Radioisotope heat source evaluation program Final report, 15 May - 13 Dec. 1964
Radioisotope heat source - annotated bibliography on nuclear characteristics of radioactive isotopes
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Radioisotope heat source - annotated bibliography on nuclear characteristics of radioactive isotopes
Incorporation of protein and nucleic acid radioactive precursors into central and peripheral nervous tissue of frogs
Solid state devices, radioactive isotopes, tracer gases, and acoustical methods for use in space vehicle leak detection
Investigations in astronomy, solid state physics, optical masers, atomic physics, and radioactive atoms for electromagnetic applications
Radioactive isotope technique for heat shield ablation measurement during reentry
Radioactive nuclide activity levels and mass spectrometric measurements of rare gas isotopes in fragments of Bondoc mesosiderite
Lattice and grain boundary self-diffusion coefficients of radioactive nickel 63 into high purity nickel measured over temperature range 650-475 degrees C
Radioactive auxin to study axial curvature in terrestrial plants, retarded growth of internodes on horizontal clinostats on seedlings, and plant growth without gravity
Lunar crust radioactivity studies using Luna-13
Differential equation for parent and daughter decay influence on radioactive tracer diffusion profiles
Automatic programed scaler for measuring and processing data on radioactive materials
POODLE low thrust radioactive propulsion technology, discussing operation, mission application, tests, capsule and thrustor performance
Radioactive tracer technique for measurement of yield and angular distribution of molybdenum sputtered by cesium ion beam
Zodiacal dust explained by radioactive Al 26 deposited in marine sediments and brought by micrometeorites exposed to solar protons
Adsorption equilibrium data obtained at high pressure for methane and propane on silica gel using radioactive tracer pulsing
Radioactive contamination of the environment occurred in the early fifties as a result of the releases from the Mayak plutonium production complex (Southern Urals, Russia). The releases of liquid wastes into the Techa river resulted in chronic exposure of 30,000 residents of the riverside communities. Since 1951 90Sr body burdens have been measured for over half of this cohort. This paper presents the analysis of data on 90Sr in humans and describes the reconstruction of internal doses for these people.
The effect of radiogenic heating on the thermal evolution of spherical icy bodies with radii 1 km < R < 100 km was investigated. The radioisotopes considered were 26Al, 40K, 232Th, 235U, and 238U. Except for the 26Al abundance, which was varied, the other initial abundances were kept fixed, at values derived from those of chondritic meteorites and corresponding to a gas-to-dust ratio of 1. The initial models were homogeneous and isothermal (To = 10 K) amorphous ice spheres, in a circular orbit at 10(4) AU from the Sun. The main object of this study was to examine the conditions under which the transition temperature from amorphous into cubic ice (Ta = 137 K) would be reached. It was shown that the influence of the short-lived radionuclide 26Al dominates the effect of other radioactive species for bodies of radii up to approximately 50 km. Consequently, if we require comets to retain their ice in amorphous form, as suggested by observations, an upper limit of approximately 4 x 10(-9) is obtained for the initial 26Al abundance in comets, a factor of 100 lower than that of the inclusions in the Allende meteorite. A lower limit for the formation time of comets may thus be derived. The possibility of a coexistence of molten cometary cores and extended amorphous ice mantles is ruled out. Larger icy spheres (R > 100 km) reached Ta even in the absence of 26Al, due to the decay of the other radionuclides. As a result, a crystalline core formed whose relative size depended on the composition assumed. Thus the outermost icy satellites in the solar system, which might have been formed of ice in the amorphous state, have probably undergone crystallization and may have exhibited eruptive activity when the gas trapped in the amorphous ice was released (e.g., Miranda).
Most cosmic-ray nuclei heavier than helium have suffered nuclear collisions in the interstellar gas, with transformation of nuclear composition. The isotopic and elemental composition at the sources has to be inferred from the observed composition near the Earth. The source composition permits tests of current ideas on sites of origin, nucleosynthesis in stars, evolution of stars, the mixing and composition of the interstellar medium and injection processes prior to acceleration. The effects of nuclear spallation, production of radioactive nuclides and the time dependence of their decay provide valuable information on the acceleration and propagation of cosmic rays, their nuclear transformations, and their confinement time in the Galaxy. The formation of spallation products that only decay by electron capture and are relatively long-lived permits an investigation of the nature and density fluctuations (like clouds) of the interstellar medium. Since nuclear collisions yield positrons, antiprotons, gamma rays and neutrinos, we shall discuss these topics briefly.