Measurement of the transmissivity of a carbon-particle-seeded nitrogen jet
Transmissivity of carbon particle-seeded nitrogen jet for heat transfer predictions
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Transmissivity of carbon particle-seeded nitrogen jet for heat transfer predictions
Germ-free seeds, seedlings, plants, tissues, and cell lines for lunar receiving laboratory, including algal and vascular plant systems
Sodium-potassium seeded argon plasma in electric field measured for electrical conductivity
Mercury or cadmium seeding effects on performance of cesium plasma diodes, obtaining plasma electron temperature from mathematical model
Thermal absorption in aerosol seeded hydrogen and helium gases
Photoionization cross section measurements for sodium line by analyzing electron-ion recombination radiation from sodium seeded plasma, determining electron temperatures and concentrations
Radiant heat transfer properties of particle seeded gases, including absorption and scattering characteristics of carbon, silicon, and tungsten
Cs seeding effect on bound-free UV photoabsorption of Cs-H plasma at constant electron density and energies below H ionization
Hg and Cd seeded Ce plasma wide-spaced diode without external light source investigated for Penning effect on diode performance
Investigating inhibitory activity of lichens on growth of seed plants and ferns
Electron kinetics in plasmas produced by neutron irradiation of nuclear seeded noble gases
Performance of helium seeded with uranium in magnetohydrodynamic generator
Nonlinear effects of recombination and collective diffusion associated with nuclear seeded plasmas using helium isotopes in gas cooled reactors
Cs plasma thermionic diode, using Penning effect for ionization rate increase via Hg or Cd seeding
The equations giving the response of a slightly ionized plasma with monatomic components to sinusoidal perturbations have been formulated. Included in the model equations were the electron Hall effect, electron thermal diffusion, radiation, and electron-atom rate processes. Plasma conditions were limited to those where viscous effects, the induced magnetic field, ion slip, and atom-atom inelastic processes can be neglected. Presented are results of numerical calculations for MHD generators with a working fluid of potassium seeded argon.
Two Skylark sounding rockets carrying chemical seeding payloads were launched from Woomera, South Australia (31 S, 137 E) in October 1969. In conjunction with these firings, the University of Adelaide conducted ground-based experiments on the upper atmosphere using the radio meteor and spaced receiver drift methods. This paper presents the measurements of properties of the neutral atmosphere above 90 km which were obtained from these experiments.
The author has identified the following significant results. The near real-time DCS platform data transfer to the time-share compare is a working reality. Six stations are now being automatically monitored and displayed with a system delay of 3 to 8 hours from time of data transmission to time of data accessibility on the computer. The DCS platform system has proven itself a valuable tool for near real-time monitoring of mountain precipitation. Data from Wolf Creek Pass were an important input in making the decision when to suspend seeding operations to avoid exceeding suspension criteria in that area. The DCS platforms, as deployed in this investigation, have proven themselves to be reliable weather resistant systems for winter mountain environments in the southern Colorado mountains.
An experimental investigation was conducted using the United Technologies Research Center (UTRC) 80 kW and 1.2 MW RF induction heater systems to aid in developing the technology necessary for designing a self-critical fissioning uranium plasma core reactor (PCR). A nonfissioning, steady-state RF-heated argon plasma seeded with pure uranium hexafluoride (UF6) was used. An overall objective was to achieve maximum confinement of uranium vapor within the plasma while simultaneously minimizing the uranium compound wall deposition. Exploratory tests were conducted using the 80 kW RF induction heater with the test chamber at approximately atmospheric pressure and discharge power levels on the order of 10 kW. Four different test chamber flow configurations were tested to permit selection of the configuration offering the best confinement characteristics for subsequent tests at higher pressure and power in the 1.2 MW RF induction heater facility.