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Dive into the research topics where Donald J. Banfield is active.

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Featured researches published by Donald J. Banfield.


Science | 1989

Voyager 2 at Neptune: Imaging Science Results

Bradford A. Smith; L. A. Soderblom; Donald J. Banfield; c. Barnet; A. T. Basilevsky; R. F. Beebe; K. Bollinger; Joseph M. Boyce; Andre Brahic; Geoffrey Briggs; Robert H. Brown; Christopher F. Chyba; Stewart A. Collins; Allan F. Cook; David Crisp; Steven K. Croft; Dale P. Cruikshank; Jeffrey N. Cuzzi; G. E. Danielson; Merton E. Davies; E. De Jong; Luke Dones; David Godfrey; J. Goguen; I. Grenier; V. R. Haemmerle; Heidi B. Hammel; Carl J. Hansen; c. P. Helfenstein; C. Howell

Voyager 2 images of Neptune reveal a windy planet characterized by bright clouds of methane ice suspended in an exceptionally clear atmosphere above a lower deck of hydrogen sulfide or ammonia ices. Neptunes atmosphere is dominated by a large anticyclonic storm system that has been named the Great Dark Spot (GDS). About the same size as Earth in extent, the GDS bears both many similarities and some differences to the Great Red Spot of Jupiter. Neptunes zonal wind profile is remarkably similar to that of Uranus. Neptune has three major rings at radii of 42,000, 53,000, and 63,000 kilometers. The outer ring contains three higher density arc-like segments that were apparently responsible for most of the ground-based occultation events observed during the current decade. Like the rings of Uranus, the Neptune rings are composed of very dark material; unlike that of Uranus, the Neptune system is very dusty. Six new regular satellites were found, with dark surfaces and radii ranging from 200 to 25 kilometers. All lie inside the orbit of Triton and the inner four are located within the ring system. Triton is seen to be a differentiated body, with a radius of 1350 kilometers and a density of 2.1 grams per cubic centimeter; it exhibits clear evidence of early episodes of surface melting. A now rigid crust of what is probably water ice is overlain with a brilliant coating of nitrogen frost, slightly darkened and reddened with organic polymer material. Streaks of organic polymer suggest seasonal winds strong enough to move particles of micrometer size or larger, once they become airborne. At least two active plumes were seen, carrying dark material 8 kilometers above the surface before being transported downstream by high level winds. The plumes may be driven by solar heating and the subsequent violent vaporization of subsurface nitrogen.


Science | 2004

Atmospheric Imaging Results from the Mars Exploration Rovers: Spirit and Opportunity

Mark T. Lemmon; M. J. Wolff; Michael D. Smith; R. T. Clancy; Donald J. Banfield; Geoffrey A. Landis; Amitabha Ghosh; Peter W. H. Smith; N. Spanovich; Barbara A. Whitney; P. L. Whelley; Ronald Greeley; Shane D. Thompson; James F. Bell; S. W. Squyres

A visible atmospheric optical depth of 0.9 was measured by the Spirit rover at Gusev crater and by the Opportunity rover at Meridiani Planum. Optical depth decreased by about 0.6 to 0.7% per sol through both 90-sol primary missions. The vertical distribution of atmospheric dust at Gusev crater was consistent with uniform mixing, with a measured scale height of 11.56 ± 0.62 kilometers. The dusts cross section weighted mean radius was 1.47 ± 0.21 micrometers (μm) at Gusev and 1.52 ± 0.18 μ at Meridiani. Comparison of visible optical depths with 9-μ optical depths shows a visible-to-infrared optical depth ratio of 2.0 ± 0.2 for comparison with previous monitoring of infrared optical depths.


Nature | 2005

Aeolian processes at the Mars Exploration Rover Meridiani Planum landing site

R. Sullivan; Donald J. Banfield; James F. Bell; Wendy M. Calvin; David A. Fike; M. P. Golombek; Ronald Greeley; John P. Grotzinger; K. E. Herkenhoff; Douglas J. Jerolmack; M. C. Malin; D. W. Ming; L. A. Soderblom; S. W. Squyres; Shane D. Thompson; Wesley Andres Watters; Catherine M. Weitz; Albert S. Yen

The martian surface is a natural laboratory for testing our understanding of the physics of aeolian (wind-related) processes in an environment different from that of Earth. Martian surface markings and atmospheric opacity are time-variable, indicating that fine particles at the surface are mobilized regularly by wind. Regolith (unconsolidated surface material) at the Mars Exploration Rover Opportunitys landing site has been affected greatly by wind, which has created and reoriented bedforms, sorted grains, and eroded bedrock. Aeolian features here preserve a unique record of changing wind direction and wind strength. Here we present an in situ examination of a martian bright wind streak, which provides evidence consistent with a previously proposed formational model for such features. We also show that a widely used criterion for distinguishing between aeolian saltation- and suspension-dominated grain behaviour is different on Mars, and that estimated wind friction speeds between 2 and 3 m s-1, most recently from the northwest, are associated with recent global dust storms, providing ground truth for climate model predictions.


Nature | 2000

Observation of moist convection in Jupiter's atmosphere

Peter J. Gierasch; Andrew P. Ingersoll; Donald J. Banfield; S. P. Ewald; Paul Helfenstein; A. Simon-Miller; Ashwin R. Vasavada; H. H. Breneman; David A. Senske

The energy source driving Jupiters active meteorology is not understood. There are two main candidates: a poorly understood internal heat source and sunlight. Here we report observations of an active storm system possessing both lightning and condensation of water. The storm has a vertical extent of at least 50 km and a length of about 4,000 km. Previous observations of lightning on Jupiter have revealed both its frequency of occurrence and its spatial distribution, but they did not permit analysis of the detailed cloud structure and its dynamics. The present observations reveal the storm (on the day side of the planet) at the same location and within just a few hours of a lightning detection (on the night side). We estimate that the total vertical transport of heat by storms like the one observed here is of the same order as the planets internal heat source. We therefore conclude that moist convection—similar to large clusters of thunderstorm cells on the Earth—is a dominant factor in converting heat flow into kinetic energy in the jovian atmosphere.


Science | 1996

Galileo's First Images of Jupiter and the Galilean Satellites

M. J. S. Belton; James W. Head; A. P. Ingersoll; Ronald Greeley; Alfred S. McEwen; Kenneth P. Klaasen; David A. Senske; Robert T. Pappalardo; G. C. Collins; Ashwin R. Vasavada; Robert John Sullivan; D. P. Simonelli; P. E. Geissler; Michael H. Carr; Merton E. Davies; J. Veverka; Peter J. Gierasch; Donald J. Banfield; M. Bell; Clark R. Chapman; Clifford D. Anger; Richard Greenberg; G. Neukum; Carl B. Pilcher; R. F. Beebe; Joseph A. Burns; Fraser P. Fanale; W. Ip; Torrence V. Johnson; David R. Morrison

The first images of Jupiter, Io, Europa, and Ganymede from the Galileo spacecraft reveal new information about Jupiters Great Red Spot (GRS) and the surfaces of the Galilean satellites. Features similar to clusters of thunderstorms were found in the GRS. Nearby wave structures suggest that the GRS may be a shallow atmospheric feature. Changes in surface color and plume distribution indicate differences in resurfacing processes near hot spots on Io. Patchy emissions were seen while Io was in eclipse by Jupiter. The outer margins of prominent linear markings (triple bands) on Europa are diffuse, suggesting that material has been vented from fractures. Numerous small circular craters indicate localized areas of relatively old surface. Pervasive brittle deformation of an ice layer appears to have formed grooves on Ganymede. Dark terrain unexpectedly shows distinctive albedo variations to the limit of resolution.


Nature | 2000

Moist convection as an energy source for the large-scale motions in Jupiter's atmosphere

Andrew P. Ingersoll; Peter J. Gierasch; Donald J. Banfield; Ashwin R. Vasavada

Jupiters dominant large-scale weather patterns (dimensions ∼10,000 km) are zonal jets and long-lived ovals. The jets have been flowing east and west at constant speeds of up to 180 m s-1 for over 100 years. These jets receive energy from small-scale eddies, which pump eastward momentum into the eastward jets and westward momentum into the westward jets. This momentum transfer was predicted by numerical models before it was observed on Jupiter. The large ovals roll between the jets in an anticyclonic direction—clockwise in the northern hemisphere and counterclockwise in the southern hemisphere—where they regularly assimilate small anticyclonic eddies. But from where the eddies receive their energy has been an open question. Here we argue that the eddies, which ultimately drive both the jets and the ovals, receive their energy from moist convection. This hypothesis is consistent with observations of jovian lightning, which is an indicator of moist convection. It also explains the anticyclonic rotation and poleward drift of the eddies, and suggests patterns of upwelling and downwelling that resemble the patterns of large-scale axisymmetric overturning in the Earths atmosphere.


Icarus | 2003

Forced waves in the martian atmosphere from MGS TES nadir data

Donald J. Banfield; Barney J. Conrath; M. D. Smith; Philip R. Christensen; R. John Wilson

Abstract We have analyzed the temperature retrievals from Mars Global Surveyor (MGS) Thermal Emission Spectrometer (TES) nadir spectra to yield latitude-height resolved maps of various atmospheric forced wave modes as a function of season for a full Mars year. Among the isolated wave modes is the zonal mean, time mean temperature, which we used to derive zonal mean zonal winds and stationary wave quasi-geostrophic indices of refraction, diagnostic of their propagation. The diurnal Kelvin wave was isolated in the data, with results roughly consistent with models (Wilson and Hamilton, 1996 , J. Atmos. Sci. 33, 1290–1326). The s = 1 and s = 2 stationary waves were found to have significant amplitude in ducts extending up the winter polar jets, while the s = 3 stationary wave was found to be confined to near the surface. The s = 1 stationary wave was found to have little phase tilt with height during northern winter, but significant westward phase tilt with height in the southern winter. This indicates that the wave carries heat poleward, slightly more than that found in Barnes et al. (1996 ; J. Geophys. Res. 101, 12,753–12,776). The s = 1 stationary wave is likely the dominant mechanism for eddy meridional heat transport for the southern winter. We noted that the phase of the s = 2 stationary wave is nearly constant with time, but that the s = 1 stationary wave moved 90° of longitude from fall to winter and back in spring in the North. While interannual variability is not yet addressed, overall, these results provide the first comprehensive benchmark for forced waves in Mars’s atmosphere against which future atmospheric models of Mars can be compared.


Science | 1989

Neptune's Story

Peter Goldreich; Norman Murray; P. Y. Longaretti; Donald J. Banfield

It is conjectured that Triton was captured from a heliocentric orbit as the result of a collision with what was then one of Neptunes regular satellites. The immediate post-capture orbit was highly eccentric with a semimajor axis a ∼ 103RN and a periapse distance rp that oscillated periodically above a minimum value of about 5RN. Dissipation due to tides raised by Neptune in Triton caused Tritons orbit to evolve to its present state in ≲109 years. For much of this time Triton was almost entirely molten. While its orbit was evolving, Triton cannibalized most of the regular satellites of Neptune and also perturbed Nereid, thus accounting for that satellites highly eccentric and inclined orbit. The only regular satellites of Neptune that survived were those that formed well within 5RN and they move on inclined orbits as the result of chaotic perturbations forced by Triton. Neptunes arcs are confined around the corotation resonances of one of these inner satellites. The widths and lengths of the arcs imply that the satellites radius is at least 30/(sin i)2/3 kilometers for i ≲ 1, where i is the angle of inclination.


Science | 2004

First Atmospheric Science Results from the Mars Exploration Rovers Mini-TES

Michael D. Smith; Michael J. Wolff; Mark T. Lemmon; N. Spanovich; Donald J. Banfield; Charles John Budney; R. Todd Clancy; Amitabha Ghosh; Geoffrey A. Landis; Peter W. H. Smith; Barbara A. Whitney; Philip R. Christensen; Steven W. Squyres

Thermal infrared spectra of the martian atmosphere taken by the Miniature Thermal Emission Spectrometer (Mini-TES) were used to determine the atmospheric temperatures in the planetary boundary layer and the column-integrated optical depth of aerosols. Mini-TES observations show the diurnal variation of the martian boundary layer thermal structure, including a near-surface superadiabatic layer during the afternoon and an inversion layer at night. Upward-looking Mini-TES observations show warm and cool parcels of air moving through the Mini-TES field of view on a time scale of 30 seconds. The retrieved dust optical depth shows a downward trend at both sites.


Journal of Geophysical Research | 2009

Thermal tides in the Martian middle atmosphere as seen by the Mars Climate Sounder

Cin-Ty A. Lee; W. G. Lawson; Mark I. Richardson; Nicholas G. Heavens; Armin Kleinböhl; Donald J. Banfield; Daniel J. McCleese; Richard W. Zurek; David Michael Kass; John T. Schofield; Conway B. Leovy; F. W. Taylor; Anthony Domenick Toigo

The first systematic observations of the middle atmosphere of Mars (35km-80km) with the Mars Climate Sounder (MCS) show dramatic patterns of diurnal thermal variation, evident in retrievals of temperature and water ice opacity. At the time of writing, the dataset of MCS limb retrievals is sufficient for spectral analysis within a limited range of latitudes and seasons. This analysis shows that these thermal variations are almost exclusively associated with a diurnal thermal tide. Using a Martian General Circulation Model to extend our analysis we show that the diurnal thermal tide dominates these patterns for all latitudes and all seasons.

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Andrew P. Ingersoll

California Institute of Technology

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M. D. Smith

California Institute of Technology

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Michael D. Smith

Goddard Space Flight Center

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Anthony Domenick Toigo

Johns Hopkins University Applied Physics Laboratory

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