Abstract
Eight pin-on-disk tribometers have been made for testing materials in space on board the International Space Station. They will be exposed directly to the low earth orbit (LEO) environment on board the “Materials on the International Space Station Experiments” platform where they will experience extreme conditions including atomic oxygen, ultrahigh vacuum, radiation (including UV radiation), and thermal ranges from −40 to 60 °C. In order to survive launch and LEO, these tribometers were designed to be extremely compact, rugged, and reliable. Pin-on-disk tribology experiments are now being performed with a 13.2 mm/s sliding velocity (14 RPM at 9 mm wear track radius) and a 1 N normal load with hemispherical pin of 1.5875 mm radius. Materials tested include MoS2/Sb2O3/Au, MoS2/Sb2O3/C, YSZ/Au/MoS2/DLC, and SiO-doped DLC coatings, and bulk samples of polytetrafluoroethylene (PTFE) alumina nanocomposites and gold.
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Acknowledgments
This project, designed, developed, and eventually delivered tribometers to the International Space Station. This could not be possible without significant collaborations and support from the research community. Significant thanks are owed to: John Jones, Michelle Ewy, Andrey Voevodin, Shane Juhl, Chris Muratore, Justin Lenoff, Jeffrey Zabinski, and Andy Korenyi-Both, Gary Pippin, Andy Robb, Many Urcia, Miria Finckenor, Phillip Jenkins, David Burris, Robert Carpick, Andy Konicek, Somuri Prasad, Chandra Venkatraman, Jim Keith, Rachel Colbert, Jennifer Vail, Nick Argibay, Jason Steffens, Dan Dickrell, Scott Perry, Linda Schadler, Thierry Blanchet, and Joe Priester.
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Appendix 1: Uncertainty Analysis for the Space Tribometers
Appendix 1: Uncertainty Analysis for the Space Tribometers
The uncertainty analysis for the friction coefficient follows the methods described by Burris and Sawyer [35] and Schmitz et al. [36]. To a reasonable approximation the uncertainty in the lateral directions is the same as the uncertainty in the normal direction, u(F L) = u(F N) = u(F). In addition, the magnitude of the lateral forces during clockwise and counterclockwise rotations are approximately equal, \( \left| {F_{{\rm L_{\rm cw} }} } \right| = \left| {F_{{\rm L_{\rm ccw} }} } \right| = \left| {F_{L} } \right| \). Hence,
Upon simplification, and a substitution for the lateral force magnitude (F L = μF N), Eq. 2 can be simplified to give Eq. 3:
Solving for uncertainty in the average friction coefficient is compactly given by Eq. 4. For low-friction materials, the uncertainty in friction coefficient is given by Eq. 5.
For the experimental design and instrumentation used on this tribometer embodiment, the uncertainty in forces was u(F) = 15 mN, and the normal load was nominally F N = 1 N. Thus, the uncertainty in friction coefficient is not better than u(μ) = 0.01. This is a reasonable result and achievement considering design constraints placed on the hardware, but, as others have demonstrated in UHV, it is certainly possible to have lower uncertainties in friction coefficient [18, 37–40].
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Krick, B.A., Sawyer, W.G. Space Tribometers: Design for Exposed Experiments on Orbit. Tribol Lett 41, 303–311 (2011). https://doi.org/10.1007/s11249-010-9689-y
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DOI: https://doi.org/10.1007/s11249-010-9689-y