D. N. Sweetnam
California Institute of Technology
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Featured researches published by D. N. Sweetnam.
Icarus | 1983
Gunnar F. Lindal; G. E. Wood; H.B. Hotz; D. N. Sweetnam; Von R. Eshleman; G. L. Tyler
Abstract Two coherently related radio signals transmitted from Voyager 1 at wavelengths of 13 cm (S-band) and 3.6 cm (X-band) were used to probe the equatorial atmosphere of Titan. The measurements were conducted during the occultation of the spacecraft by the satellite on November 12, 1980. An analysis of the differential dispersive frequency measurements did not reveal any ionization layers in the upper atmosphere of Titan. The resolution was approximately 3 × 10 3 and 5 × 10 3 electrons/cm 3 near the evening and morning terminators, respectively. Abrupt signal changes observed at ingress and egress indicated a surface radius of 2575.0 ± 0.5 km, leading to a mean density of 1.881 ± 0.002 g cm −3 for the satellite. The nondispersive data were used to derive profiles in height of the gas refractivity and microwave absorption in Titans troposphere and stratosphere. No absorption was detected; the resolution was about 0.01 dB/km at the 13-cm wavelength. The gas refractivity data, which extend from the surface to about 200 km altitude, were interpreted in two different ways. In the first, it is assumed that N 2 makes up essentially all of the atmosphere, but with very small amounts of CH 4 and other hydrocarbons also present. This approach yielded a temperature and pressure at the surface of 94.0 ± 0.7°K and 1496 ± 20 mbar, respectively. The tropopause, which was detected near 42 km altitude, had a temperature of 71.4 ± 0.5°K and a pressure of about 130 mbar. Above the tropopause, the temperature increased with height, reaching 170 ± 15°K near the 200-km level. The maximum temperature lapse rate observed near the surface (1.38 ± 0.10°K/km) corresponds to the adiabatic value expected for a dry N 2 atmosphere—indicating that methane saturation did not occur in tbis region. Above the 3.5-km altitude level the lapse rate dropped abruptly to 0.9 ± 0.1°K/km and then decreased slowly with increasing altitude, crossing zero at the tropopause. For the N 2 atmospheric model, the lapse rate transition at the 3.5-km level appears to mark the boundary between a convective region near the surface having the dry adiabatic lapse rate, and a higher stable region in radiative equilibrium. In the second interpretation of the refractivity data, it is assumed, instead, that the 3.5 km altitude level corresponds to the bottom of a CH 4 cloud layer, and that N 2 and CH 4 are perfectly mixed below this level. These assumptions lead to an atmospheric model which below the clouds contains about 10% CH 4 by number density. The temperature near the surface is about 95°K. Arguments concerning the temperature lapse rates computed from the radio measurements appear to favor models in which methane forms at most a limited haze layer high in the troposphere.
Science | 1974
H. T. Howard; G. L. Tyler; Gunnar Fjeldbo; A. J. Kliore; G. S. Levy; D. L. Brunn; R. Dickinson; Robert E. Edelson; W. L. Martin; R. B. Postal; B. L. Seidel; T.T. Sesplaukis; D. L. Shirley; C. T. Stelzried; D. N. Sweetnam; A. I. Zygielbaum; P. B. Esposito; J. D. Anderson; Irwin I. Shapiro; Robert D. Reasenberg
Analysis of the Doppler tracking data near encounter yields a value for the ratio of the mass of the sun to that of Venus of 408,523.9 � 1.2, which is in good agreement with prior determinations based on data from Mariner 2 and Mariner 5. Preliminary analysis indicates that the magnitudes of the fractional differences in the principal moments of inertia of Venus are no larger than 10-4, given that the effects of gravity-field harmonics higher than the second are negligible. Additional analysis is needed to determine the influence of the higher order harmonics on this bound. Four distinct temperature inversions exist at altitudes of 56, 58, 61, and 63 kilometers. The X-band signal was much more rapidly attenuated than the S-band signal and disappeared completely at 52-kilometer altitude. The nightside ionosphere consists of two layers having a peak density of 104 electrons per cubic centimeter at altitudes of 140 and 120 kilometers. The dayside ionosphere has a peak density of 3 X 105 electrons per cubic centimeter at an altitude of 145 kilometers. The electron number density observed at higher altitudes was ten times less than that observed by Mariner 5, and no strong evidence for a well-defined plasmapause was found.
Science | 1986
G. L. Tyler; D. N. Sweetnam; John D. Anderson; J. K. Campbell; Von R. Eshleman; David P. Hinson; G. S. Levy; Gunnar F. Lindal; Essam A. Marouf; Richard A. Simpson
Voyager 2 radio occultation measurements of the Uranian atmosphere were obtained between 2 and 7 degrees south latitude. Initial atmospheric temperature profiles extend from pressures of 10 to 900 millibars over a height range of about 100 kilometers. Comparison of radio and infrared results yields mole fractions near the tropopause of 0.85 and 0.15 � 0.05 for molecular hydrogen and helium, respectively, if no other components are present; for this composition the tropopause is at about 52 kelvins and 110 millibars. Distinctive features in the signal intensity measurements for pressures above 900 millibars strongly favor model atmospheres that include a cloud deck of methane ice. Modeling of the intensity measurements for the cloud region and below indicates that the cloud base is near 1,300 millibars and 81 kelvins and yields an initial methane mole fraction of about 0.02 for the deep atmosphere. Scintillations in signal intensity indicate small-scale stucture throughout the stratosphere and upper troposphere. As judged from data obtained during occultation ingress, the ionosphere consists of a multilayer structure that includes two distinct layers at 2,000 and 3,500 kilometers above the 100-millibar level and an extended topside that may reach altitudes of 10,000 kilometers or more. Occultation measurements of the nine previously known rings at wavelengths of 3.6 and 13 centimeters show characteristic values of optical depth between about 0.8 and 8; the maxim value occurs in the outer region of the ∈ ring, near its periapsis. Forward-scattered signals from this ring have properties that differ from those of any of Saturns rings, and they are inconsistent with a discrete scattering object or local (three-dimensional) assemblies of orbiting objects. These signals suggest a new kdnd of planetary ring feature characterized by highly ordered cylindrical substructures of radial scale on the order of meters and azimuthal scale of kilometers or more. From radio data alone the mass of the Uranian system is GMsys = 5,794,547– 60 cubic kilometers per square second; from a combination of radio and optical navigation data the mass of Uranus alone is GMu = 5,793,939� 60 cubic kilometers per square second. From all available Voyager data, induding imaging radii, the mean uncompressed density of the five major satellites is 1.40� 0.07 grams per cubic centimeter; this value is consistent with a solar mix of material and apparently rules out a cometary origin of the satellites.
Icarus | 1975
A. J. Kliore; Gunnar Fjeldbo; B. L. Seidel; D. N. Sweetnam; T.T. Sesplaukis; Peter M. Woiceshyn; S.I. Rasool
Abstract The occultation of the Pioneer 10 spacecraft by Io (JI) provided an opportunity to obtain two S -band radio occultation measurements of its atmosphere. The dayside entry measurements revealed an ionosphere having a peak density of about 6 × 10 4 elcm −3 at an altitude of about 100 km. The topside scale height indicates a plasma temperature of about 406 K if it is composed of Na + and 495 K if N 2 + is principal ion. A thinner and less dense ionosphere was observed on the exit (night side), having a peak density of 9 × 10 3 elcm −3 at an altitude of 50 km. The topside plasma temperature is 160 K for N 2 − and 131 K for Na + . If the ionosphere is produced by photoionization in a manner analogous to the ionospheres of the terrestrial planets, the density of neutral particles at the surface of Io is less than 10 11 −10 12 cm 3 , corresponding to a surface pressure of less than 10 −8 to 10 −9 bars. Two measurements of its radius were also obtained yielding a value of 1830 km for the entry and 192 km for the exit. The discrepancy between these values may indicate an ephemeris uncertainty of about 45 km. The two measurements yield an average radius of 1875 km, which is not in agreement with the results of the Beta Scorpii stellar occultation.
Science | 1980
Arvydas J. Kliore; Gunnar F. Lindal; Indu R. Patel; D. N. Sweetnam; Henry B. Hotz; Thomas R. Mcdonough
Radio occultation measurements at S band (2.293 gigahertz) of the ionosphere and upper neutral atmosphere of Saturn were obtained during the flyby of the Pioneer 11 Saturn spacecraft on 5 September 1979. Preliminary analysis of the occultation exit data taken at a latitude of 9.5�S and a solar zenith angle of 90.6� revealed the presence of a rather thin ionosphere, having a main peak electron density of about 9.4 x 10/3 per cubic centimeter at an altitude of about 2800 above the level of a neutral number density of 1019 per cubic centimeter and a lower peak of about 7 x 103 per cubic centimeter at 2200 kilometers. Data in the neutral atmosphere were obtained to a pressure level of about 120 millibars. The temperature structure derived from these data is consistent with the results of the Pioneer 11 Saturn infrared radiometer experiment (for a helium fraction of 15 percent) and with models derived from Earth-based observations for a helium fraction by number of about 4 to 10 percent. The helium fraction will be further defined by mutual iteration with the infrared radiometer team.
Science | 1976
William H. Michael; A. P. Mayo; W. T. Blackshear; R. H. Tolson; G. M. Kelly; J. P. Brenkle; Dan L. Cain; Gunnar Fjeldbo; D. N. Sweetnam; R.B. Goldstein; P. E. Macneil; Rabert D. Reasenberg; Irwin I. Shapiro; T. I. S. Boak; M. D. Grossi; C. H. Tang
Approximately 3 months of radio tracking data from the Viking landers have been analyzed to determine the lander locations, the orientation of the spin axis of Mars, and a first estimate from Viking data of the planets spin rate. Preliminary results have also been obtained for atmospheric parameters and radii at occultation points and for properties of the surface in the vicinity of lander 1.
Journal of Geophysical Research | 1981
Gunnar F. Lindal; G. E. Wood; G. S. Levy; John D. Anderson; D. N. Sweetnam; H. B. Hotz; B. J. Buckles; D. P. Holmes; P. E. Doms; Von R. Eshleman; G. L. Tyler; T. A. Croft
Journal of Geophysical Research | 1987
Gunnar F. Lindal; J. R. Lyons; D. N. Sweetnam; Von R. Eshleman; David P. Hinson; G. L. Tyler
Science | 1989
G. L. Tyler; D. N. Sweetnam; John D. Anderson; S. E. Borutzki; J. K. Campbell; Von R. Eshleman; D. L. Gresh; E.M. Gurrola; David P. Hinson; N. Kawashima; E. R. Kursinski; G. S. Levy; Gunnar F. Lindal; J. R. Lyons; Essam A. Marouf; Paul Alan Rosen; Richard A. Simpson; G. E. Wood
Journal of Geophysical Research | 1979
Gunnar F. Lindal; Henry B. Hotz; D. N. Sweetnam; Zvi Shippony; Joseph P. Brenkle; Gene V. Hartsell; Richard T. Spear; William Michael