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Dive into the research topics where Stanley H. Zisk is active.

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Featured researches published by Stanley H. Zisk.


Earth Moon and Planets | 1974

High-resolution radar maps of the lunar surface at 3.8-cm wavelength

Stanley H. Zisk; Gordon H. Pettengill; G. W. Catuna

The entire earth-facing lunar surface has been mapped at a resolution of 2 km using the 3.8-cm radar of Haystack Observatory. The observations yield the distribution of relative radar backscattering efficiency with an accuracy of about 10% for both the polarized (primarily quasispecular or coherent) and depolarized (diffuse or incoherent) scattered components. The results show a variety of discrete radar features, many of which are correlated with craters or other features of optical photographs. Particular interest, however, attaches to those features with substantially different radio and optical contrasts. An anomaly near 63° is noted in the mean angular scattering law obtained from a summary of the radar data.


Earth Moon and Planets | 1977

The Aristarchus-Harbinger region of the moon: Surface geology and history from recent remote-sensing observations

Stanley H. Zisk; Carroll Ann Hodges; H. J. Moore; R. W. Shorthill; T. W. Thompson; Ewen A. Whitaker; Don E. Wilhelms

The region including the Aristarchus Plateau and Montes Harbinger is probably the most diverse, geologically, of any area of comparble size on the Moon. This part of the northwest quadrant of the lunar near side includes unique dark mantling material; both the densest concentration and the largest of the sinuous rilles; apparent volcanic vents, sinks, and domes; mare materials of various ages and colors; one of the freshest large craters (Aristarchus) with ejecta having unique colors and albedos; and three other large craters in different states of flooding and degradation (krieger, Herodotus, and Prinz). The three best-authenticated lunar transient phenomena were also observed here.This study is based principally on photographic and remote sensing observations made from Earth and Apollo orbiting space craft. Results include (1) delineation of geologic map units and their stratigraphic relationships; (2) discussion of the complex interrelationships between materials of volcanic and impact origin, including the effects of excavation, redistribution and mixing of previously deposited materials by younger impact craters; (3) deduction of physical and chemical properties of certain of the geologic units, based on both the remote-sensing information and on extrapolation of Apollo data to this area; and (4) development of a detailed geologic history of the region, outlining the probable sequence of events that resulted in its present appearance.A primary concern of the investigation has been anomalous red dark mantle on the Plateau. Based on an integration of Earth- and lunar orbit-based data, this layer seems to consist of fine-grained, block-free material containing a relatively large fraction of orange glass. It is probably of pyroclastic origin, laid down at some time during the Imbrian period of mare flooding.


Earth Moon and Planets | 1974

A comparison of infrared, radar, and geologic mapping of lunar craters

T. W. Thompson; Harold Masursky; R. W. Shorthill; G. L. Tyler; Stanley H. Zisk

Between 1000 and 2000 infrared (eclipse) and radar anomalies have been mapped on the nearside hemisphere of the Moon. A study of 52 of these anomalies indicates that most are related to impact craters and that the nature of the infrared and radar responses is compatible with a previously developed geologic model of crater aging processes. The youngest craters are pronounced thermal and radar anomalies; that is, they have enhanced eclipse temperatures and are strong radar scatterers. With increasing crater age, the associated thermal and radar responses become progressively less noticeable until they assume values for the average lunar surface. The last type of anomaly to disappear is radar enhancement at longer wavelengths. A few craters, however, have infrared and radar behaviors not predicted by the aging model. One previously unknown feature - a field strewn with centimeter-sized rock fragments - has been identified by this technique of comparing maps at the infrared, radar, and visual wavelengths.


Earth Moon and Planets | 1975

Lava flows in mare imbrium: An evaluation of anomalously low earth-based radar reflectivity

Gerald G. Schaber; T. W. Thompson; Stanley H. Zisk

The lunar maria reflect two to five times less Earth-based radar power than the highlands, the spectrally blue maria surfaces returning the lowest power levels. This effect of weakening signal return has been attributed to increased signal absorption related to the electrical and magnetic characteristics of the mineral ilmenite (FeTiO3).The surface of Mare Imbrium contains some of the most distinct red-blue colorimetric boundaries and depolarized 70 cm wavelength reflectivity variations on the near side of the Moon. The weakest levels of both 3.8 cm and 70 cm reflectivity within Imbrium are confined to regional mare surfaces of the blue spectral type that can be recognized as stratigraphically unique flow surfaces. Frequency distributions of the 70 cm polarized and depolarized radar return power for five mare surfaces within the basin indicate that signal absorption, and probably the ilmenite content, increases generally from the beginning of the Imbrian Period to the end of the Eratosthenian Period with slight reversal between the end of the Imbrian and beginning of the Eratosthenian.TiO2 calibrated radar reflectivity curves can be utilized for lunar maria geochemical mapping in the same manner as the TiO2 calibrated spectral reflectivity curves of Charetteet al. (1974). The long wavelength radar data may be a sensitive indicator of mare chemical variations as it is unaffected by the normal surface rock clutter that includes ray materials from large impact craters.


Earth Moon and Planets | 1979

Blocky craters: Implications about the lunar megaregolith

Thomas W. Thompson; W. J. Roberts; W. K. Hartmann; R. W. Shorthill; Stanley H. Zisk

Radar, infrared, and photogeologic properties of lunar craters have been studied to determine whether there is a systematic difference in blocky craters between the maria and terrae and whether this difference may be due to a deep megaregolith of pulverized material forming the terra surface, as opposed to a layer of semi-coherent basalt flows forming the mare surface. Some 1310 craters from about 4 to 100 km diameter have been catalogued as radar and/or infrared anomalies. In addition, a study of Apollo Orbital Photography confirmed that the radar and infrared anomalies are correlated with blocky rubble around the crater.Analysis of the radar and infrared data indicated systematic terra—mare differences. Fresh terra craters smaller than 12 km were less likely to be infrared and radar anomalies than comparable mare craters: but terra and mare craters larger than 12 km had similar infrared and radar signatures. Also, there are many terra craters which are radar bright but not infrared anomalies.Our interpretation of these data is that while the maria are rock layers (basaltic flow units) where craters eject boulder fields, the terrae are covered by relatively pulverized megaregolith at least 2 km deep, where craters eject less rocky rubble. Blocky rubble, either in the form of actual rocks or partly consolidated blocks, contributes to the radar and infrared signatures of the crater. However, aging by impacts rapidly destroys these effects, possibly through burial by secondary debris or by disintegration of the blocks themselves, especially in terra regions.


Earth Moon and Planets | 1974

The mapping of lunar radar scattering characteristics

Gordon H. Pettengill; Stanley H. Zisk; T. W. Thompson

This is the first of four articles describing a comprehensive series of radar maps of the entire visible lunar hemisphere carried out at wavelengths of 3.8 and 70 cm and analyzing the echoes in both orthogonal senses of circular polarization. In this paper, the basic techniques of delay-Doppler mapping by radar are developed, and the particular steps employed in mapping the Moon are outlined. Succeeding articles present the results obtained and discuss the way in which these results relate to other, nonradar measurements as well as to the actual lunar surface properties.


Science | 1971

Lunar apennine-hadley region: geological inplications of Earth-based radar and infrared measurements.

Stanley H. Zisk; Michael H. Carr; Harold Masursky; R. W. Shorthill; T. W. Thompson

Recently completed high-resolution radar maps of the moon contain information on the decimeter-scale structure of the surface. When this information is combined with eclipse thermal-enhancement data and with high-resolution Lunar Orbiter photography, the surface morphology is revealed in some detail. A geological history for certain features and subareas can be developed, which provides one possible framework for the interpretation of the findings from the Apollo 15 landing. Frequency of decimeter-and meter-size blocks in and around lunar craters, given by the remote-sensed data, supports a multilayer structure in the Palus Putredinis mare region, as well as a great age for the bordering Apennine Mountains scarp.


Earth Moon and Planets | 1974

Mare serenitatis: a preliminary definition of surface units by remote observations

T. W. Thompson; R. W. Shorthill; Ewen A. Whitaker; Stanley H. Zisk

There are many surface units in Mare Serenitatis and in the adjacent Montes Haemus that can be defined by remote, Earth-based observations at visual, infrared, and radar wavelengths. These highland and mare surface units are obvious in color-difference photographs and in radar images, while the infrared images have little or no differences. These characteristics are consistent with units having definite chemical differences. However, a better definition of these surfaces requires the synthesis of many more data sets.


Optics, Illumination, and Image Sensing for Machine Vision II | 1988

Camera Edge Response

Stanley H. Zisk; Norman Wittels

Edge location is an important machine vision task. Machine vision systems perform mathematical operations on rectangular arrays of numbers that are intended to faithfully represent the spatial distribution of scene luminance. The numbers are produced by periodic sampling and quantization of the cameras video output. This sequence can cause artifacts to appear in the data with a noise spectrum that is high in power at high spatial frequencies. This is a problem because most edge detection algorithms are preferentially sensitive to the high-frequency content in an image. Solid state cameras can introduce errors because of the spatial periodicity of their sensor elements. This can result in problems when image edges are aligned with camera pixel boundaries: (a) some cameras introduce transients into the video signal while switching between sensor elements; (b) most cameras use analog low-pass filters to minimize sampling artifacts and these introduce video phase delays that shift the locations of edges. The problems compound when the vision system samples asynchronously with the cameras pixel rate. Moire patterns (analogous to beat frequencies) can result. In this paper, we examine and model quantization effects in a machine vision system with particular emphasis on edge detection performance. We also compare our models with experimental measurements.


Optics, Illumination, and Image Sensing for Machine Vision | 1987

Lighting Design for Industrial Machine Vision

Norman Wittels; Stanley H. Zisk

The purpose of the lighting in an industrial machine vision application is to produce an image that is well matched to the camera and vision system. The brightest areas of the scene should cause a sensor illuminance that is just below the cameras saturation level and the video signal from the darkest significant areas of the scene should lie just above the vision systems noise level. This paper describes the fundamental principles and the techniques used to design lighting that meets these requirements. The cameras transfer function, the vision systems noise level, and the relative lens aperture are used to calculate optimal luminances for the brightest and darkest areas in the scene. The necessary reflectivity coefficients for the objects in the scene are measured and lighting is designed which produces the correct object luminances in both the specular highlights and the diffuse background areas of the scene. We show how to specify the light sources required to produce the lighting and present an example of printed circuit board inspection. The burden that this design method places on the vision algorithms is also discussed.

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T. W. Thompson

Jet Propulsion Laboratory

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Martin A. Slade

California Institute of Technology

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Norman Wittels

Worcester Polytechnic Institute

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Alan E. E. Rogers

Massachusetts Institute of Technology

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Gordon H. Pettengill

Massachusetts Institute of Technology

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Harold Masursky

United States Geological Survey

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Raymond F. Jurgens

California Institute of Technology

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