WEAR OF MATERIALS IN LUNAR DUST ENVIRONMENT Koji MATSUMOTO (1), Mineo SUZUKI (1), Shin-ichiro NISHIDA (2), and Sachiko WAKABAYASHI (2) (1) Japan Aerospace Exploration Agency (JAXA), Aerospace Research and Development Directorate, 7-44-1 Jindaiji-higashimachi, Chofu, Tokyo 182-8522, Japan Phone: +81-422-40-3181, E-mail: [email protected] (2) Japan Aerospace Exploration Agency (JAXA), JAXA Space Exploration Center, 3-1-1 Yoshinodai, Sagamihara, Kanagawa 229-8510, Japan ABSTRACT Friction tests were carried out to investigate effects of dust particles covering the moon surface on wear properties of materials for space components. Especially, influences of particle sizes on wear were evaluated using a lunar soil simulant. The simulant was sieved into particle sizes of less than 32 µm and 100-300 µm. The particles were put on contact areas of specimens before the friction tests. The friction tests were conducted for several kinds of materials in vacuum. Tested materials were a few metals: stainless steel, titanium and aluminum alloys. A few coatings, PTFE films and MoS2 film that have been used for space, were also evaluated. Results show that wear of most of the materials increased by existence of simulant of lunar dust particles. Differences in friction were not significant but differences in wear were found between particle sizes. The effects of dust particles on the wear of tested materials are reported. 1. INTRODUCTION Activities on the moon are the next targets of space development around the world. Also in Japan, "Kaguya", which is a full-scale lunar exploration project since NASA's Apollo program, obtained important data using several kinds of observation instruments. The Japan Aerospace Exploration Agency (JAXA) will also progress to research and development on a subsequent explorer following Kaguya and observation and experimentation systems [1, 2]. The next steps for lunar exploration are landing and moving on the lunar surface. The moon is covered by large amounts of dust particles, called regolith, which should make serious problems for tribological component on the moon [3, 4]. Moreover, for activities on the moon, not only tribological parts sealed from dust particles but also some parts exposed directly to the dust environment will be necessary (e.g. crawlers, wheels of rovers) [5]. However, effects of the moon dust particles on parts in vacuum have not been clarified. Acquisition of data about legolith effects is necessary. Some studies of tribological effects of regolith have been started. Matsumoto et al. evaluated effects of dust particles on bonded lubricant films of MoS2 and PTFE in vacuum [6, 7]. Results show that the particles easily wore away the films. Ishibashi et al. conducted tribological tests for several ceramics [8, 9], showing wear rates for hardness of the ceramics. In this study, friction tests were carried out in vacuum to investigate the wears of some metal materials and a few types of coatings without binder materials, and changes in their frictional performance by lunar soil simulant. Those data will be useful for design and material selection for component moving on the moon. 2. EXPERIMENTAL DETAILS 2.1 Lunar soil simulant The lunar soil simulant [10, 11] was made from basaltic lava; it simulates the hardness and distribution of particle size to real lunar dust particles, regolith, which were extracted and retrieved during the Apollo program. The particles’ medium size was 70 µm. As with real regolith, its major constituent is silicon oxide. The simulant was sieved into two particle sizes to evaluate the particle size effects: less than 32 µm, and 100-300 µm. Fig. 1 shows photographs of both sizes of dust particles by optical microscope. 250 µm Particle sizes of less than 32 µm 100 - 300 µm (<32 µm) Fig. 1 Photographs of lunar soil simulant classified into particle sizes. Roller specimen (Coatings) Load Dust particles Arch-shaped specimen Fig. 2 Configuration of test specimens. Table 1 Combinations of test specimen materials Arch-shaped specimen Roller specimen Coating Substrate Stainless steel (440C) Titanium alloy (Ti-6Al-4V) 440C Aluminum alloy (A6061) stainless steel PTFE A A6061 PTFE B 440C MoS2 440C 2.2 Test specimens The configuration of the friction test is presented in Fig. 2. A roller specimen rotates against an arch-shaped specimen [6, 7]. This configuration was designed to restrain dust particles from leaving the contact area easily. The roller specimen had a curvature in the axial direction to apply a load uniformly; it was made of 440C stainless steel. Arch-shaped specimens were made of various metals: stainless steel (440C), titanium alloy (Ti-6Al-4V) and aluminum alloy (A6061). Coatings used for space applications were deposited inside the arch-shaped specimens. The coatings tested in this study were PTFE films and MoS2 film. The PTFE films were made by impregnating PTFE into many minute holes on hard anodized aluminum on the aluminum alloy surface (PTFE film A) [12] and into a non-electrolytic nickel layer, which was containing numerous micropores and deposited on 440C stainless steel (PTFE film B). The thicknesses of the PTFE films were 20-50 µm. The MoS2 film was sputter-deposited using an RF-magnetron. The film thickness was approximately 2.0 µm. Combinations of roller specimen and arch-shaped specimens are presented in Table 1. 2.3 Friction tests The lunar soil simulant of 5 mg, with a certain particle size, was put on the contact area of the arch-shaped specimen. Then a friction test was started in vacuum by putting a rotating roller specimen on an arch-shaped specimen with an applied load. The vacuum pressure was less than 1 × 10-4 Pa. Friction tests were conducted at a load of 10 N and a sliding speed of Fig. 3 Friction behaviors of the 440C roller specimen against arch-shaped specimens made of (a) 440C, (b) Ti alloy and (c) Al alloy with and without dust particles. 15 mm/s. The test duration was 500 rotations of the roller specimen. 3. RESULTS AND DISCUSSIONS 3.1 Results for bare metals Friction coefficients of the 440C roller specimen against three arch-shaped metal specimens are presented respectively in Figs. 3(a), 3(b) and 3(c). High friction coefficients of 0.8 to 1.0 were observed irrespective of the existence of dust particles for the 440C-440C combination. For the combination of 440C against Ti alloy, relatively low friction coefficients of 0.6 were obtained with dust particles in spite of the high value of 0.8 in the case of no particles. Dust particles acted as a lubricant. Their rotation on contact surface seemed to decrease friction. Especially, smaller particles showed a lower value at the beginning of the test. Unstable behavior shown later might have occurred by reduction of particles at the contact area. For the Al alloy arch-shaped specimen, no difference in friction behavior was found between tests except that the non-particle test showed a slightly lower value than the tests with particles at the start of the tests. (a) 440C against 440C Photographs of wear tracks of both roller and arch-shaped specimens by microscopic observation and surface profiles are depicted in Fig. 4. Much adhesive wear of both specimens occurred for the combination of 440C-440C. Smaller particles operated to restrain adhesive wear by reducing contacts between specimens. However, adhesive wear by 100-300 µm particles was greater than that occurring without particles. Removal of surface contaminants or oxides by the particles and subsequent removal of the particles themselves might have increased the adhesive wear. Severe adhesive wear was not observed in the case of 440C against different metals without particles. However, the amount of wear increased by dust particles. Much wear was observed on both 440C roller specimen and Ti alloy arch-shaped specimen with particle size of less than 32 µm. With larger particles, Ti alloy specimens showed little wear, as in the case with no particles. The aluminum alloy arch-shaped specimens showed the most wear with each particle size although the counterpart of 440C roller specimens showed no noticeable wear. (b) 440C against Ti alloy 3.2 (c) 440C against Al alloy Fig. 4 morphologies and surface profiles of wear tracks of both roller specimen and arch-shaped specimens after the friction tests with and without dust particles. Results for coatings Figure 5 presents friction coefficients of PTFE film A on Al alloy and wear tracks of the coatings and 440C roller specimens after the tests. The test without dust particles started with a friction coefficient of about 0.8 and became stable at a value of approximately 0.5. The friction coefficient of the coating with particle size of <32 µm increased gradually to 0.9 from the test start and became stable at 0.8. The friction behavior of the test with particle size of 100-300 µm was similar to that found in the non-particle test. Wear in the test without dust particles was greater than that of non-coated Al alloy. However, the wear of arch-shaped specimens by particles decreased with the coating. Wear resistance was improved by the coating in case of existence of dust particles. On other hand, the wear of the roller specimen increased compared to the case of the bare Al alloy arch-shaped specimen. Long scratched scars were apparent on the roller specimen with particle of 100-300 µm; it was more obvious than with <32 µm particles. The larger particles seemed to be removed from the contact area early in the test, so friction behavior was similar to that of the test with no particles. Fig. 5 Friction behaviors and wear tracks of PTFE film A with and without dust particles. Friction behavior of PTFE film B on 440C and results of observation after the tests are presented in Fig. 6. The friction coefficient showed a high value of 1.2 without particles, whereas significant wear was not found. Compared to the non-particle test, lower friction of 0.6 was observed with particles; it did not depend on the particle size. Some wear debris was found on the roller specimen but the wear depths of the coating were small and similar to the case of no particles. This coating showed excellent wear resistance for the lunar regolith except for the high friction in the case of no particles. The low friction coefficient of 0.1 was obtained for MoS2 film on 440C, as depicted in Fig. 7. However, because of the dust particles’ existence, high friction and much wear were observed. The film was worn away by particles early in the tests because the friction coefficient and wear morphology were almost identical to results of the 440C against bare 440C tests. Low hardness of the film and thin film thickness seemed to cause these results. Fig. 6 Friction behaviors and wear tracks of PTFE film B with and without dust particles. 3.3 Discussions The wear mechanism is expected to be abrasive wear when dust particles existed at the contact surface although the scratch track sizes differed between particle sizes. However, in some cases, e.g. 440C-440C and 440C-Ti alloy combinations, morphology of the wear tracks by particle size of 100-300 µm was observed as identical to those obtained from non-particle tests, apparently because of moving out of the particles. Wear by larger particles seemed to differ with the movement and action of the particles: the particle stayed at the contact surface, it left there soon or it was crashed to a smaller size. Action of the dust particles probably depended on test conditions, surface activation, static electricity of surfaces, and so on. Results obtained in this study also show that materials without high hardness, such as aluminum alloy, are difficult to use in a moon dust environment. However, wear resistance against dust particles was improved by PTFE coatings. To select materials and coatings for activities on the moon, hardness is an important consideration; however, its relationship to counterpart materials, toughness, particles adhesion and so on should be also considered. With consideration for 5. REFERENCES 1. http://moon.jaxa.jp/ja/future/index.html 2. Hoshino, T. and Matsumoto, K., “Strategies and Systems for Long Term Activities on the Moon”, Proc. of 26th ISTS, 2008-k-58, (2008). 3. Grant H. Heiken, et al., “Lunar Sourcebook, 3.4. Dust”, Cambridge University Press p34 (1991). 4. Spudis, P.D., translated by Mizutani, H., “The Once and Future Moon”, p89-108 (2000). 5. Gaier J. R., “The effects of Lunar Dust on EVA Systems”, NASA/TM-2005-213610 (2005). 6. Matsumoto, K., et al., “Effect of dust in vacuum on solid lubricants”, Proc. of JAST Tribology Conf. Saga, p195-196, (2007). 7. Matsumoto, K., et al., “Tribological Properties of Solid Lubricants in Moon Dust Environment”, World Tribology Congress, Kyoto, (2009). 8. Ishibashi K., et al., “Abrasive Wear of Ceramics by Lunar Regolith Simulant”, Proc. of JAST Tribology Conf. Saga, p113-114, (2007). Fig. 7 Friction behaviors and wear tracks of MoS2 sputtered film with and without dust particles. them, acquisition of further data related to other materials, coatings and treatments, along with different combinations are necessary to enhance wear resistance more. 4. SUMMARY Some metal materials and coatings used for space were evaluated on wear and friction properties in vacuum and lunar dust environment. Wear of most of the metal materials increased by existence of simulant of lunar dust particles. Differences in friction were not great, but differences in wear were observed between particle sizes. Regarding the coatings, most coatings tested in this study also had much wear or wore away easily by dust particles. However, a PTFE impregnated film having high wear resistance against dust particles was identified. 9. Ishibashi K., et al., “Abrasive Wear of Ceramics by Lunar Regolith Simulant (Section 2) – Wear Characteristics in Rolling Contacts –”, Proc. of JAST Tribology Conf. Tokyo, p65-66, (2008). 10. Wakabayashi, S. and Matsumoto K., “Development of Slope Mobility Testbed using Simulated Lunar Soil”, JAXA-RM-05-003 (2006). 11. Sueyoshi K., et al., “Reaction Mechanism of Various Types of Lunar Soil Simulants by Hydrogen Reduction”, Proc. of Earth & Space 2008 Conference, Long Beach, USA (2008). 12. Matsumoto, K. and Suzuki, M., “Evaluation of Various PTFE Films for Space use”, Proc. of International Tribology Conf. Kobe, (2005).
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