Solubility and diffusion studies of ultra pure transition elements in ultra pure alkali metals Status summary report
Solution rates of pure iron and molybdenum in liquid potassium
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Solution rates of pure iron and molybdenum in liquid potassium
Molybdenum alloy /TZM/ capsule experiments with boiling-refluxing potassium to determine mass transfer parameters
Long time creep test data on molybdenum base alloys, tantalum base alloys, and vapor deposited tungsten
Welding parameters and elevated temperature aging and strength characteristics of transition joints between chromium molybdenum alloy steel and stainless steel
Mercury corrosion and evaluation of corrosion products found in separators of three chromium molybdenum alloy boiling thermal convection loops
Removal of SNAP-8 lubricant/coolant fluid from chromium-molybdenum steel
Mechanical properties of chromium molybdenum steel
Iridium-molybdenum diffusion for protective coatings on refractory metals
Space lubrication problems, molybdenum disulfide films for heavily loaded gears, and ball bearing protection from contamination
Lubrication and bearing problems in space environment, noting molybdenum disulfide and silicones
Ball bearing life operating in vacuum with molybdenum disulfide and oils as lubricant
Performance of thermionic converters, discussing voltage output, interelectrode spacing, rhenium- rhenium and rhenium-molybdenum electrode systems
The lifetime of an AMTEC electrode depends on the rate of grain growth, which in turn depends on the surface self-diffusion coefficient of the electrode material under AMTEC operating conditions. Grain growth rates for molybdenum and platinum-tungsten alloy electrodes have been determined, and have been used to predict operating lifetimes of AMTEC electrodes. For lifetimes of 10 years of more, Mo may be used in AMTEC cells only at operating temperatures under 1100 K. Pt(sub 2.5)W electrodes may be used at much higher temperatures, up to 1300 K.
With NASA’s desire to replace iodine as the biocide within the potable water system of future missions, we continue our development of the biocidal MoS2 (BioMoSS) system. BioMoSS is a visible-light activated photocatalyst based upon few-layered vertically aligned molybdenum disulfide (FLV-MoS2) for the production of reactive oxygen species (ROS) as a biocide. FLV-MoS2 has been reported to have a high bacterial kill rate. We report significant improvements in the vertical-alignment and biocidal efficacy of the FLV-MoS2 compared to our initial results reported last year. Furthermore, we report the results of peroxide formation with and without surface deposition using gold. Finally, we investigate the delamination of the FLV-MoS2 films under immersion in water.
The sputtering yield of molybdenum under xenon ion bombardment was mesured using a Quartz Crystal Microbalance.
Sputter yields have been measured for chemically-vapor deposited polycrystalline diamond, carbon-carbon composite, and molybdenum subject to bambardment with xenon ions at 150, 250, 500, and 750 electron volts. The diamond yield ranged from 0.12 to 0.33 over the range of energies investigated.
This work is a follow-on to a prior study on the effect of exposure to humid air on the durability of a molybdenum disulfide (MoS2) dry film lubricant on spur gears operated in vacuum, motivated by the James Webb Space Telescope (JWST) mission. In this study, MoS2 dry-lubricating films (DFLs) matching JWST specification were applied to test gears. The gear specimens were subjected to a brief run-in period in vacuum prior to their exposure to humid air, mimicking the sequence of mechanism checkout testing, exposure to air during integration, and then storage prior to launch. Test gear exposure times to humid air ranged from 1 hour to 326 days. After exposure, gear durability tests were conducted as an indication of film lifetime. MoS2 DFLs that were exposed to humid air (57% RH) exhibited reduced film durability relative to DFLs that were not exposed. On average, the exposed specimens demonstrated 75% shorter film life. The severity of the reduction in film durability did not correlate with the duration of exposure, i.e., long exposures to humid air were not more impactful to film durability than were short exposures.
A method of calculating a relation for the critical surface temperature for ion current emission is presented. The method is based on the S-shaped electron emission curves for surfaces in the presence of ionizable vapors and upon the assumptions of thermodynamic equilibrium involved in the Saha-Langmuir relation. A comparison of the critical temperatures so calculated with the relation obtained from actual ion emission data on the cesium-tungsten system shows good agreement over a wide current density range. Critical temperatures for cesium ion current densities of 0.21 and 1.9 amperes per square centimeter calculated by this method are presented for surfaces of rhenium, molybdenum, tantalum, and niobium. Tentative relations of the form log j equals A (sub p) plus (B (sub p) over T) are presented for these same systems, where j is the ion current density, A (sub p) and B (sub p) are constants, and T is the temperature.