploration Innovation Hub Center Space Exploration Experiment Building

JAXA Space Exploration Innovation Hub Center.
A rover or lander cannot be qualified against the Moon itself, so an agency has to decide which pieces of the lunar environment it will build indoors and which it will accept losing. Large agencies answer that question by spreading the environment across a set of separate buildings rather than one: NASA Glenn, for instance, lists distinct facilities for vacuum, vibration, icing and engine test rather than a single hall that does everything [13]. JAXA’s answer at Sagamihara is the same split. The Space Exploration Field is a 400 square meter indoor sand field with controlled lighting and climate in which full-size rovers and landers are driven, dropped and operated [1], and it is deliberately narrow: repeatable terrain and illumination, nothing else. It occupies the Space Exploration Experiment Building, run by the Space Exploration Innovation Hub Center. Both English names are translations: JAXA publishes the building and the field only in Japanese, as 宇宙探査実験棟 and 宇宙探査フィールド [1][2]. It was completed in February 2017 and entered service in May 2017. The building sits alongside the older ISAS Sagamihara test buildings, which provide the structural, vibration, thermal vacuum, anechoic and drop-test capability the field itself does not attempt [3].
Laboratory data
Section titled “Laboratory data”| Parameter | Value |
|---|---|
| Operator | JAXA Space Exploration Innovation Hub Center, known as TansaX [1][3] |
| Location | Sagamihara Campus, Chuo-ku, Sagamihara, Kanagawa, Japan |
| Commissioned | Building completed February 2017, operational May 2017 [2] |
| Type | Indoor analogue terrain field with controlled illumination and climate |
| Floor area | Gross floor area 1232.76 m2; building area 899.83 m2; field 400 m2 [1][2] |
| Capabilities | Field, control rooms, cleanroom |
| Simulant or terrain | Silica sand, 425 t: 410 t at 0.3 to 0.6 mm, 15 t at 3 to 5 mm |
| Instrumentation | Two control rooms, a catwalk, a 2.8 t indoor crane, xenon solar illumination |
| Ground truth | Not published. Users bring their own metrology |
| Fidelity limits | Ambient pressure, 1 g, room temperature; silica sand, not a simulant [1][7]. See below |
| Access | Open innovation and joint research with industry [1][2]. No lead time or fee published |
| Cited by | sora-q, lev-1 |
Capabilities
Section titled “Capabilities”Space Exploration Field
Section titled “Space Exploration Field”| Parameter | Value |
|---|---|
| Working volume | 22.6 x 17.7 m, 400 m2, ceiling height 10.5 m [1] |
| Test article limits | Handling by a 2.8 t indoor crane [1][2] |
| Vacuum | Not applicable. Ambient pressure |
| Temperature | Controlled, not cycled. No range or ramp rate published |
| Illumination | Darkroom with a single xenon solar source. No solar constant or collimation published |
| Simulant or terrain | Silica sand, 425 t, 0.3 to 0.6 mm and 3 to 5 mm, in flat, hill and gravel sections [1][2] |
| Slope | Piled by hand. 0 to 18 degrees used in a published campaign [5]. Maximum not published |
| Gravity offload | Not applicable |
| Instrumentation | Xenon solar illumination, catwalk, 2.8 t crane [1][2]. Users bring metrology |
The field is the center of the building and is described by JAXA as reproducing lunar surface terrain and illumination conditions so that exploration robots and landers can be evaluated under conditions close to real operation. The stated test types are surface driving, landing drop tests, flight tests and exploration work operation tests, run as a connected sequence rather than separately. JAXA attributes the field’s ability to take full-size landers and cooperative tests of several robots at once to its being among the largest in the world in both area and height.
Three design decisions define the envelope. The roof is a double folded insulated metal panel chosen to keep the interior temperature uniform against outside weather [2]. The ground under the field was improved into a strong bearing layer to support 425 tonnes of sand, and the floor was built uniform across its whole area so that terrain can be piled into a hill or dug out like a well at any point, and so that it withstands the impact of a lander touchdown test. Temperature and humidity are managed so that the sand state and the lighting are identical from run to run [1]. No relative density target or preparation procedure between runs is published, and no solar constant fraction, collimation angle or achievable solar elevation is published for the xenon illumination.
Operations control rooms
Section titled “Operations control rooms”| Parameter | Value |
|---|---|
| Working volume | Two rooms adjoining the field and overlooking it [1][2] |
| Instrumentation | Laid out to simulate a three-point relay chain [2] |
The two control rooms are laid out to stand in for a three-node relay, such as ground station, spacecraft interior and surface, or Earth, Moon and rover, rather than for a single operator position [2]. That makes operations latency and relay topology a testable variable alongside the terrain.
The second-floor viewing corridor gives a full view of the field for public visitors, and uses instantly switchable glass that changes from frosted to clear. JAXA states the switch is not only theatrical: it protects the intellectual property embodied in the hardware under test by making the field invisible on demand.
Cleanroom
Section titled “Cleanroom”Adjacent to the field, the Innovation Hub operates an ISO Class 1 cleanroom at Sagamihara, built for planetary protection work: comparing the sterilization and decontamination effectiveness and corrosion behavior of different techniques, building decontamination systems able to break down spores and biomolecules, extending inactivation to viruses and allergens where prior knowledge was thin, and developing the verification methods for all of it [4]. That work sits inside a discipline that has been under continuous revision since the first NASA sterilization policies: bioburden reduction, remote bioassay laboratories and the microbial detection methods used to certify a spacecraft clean have all changed as mission categories and science objectives have grown more demanding [8]. The Sagamihara cleanroom’s decontamination and verification work is a contribution to that same open problem rather than a fixed, solved procedure.
Instrumentation
Section titled “Instrumentation”Facility-supplied instrumentation published for the field is limited to the control rooms, the catwalk, the crane and the xenon solar illumination [1]. Campaign-specific metrology is brought by users. In the Tohoku University EX1 campaign the rover was tracked by a 16-camera OptiTrack system running at 180 Hz with plus or minus 0.15 mm accuracy, wheel speed came from encoders, and external cameras independently timed wheel rotations across a 2 m section so that average slip could be estimated without relying on the rover [5]. That approach mirrors how the Mars Science Laboratory traverse campaign was instrumented on Earth: Mars-weight test vehicles driven over analog terrain with slip measured against slope and cross-checked against wheel sinkage, rather than inferred from the rover’s own odometry alone [11].
The neighboring ISAS buildings hold the environmental test capability the field does not: the Flight Environment Test Building carries the mechanical environment test room for vibration, shock and dynamic balance, plus a magnetic shield room, a space chamber, a radio anechoic chamber and a clean assembly room; the Structure and Mechanics Test Building tests strength and rigidity of structures and the function of interstage joints and fairings; and the Advanced Facility for Space Science and Technology holds wind tunnels, space plasma and cosmic radiation experiment facilities and a weightless drop test facility [3].
What it does not reproduce
Section titled “What it does not reproduce”The field trades environment for repeatability, and JAXA says so in those terms: the value claimed is that the sand state and the illumination are the same on every run and are not affected by weather, achieved through temperature and humidity control, a darkroom and artificial lighting. Nothing in the published description offers vacuum, thermal cycling or reduced gravity in the field.
The soil is silica sand, 0.3 to 0.6 mm for the bulk of the mass and 3 to 5 mm for the gravel section [1], graded for handling and repeatability rather than matched to lunar mineralogy, and coarser than lunar regolith. A user group has published its view of the same class of material, that dry loose silica sand is a low-fidelity lunar regolith simulant whose sparse grain distribution makes sinkage and slip conditions more challenging than the real surface would [5]. NASA’s own simulant standardization effort exists for exactly this gap: a 2005 workshop and its follow-on recommendations argued that lunar surface technology development needs a common, traceable, characterized simulant rather than ad hoc local material, because the Apollo sample inventory is both too small and too scientifically valuable to consume in routine mechanical testing [6]. The current revision of that guide still treats simulant selection as an open, evolving choice among competing materials rather than a settled standard [7]. Bulk graded silica sand, chosen at Sagamihara for handling four hundred tonnes repeatably, sits outside that standardization effort rather than inside it.
Drop testing is bounded by the building. The floor was designed to withstand the impact of a lander touchdown test [2], which is a structural limit on the energy that can be delivered, and the 10.5 m ceiling bounds the drop height available [1]. Other agencies have solved the same full-scale drop-test problem with dedicated rigs rather than a shared field floor: the Mars Exploration Rover program characterized its airbag landing loads with an instrumented drop tower and a separate quasi-static shaker qualification path for hardware that could not be airbag-tested directly [9][10], and NASA’s Impact Dynamics Research Facility, built two decades earlier for full-scale aircraft crash testing, used a pendulum swing rather than a fixed drop height to reach a range of flight paths and impact velocities [12]. Sagamihara’s approach is the opposite of both: one uniform floor and a fixed ceiling height, traded for being able to take any lander or rover the crane can lift rather than a purpose-built rig for one vehicle class.
Campaigns run there
Section titled “Campaigns run there”SLIM and SORA-Q. JAXA states that the SLIM lander and the SORA-Q transformable lunar robot were tested in the Space Exploration Experiment Building, and the facility runs public tours built around that history [1]. See sora-q.
Lunar base construction machinery. Joint research on force-controlled construction machinery for lunar base building, with Yanmar Holdings, is run in the field, aimed at automatic and autonomous operation of construction equipment on the lunar surface [1].
Tohoku University EX1 high-speed rover campaign. A four-wheeled 21.63 kg rover of 0.82 by 0.52 by 0.67 m with a passive spring-damper suspension was driven over a 20 m by 20 m area of silica sand about 0.3 m deep, at wheel velocities of 0.23 to 1.17 m/s on flat ground and on slopes of 0 to 18 degrees at up to 0.47 m/s, with additional rapid acceleration and deceleration runs to capture transient slip [5]. The resulting slip and sinkage regressions were fitted for use in a real-time lunar surface simulator. The campaign also established that grouser length has to be included in the effective wheel radius or the computed slip comes out negative during normal driving [5].
What is not established
Section titled “What is not established”JAXA’s own publications give area, mass and completion date for the field but no relative density target, no preparation procedure between runs, and no solar constant fraction, collimation angle or achievable solar elevation for the xenon source [1][2]. No ground truth for slope, sinkage or slip is published by the facility itself; every quantitative result that exists, including the EX1 slip-sinkage regressions, comes from a visiting team’s own instrumentation rather than from the facility [5]. Whether the silica sand’s mechanical behavior has been benchmarked against a characterized lunar simulant such as those NASA catalogs, rather than only asserted to be coarser and more sparsely graded, is not published [6][7]. The maximum drop height the 10.5 m ceiling actually permits for a given test article mass, and any correlation between Sagamihara drop results and analytical or scaled models as exists for other agencies’ drop-test programs [9][10], is not stated.
References
- (2026). JAXA Space Exploration Innovation Hub Center: Space Exploration Experiment Building. ihub-tansa.jaxa.jp/about/afse.html
BibTeX
@misc{jaxaafse, title = {JAXA Space Exploration Innovation Hub Center: Space Exploration Experiment Building}, organization = {ihub-tansa.jaxa.jp}, year = {2026}, url = {https://www.ihub-tansa.jaxa.jp/about/afse.html} } - (2026). JAXA Facilities Department: Space Exploration Experiment Building. stage.tksc.jaxa.jp/shisetsu/locations/sagamihara/exploration
BibTeX
@misc{jaxashisetsuafse, title = {JAXA Facilities Department: Space Exploration Experiment Building}, organization = {stage.tksc.jaxa.jp}, year = {2026}, url = {https://stage.tksc.jaxa.jp/shisetsu/locations/sagamihara/exploration/} } - (2026). ISAS: Sagamihara Campus Facilities. isas.jaxa.jp/en/about/facilities/sagamihara.html
BibTeX
@misc{isassagamihara, title = {ISAS: Sagamihara Campus Facilities}, organization = {isas.jaxa.jp}, year = {2026}, url = {https://www.isas.jaxa.jp/en/about/facilities/sagamihara.html} } - (2026). JAXA Space Exploration Innovation Hub Center: Cleanroom. ihub-tansa.jaxa.jp/about/cleanroom.html
BibTeX
@misc{jaxaihubcleanroom, title = {JAXA Space Exploration Innovation Hub Center: Cleanroom}, organization = {ihub-tansa.jaxa.jp}, year = {2026}, url = {https://www.ihub-tansa.jaxa.jp/about/cleanroom.html} } - Kern, J. M., Hurrell, J. M., Santra, S., Takehana, K., Uno, K. and Yoshida, K. (2025). Data-Driven Terramechanics Approach Towards a Realistic Real-Time Simulator for Lunar Rovers
. arXiv preprint. Source
BibTeX
@article{kern2026data, title = {Data-Driven Terramechanics Approach Towards a Realistic Real-Time Simulator for Lunar Rovers}, author = {Kern, Jakob M. and Hurrell, James M. and Santra, Shreya and Takehana, Keisuke and Uno, Kentaro and Yoshida, Kazuya}, journal = {arXiv preprint}, pages = {662-668}, year = {2025}, doi = {10.1109/isparo66239.2025.11436587}, abstract = {High-fidelity simulators for the lunar surface provide a digital environment for extensive testing of rover operations and mission planning. However, current simulators focus on either visual realism or physical accuracy, which limits their capability to replicate lunar conditions comprehensively. This work addresses that gap by combining high visual fidelity with realistic terrain interaction for a realistic representation of rovers on the lunar surface. Because direct simulation of wheel-soil interactions is computationally expensive, a data-driven approach was adopted, using regression models for slip and sinkage from data collected in both full-rover and single-wheel experiments and simulations. The resulting regression-based terramechanics model accurately reproduced steady-state and dynamic slip, as well as sinkage behavior, on flat terrain and slopes up to 20°, with validation against field test results. Additionally, improvements were made to enhance the realism of terrain deformation and wheel trace visualization. This method supports real-time applications that require physically plausible terrain response alongside high visual fidelity.} } - Sibille, L., Carpenter, P., Schlagheck, R. and French, R. A. (2006). Lunar Regolith Simulant Materials: Recommendations for Standardization, Production, and Usage
. NASA Marshall Space Flight Center, NASA/TP-2006-214605. Source
BibTeX
@techreport{sibille2006development, title = {Lunar Regolith Simulant Materials: Recommendations for Standardization, Production, and Usage}, author = {Sibille, Laurent and Carpenter, Paul and Schlagheck, R. and French, R. A.}, number = {NASA/TP-2006-214605}, institution = {NASA Marshall Space Flight Center}, type = {NASA Technical Publication}, year = {2006}, url = {https://ntrs.nasa.gov/citations/20060051776}, abstract = {Experience gained during the Apollo program demonstrated the need for extensive testing of surface systems in relevant environments, including regolith materials similar to those encountered on the lunar surface. As NASA embarks on a return to the Moon, it is clear that the current lunar sample inventory is not only insufficient to support lunar surface technology and system development, but its scientific value is too great to be consumed by destructive studies. Every effort must be made to utilize standard simulant materials, which will allow developers to reduce the cost, development, and operational risks to surface systems. The Lunar Regolith Simulant Materials Workshop held in Huntsville, AL, on January 24 26, 2005, identified the need for widely accepted standard reference lunar simulant materials to perform research and development of technologies required for lunar operations. The workshop also established a need for a common, traceable, and repeatable process regarding the standardization, characterization, and distribution of lunar simulants. This document presents recommendations for the standardization, production and usage of lunar regolith simulant materials.} } - Slabic, A., Gruener, J. E., Kovtun, R. N., Rickman, D. L., Sibille, L., Oravec, H. A., Edmunson, J. and Keprta, S. (2024). Lunar Regolith Simulant User's Guide, Revision A
. NASA, NASA/TM-20240011783. Source
BibTeX
@techreport{slabic2024lunar, title = {Lunar Regolith Simulant User's Guide, Revision A}, author = {Slabic, Ane and Gruener, John E. and Kovtun, Rostislav N. and Rickman, Douglas L. and Sibille, Laurent and Oravec, Heather A. and Edmunson, Jennifer and Keprta, Sean}, number = {NASA/TM-20240011783}, institution = {NASA}, year = {2024}, url = {https://ntrs.nasa.gov/citations/20240011783}, abstract = {This guide is titled Lunar Regolith Simulant User's Guide, Rev A, and two points need to be made about the title. First, is the use of the term "regolith". During the Apollo Program, the term "soil" was used for taking a sample of the loose material on the surface, and then cataloging that sample in the lunar curation database as a "soil sample". By the 1980s, the term "regolith" gained favor by lunar scientists. In the Lunar Sourcebook (Heiken et al., 1991), regolith is defined as "a general term for the layer or mantle of fragmental and unconsolidated rock material, whether residual or transported and of highly varied character, that nearly everywhere forms the surface of the land and overlies or covers bedrock". Regolith is a terrestrial term that seems to go back to 1897, according to a recent paper by Huggett (2023). Huggett summed up his paper by writing, "soil and regolith are one in the same". "Regolith" will mostly be used throughout this guide, as it tends to separate in one's mind the unique nature of the Moon's surface when compared to the inherent bias humans have in their mind when they hear and use the word "soil". When referring to Apollo samples, "soil" is used for historical context and in some places the simple term "lunar simulant" is also used. Secondly, Rev A is used in the title because NASA released its first Lunar Regolith Simulant User's Guide in 2010, near the end of NASA's Constellation Program (Schrader et al., 2010). This guide follows in the pattern of that first guide and will be updated on a periodic basis as new simulants are created, characterized and used, and as new information emerges about the Moon's regolith due to new lunar exploration missions, both robotic and human.} } - Kazarians, G. A., Benardini, J. N., Stricker, M. C., Schubert, W. W., Chen, F., Vaishampayan, P., Jones, M. A., Barengoltz, J. and Koukol, R. (2017). The Evolution of Planetary Protection Implementation on Mars Landed Missions
. IEEE Aerospace Conference. Source
BibTeX
@inproceedings{kazarians2017evoluation, title = {The Evolution of Planetary Protection Implementation on Mars Landed Missions}, author = {Kazarians, Gayane A. and Benardini, James N. and Stricker, Moogega C. and Schubert, Wayne W. and Chen, Fei and Vaishampayan, Parag and Jones, Melissa A. and Barengoltz, Jack and Koukol, Robert}, booktitle = {IEEE Aerospace Conference}, pages = {1-20}, publisher = {IEEE}, year = {2017}, doi = {10.1109/aero.2017.7943576}, abstract = {NASA has developed requirements dedicated to the prevention of forward and backward contamination during space exploration. Historically, international agreements provided guidelines to prevent contamination of the Moon and other celestial bodies, as well as the Earth (e.g., sample return missions). The UN Outer Space Treaty was established in 1967 and the Committee on Space Research (COSPAR) maintains a planetary protection policy complying with Article IX of this treaty. By avoiding forward contamination, the integrity of scientific exploration is preserved. Planetary Protection mission requirements are levied on missions to control contamination. These requirements are dependent on the science of the mission and on the celestial bodies encountered or targeted along the way. Consequently, categories are assigned to missions, and specific implementation plans are developed to meet the planetary protection requirements. NASA missions have evolved over time with increasingly more demanding scientific objectives and more complex flight systems to achieve those objectives and, thus, planetary protection methods and processes used for implementation have become much more intricate, complicated, and challenging. Here, we will portray the evolution of planetary protection implementation at JPL in several important areas throughout the course of NASA sponsored robotic Mars lander or rover missions, starting from Mars Pathfinder through the beginning of Mars 2020. Highlighted in the discussion will be process changes in planetary protection requirements development and flow down. Development and implementation of new and improved methods used in the reduction of spacecraft bioburden will be discussed as well as approaches and challenges that come along with setting up remote laboratories to perform bioassays. The consequences and forward planning of delays on missions will be highlighted as well as lessons learned on the impact of communication and training in achieving planetary protection requirements. The evolution of methods used for the detection of microbial bioburden on spacecraft hardware will be considered. These methods use standard microbiology as well as the adaptation of advances in biotechnology, molecular biology, and bioinformatics. Technical approaches developed for the prevention of contamination and recontamination of hardware during Assembly, Test, and Launch Operations will be discussed.} } - Adams, D. S. (2004). Mars Exploration Rover Airbag Landing Loads Testing and Analysis
. AIAA/ASME/ASCE/AHS/ASC Structures, Structural Dynamics, and Materials Conference. Source
BibTeX
@inproceedings{adams2004mars, title = {Mars Exploration Rover Airbag Landing Loads Testing and Analysis}, author = {Adams, Douglas S.}, booktitle = {AIAA/ASME/ASCE/AHS/ASC Structures, Structural Dynamics, and Materials Conference}, publisher = {American Institute of Aeronautics and Astronautics}, year = {2004}, doi = {10.2514/6.2004-1795}, abstract = {This paper presents a summary of the testing and analysis used to quantify the expected airbag landing loads for the Mars Exploration Rovers. The airbag drop test setup, lander instrumentation, and the test data reduction method are discussed in order to provide an understanding of the empirical loads. A set of limiting cases that bound the empirical data are developed for use in finite element modeling of the lander and rover models. A favorable comparison is made between the empirical data and available computational airbag models boosting confidence in the results.} } - Davis, G. L., Scharton, T. D. and Tsoi, W. B. (2002). Dynamic testing techniques for qualifying Mars Exploration Rover equipment to quasi-static landing loads
. IEEE Aerospace Conference. Source
BibTeX
@inproceedings{davis2002dynamic, title = {Dynamic testing techniques for qualifying Mars Exploration Rover equipment to quasi-static landing loads}, author = {Davis, G. L. and Scharton, Terry D. and Tsoi, W. B.}, booktitle = {IEEE Aerospace Conference}, publisher = {JPL Open Repository}, year = {2002}, url = {https://dataverse.jpl.nasa.gov/dataset.xhtml?persistentId=hdl:2014/8681} } - Heverly, M., Matthews, J., Lin, J., Fuller, D., Maimone, M., Biesiadecki, J. and Leichty, J. (2013). Traverse Performance Characterization for the Mars Science Laboratory Rover
. Journal of Field Robotics. Source
BibTeX
@article{heverly2013traverse, title = {Traverse Performance Characterization for the Mars Science Laboratory Rover}, author = {Heverly, Matt and Matthews, Jaret and Lin, Justin and Fuller, Dan and Maimone, Mark and Biesiadecki, Jeffrey and Leichty, John}, journal = {Journal of Field Robotics}, volume = {30}, pages = {835-846}, year = {2013}, doi = {10.1002/rob.21481}, abstract = {It is anticipated that the Mars Science Laboratory rover, named Curiosity, will traverse 10–20 km on the surface of Mars during its primary mission. In preparation for this traverse, Earth‐based tests were performed using Mars weight vehicles. These vehicles were driven over Mars analog bedrock, cohesive soil, and cohesionless sand at various slopes. Vehicle slip was characterized on each of these terrains versus slope for direct upslope driving. Results show that slopes up to 22 degrees are traversable on smooth bedrock and that slopes up to 28 degrees are traversable on some cohesive soils. In cohesionless sand, results show a sharp transition between moderate slip on 10 degree slopes and vehicle embedding at 17 degrees. For cohesionless sand, data are also presented showing the relationship between vehicle slip and wheel sinkage. Side by side testing of the Mars Exploration Rover test vehicle and the Mars Science Laboratory test vehicle show how increased wheel diameter leads to better slope climbing ability in sand for vehicles with nearly identical ground pressure. Lastly, preliminary data from Curiosity's initial driving on Mars are presented and compared to the Earth‐based testing, showing good agreement for the driving done during the first 250 Martian days.} } - Vaughan, V. L. J. and Alfaro-Bou, E. (1976). Impact dynamics research facility for full-scale aircraft crash testing
. NASA, NASA-TN-. Source
BibTeX
@techreport{vaughan1976impact, title = {Impact dynamics research facility for full-scale aircraft crash testing}, author = {Vaughan, V. L. J. and Alfaro-Bou, E.}, number = {NASA-TN-}, institution = {NASA}, year = {1976}, url = {https://ntrs.nasa.gov/citations/19760014085}, abstract = {An impact dynamics research facility (IDRF) was developed to crash test full-scale general aviation aircraft under free-flight test conditions. The aircraft are crashed into the impact surface as free bodies; a pendulum swing method is used to obtain desired flight paths and velocities. Flight paths up to -60 deg and aircraft velocities along the flight paths up to about 27.0 m/s can be obtained with a combination of swing-cable lengths and release heights made available by a large gantry. Seven twin engine, 2721-kg aircraft were successfully crash tested at the facility, and all systems functioned properly. Acquisition of data from signals generated by accelerometers on board the aircraft and from external and onboard camera coverage was successful in spite of the amount of damage which occurred during each crash. Test parameters at the IDRF are controllable with flight path angles accurate within 8 percent, aircraft velocity accurate within 6 percent, pitch angles accurate to 4.25 deg, and roll and yaw angles acceptable under wind velocities up to 4.5 m/s.} } - NASA Glenn Research Center. (2026). Glenn Labs and Test Facilities. nasa.gov/glenn-labs-and-test-facilities
BibTeX
@misc{grc2026labs, title = {Glenn Labs and Test Facilities}, author = {{NASA Glenn Research Center}}, organization = {nasa.gov}, year = {2026}, url = {https://www.nasa.gov/glenn-labs-and-test-facilities/} }