Aerospace & Aviation

The distant magnetic field - infinitesimal hydromagnetic waves

Trajectories for return to earth phase of lunar missions

Aluminum oxide particle growth in nickel matrix

Slow cosmic ray neutrons in ionosphere to 200 km.

Apparent flame strength - measure of maximum reaction rate in diffusion flames

Effect of oxygen pressure on internal oxidation of nickel-aluminum alloys

Density of very concentrated nitric acid-water mixtures

Star formation in elliptical galaxies and intense radio sources

Of late, liquid hydrogen has become a very popular fuel for space missions. It is being used in such programs as Centaur and Saturn. Furthermore, hydrogen is the ideal working fluid for nuclear powered space vehicles currently under development. In these applications, liquid hydrogen fuel is generally transferred to the combustion chamber by a combination of pumping and pressurization. The pump forces the liquid propellant from the fuel tank to the combustion chamber; gaseous pressurant holds tank pressure sufficiently high to prevent cavitation at the pump inlet and to maintain the structural rigidity of the tank. The pressurizing system, composed of pressurant, tankage, and associated hardware can be a large portion of the total vehicle weight. Pressurant weight can be reduced by introducing the pressurizing gas at temperatures substantially greater than those of liquid hydrogen. Heat and mass transfer processes thereby induced complicate gas requirements during discharge. These requirements must be known to insure proper design of the pressurizing system. The aim of this paper is to develop from basic mass and energy transfer processes a general method to predict helium and hydrogen gas usage for the pressurized transfer of liquid hydrogen. This required an analytical and experimental investigation, the results of which are described in this paper.

Boundary nature of the b stars

Thickness determination of thin films by the evaporation method

Long range effects in the motion of artificial satellites

Hydrogen convective cooling of rocket nozzles

Electrode erosion in spark discharges

A scaling program was undertaken to establish the relations between performance parameters and the size of the electron bombardment ion source. The experimental results of this investigation are the subject of this paper. Two geometrically similar sources, a 5- and a 20-cm-diameter beam source, were scaled from a 10-cm-diameter source to allow a performance comparison to be made. The three ion sources are compared for ion chamber characteristics and overall engine efficiency. The results of the chamber investigations are compared with scaling variations indicated by simple plasma theory. The effects of size on operating limits are also discussed. Mercury was used as the propellant in this investigation.