Statistical specification of the 500-mb height fields using smoothed medium-resolution radiometric fields of Nimbus 2
Statistical specification of 500 mb height fields using medium resolution radiometric fields of Nimbus 2
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Statistical specification of 500 mb height fields using medium resolution radiometric fields of Nimbus 2
Heights of cloud bases and convective cloud tops determined by stereoscopic photogrammetry of Apollo 6 mission
Discrete levels of beginning height of meteors in stream
Wide range pulse height discriminator with milliwatt power drain for use in nuclear experiments on scientific satellites
Laminar boundary layer critical height determination using Rouse stability parameter
Photomultipliers single electron response by measuring electron pulse height distribution
Continuous differential energy pulse height spectra reduction to photon upper atmospheric spectra
Scientific satellites pulse height analyzer and associated threshold detection and logic circuitry
Ionospheric electron density disturbance heights measured via radio signal scintillation from earth satellite, using spaced receiver method
Lower chromosphere shock wave heating, analyzing density scale height effects
Measuring radar sea return as function of wave height and wind speed for fully developed seas
Computer programs for processing two-dimensional analyzer pulse height data for automatic separation of gamma and neutron counts
Ocean height measurement by orbit determination from satellite altimetry, considering least squares solutions and instrument errors
Height variations of Venusian cloud tops at planet equatorial and polar regions
Quantitative analysis of Gilbert's (1893) observation regarding the surface geometry of lunar craters and terrestrial calderas. Topographic measurements were made using the ratio of exterior rim height to interior crater depth, and then extended to other types of crater. The morphometric data obtained as well as those presented elsewhere (Murray et al., 1970; Guest and Murray, 1969) verify Gilbert's contention that terrestrial calderas and most rimmed lunar craters are entirely unrelated phenomena. Auxiliary characteristics previously interpreted in terms of primary volcanic cratering on the moon are either of nonendogenic origin or are secondary endogenic features superposed on initial impact landforms (Pike, 1967).
A flight-worthy pulse height analyzer that has a quadratic transfer function is described. This quadratic function permits optimum usage of the entire PHA dynamic range due to the quadratic nature of the gamma ray spectrometer's resolution vs energy. After the theoretical design discussion, the implementation of the design is examined and test results described. The analyzer is part of the University of New Hampshire gamma ray monitor for OSO-H.
Consideration is given for 26 streams of meteors classified according to Ceplecha's discrete levels of beginning height, 13 of which are associated with known comets. Comet Biela produced in the Andromedids a double-peaked distribution (Classes A and C). Apparently no known comets produce a stream of Class B. Consideration of Whipple and Stefanik's model of an icy conglomerate nucleus with radioactive heating and redistribution of ice leads to association of Ceplecha's Class C with the residue of the ice-impregnated surface of a cometary nucleus after sublimation of the ices, and of Ceplecha's Class A with the core of a cometary nucleus. Class B meteoroids are then associated with less dense cores of smaller cometary nuclei that have lost their surfaces and are too small to have been observed. It is concluded that the density of Class A meteoroids (1.2 g/cu cm) is so close to that of Type 1 carbonaceous chondrites (2 g/cu cm) as to suggest that the latter come from old cores of very large nuclei of comets, an idea originally proposed by McCrosky and Ceplecha.
The method of inferring photon spectra from an analysis of the measured pulse-height spectrum is considered along with the spectrum shape and its variation energy. The case is examined where photoelastic absorption predominates, and Compton scattering and pair production are negligible. The analytic method for obtaining the elemental composition from the observed lunar surface spectrum is described, and theoretical and calculated weight fraction fluxes for average lunar composition are tabulated.