Atmospheric Refraction: a History
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Atmospheric Refraction
Z w o :::> l I ~ <x: '----1-'-1----- WAVE FR ON T Z = -rnX + Zal rn = tan e '----------------------X HORIZONTAL POSITION de = ~~ = (~~) tan8dz v FIG. 1. Origin of atmospheric refraction. DR. SIDNEY BERTRAM The Bunker-Ramo Corp. Canoga Park, Calif. Atmospheric Refraction INTRODUCTION it is believed that the treatment presented herein represents a new and interesting ap T IS WELL KNOWN that the geometry of I aerial photographs may be appreciably proach to the problem. distorted by refraction in the atmosphere at THEORETICAL DISCUSSION the time of exposure, and that to obtain maximum mapping accuracy it is necessary The origin of atmospheric refraction can to compensate this distortion as much as be seen by reference to Figure 1. A light ray knowledge permits. This paper presents a L is shown at an angle (J to the vertical in a solution of the refraction problem, including medium in which the velocity of light v varies a hand calculation for the ARDC Model 1 A. H. Faulds and Robert H. Brock, Jr., "Atmo Atmosphere, 1959. The effect of the curva spheric Refraction and its Distortion of Aerial ture of the earth on the refraction problem is Photography," PSOTOGRAMMETRIC ENGINEERING analyzed separately and shown to be negli Vol. XXX, No.2, March 1964. 2 H. H. Schmid, "A General Analytical Solution gible, except for rays approaching the hori to the Problem of Photogrammetry," Ballistic Re zontal. The problem of determining the re search Laboratories Report No. 1065, July 1959 fraction for a practical situation is also dis (ASTIA 230349). cussed. 3 D. C. -
Atmospheric Optics
53 Atmospheric Optics Craig F. Bohren Pennsylvania State University, Department of Meteorology, University Park, Pennsylvania, USA Phone: (814) 466-6264; Fax: (814) 865-3663; e-mail: [email protected] Abstract Colors of the sky and colored displays in the sky are mostly a consequence of selective scattering by molecules or particles, absorption usually being irrelevant. Molecular scattering selective by wavelength – incident sunlight of some wavelengths being scattered more than others – but the same in any direction at all wavelengths gives rise to the blue of the sky and the red of sunsets and sunrises. Scattering by particles selective by direction – different in different directions at a given wavelength – gives rise to rainbows, coronas, iridescent clouds, the glory, sun dogs, halos, and other ice-crystal displays. The size distribution of these particles and their shapes determine what is observed, water droplets and ice crystals, for example, resulting in distinct displays. To understand the variation and color and brightness of the sky as well as the brightness of clouds requires coming to grips with multiple scattering: scatterers in an ensemble are illuminated by incident sunlight and by the scattered light from each other. The optical properties of an ensemble are not necessarily those of its individual members. Mirages are a consequence of the spatial variation of coherent scattering (refraction) by air molecules, whereas the green flash owes its existence to both coherent scattering by molecules and incoherent scattering -
Einstein's Mirage
Paul L. Schechter Einstein’s Mirage he first prediction of Einstein’s general theoryof relativity T to be verified experimentallywas the deflection of light by a massive body—the Sun. In weak gravitational fields (and for such purposes the Sun’s field is considered weak), light behaves as if there were an index of refraction proportional to the gravitational potential. The stronger the gravitational field, the larger the angu- lar deflection of the light. The Sun is not unique in this regard, and it was quickly appreci- ated that stars in our own galaxy (the MilkyWay) and the combined mass of stars in other galaxies would also, on very rare occasions, produce observable deflections. Variations in the “gravitational” index of refraction would also distort images, stretching them in some directions and shrinking them in others. In the analogous case of terrestrial mirages, the deflections and distortions are due to thermal variations in the index of refraction of air. 36 ) schechter mit physics annual 2003 OTH TERRESTRIAL AND GRAVITATIONAL Bmirages sometimes produce multiple distorted images of the same object. When they do, at least one of the images has the opposite handedness of the object being imaged—it is a mirror image, but distorted. At least one of the other images must have the correct handedness, but it will also be distorted. The French call such distorted images gravitational mirages. In the half century following the confirmation of general relativity, the idea that cosmic mirages might actually be observed was taken seriously byonly a small number of astrophysicists. Most of the papers written on the subject treated them as academic curiosities, far too unlikely to actually be observed. -
Evaluating the Effectiveness of Current Atmospheric Refraction Models in Predicting Sunrise and Sunset Times
Michigan Technological University Digital Commons @ Michigan Tech Dissertations, Master's Theses and Master's Reports 2018 Evaluating the Effectiveness of Current Atmospheric Refraction Models in Predicting Sunrise and Sunset Times Teresa Wilson Michigan Technological University, [email protected] Copyright 2018 Teresa Wilson Recommended Citation Wilson, Teresa, "Evaluating the Effectiveness of Current Atmospheric Refraction Models in Predicting Sunrise and Sunset Times", Open Access Dissertation, Michigan Technological University, 2018. https://doi.org/10.37099/mtu.dc.etdr/697 Follow this and additional works at: https://digitalcommons.mtu.edu/etdr Part of the Atmospheric Sciences Commons, Other Astrophysics and Astronomy Commons, and the Other Physics Commons EVALUATING THE EFFECTIVENESS OF CURRENT ATMOSPHERIC REFRACTION MODELS IN PREDICTING SUNRISE AND SUNSET TIMES By Teresa A. Wilson A DISSERTATION Submitted in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY In Physics MICHIGAN TECHNOLOGICAL UNIVERSITY 2018 © 2018 Teresa A. Wilson This dissertation has been approved in partial fulfillment of the requirements for the Degree of DOCTOR OF PHILOSOPHY in Physics. Department of Physics Dissertation Co-advisor: Dr. Robert J. Nemiroff Dissertation Co-advisor: Dr. Jennifer L. Bartlett Committee Member: Dr. Brian E. Fick Committee Member: Dr. James L. Hilton Committee Member: Dr. Claudio Mazzoleni Department Chair: Dr. Ravindra Pandey Dedication To my fellow PhD students and the naive idealism with which we started this adventure. Like Frodo, we will never be the same. Contents List of Figures ................................. xi List of Tables .................................. xvii Acknowledgments ............................... xix List of Abbreviations ............................. xxi Abstract ..................................... xxv 1 Introduction ................................. 1 1.1 Introduction . 1 1.2 Effects of Refraction on Horizon . -
On Some Borrowed and Misunderstood Problems in Greek Catoptrics
On Some Borrowed and Misunderstood Problems in Greek Catoptrics by ALEXANDERJONES Optics was one of the first sciences to which ancient Greek mathe- maticians attempted to apply the apparatus of geometry. They were most successful in describing geometrically certain phenomena of per- spective (as in Euclid’s Optics and parts of Pappus’s Collection, Book 6),less so in catoljtrics, the study of mirrors.’ The problems typically encountered in the surviving writings on catoptrics fall into two classes: those dealing with the reflection of rays cast from a luminous source such as the sun upon minors of plane or curved surface, and those involving the projection of lines of sight from the eye by way of a minor to an object. The most basic problem of the first class, to make a burning mirror, is solved correctly in Diocles’s On Burning Mirrors (ca. 200 B.C.) with both spherical and parabolic mirrors; other prob- lems were investigated by Diocles, by Anthemius (ca. A.D. 620) in his On Paradoxical Devices, and doubtless by other authors in the cen- turies between.2 In general these problems were amenable to geo- metrical treatment in antiquity because Hellenistic geometers were equipped to study the tangent lines to a wide range of curves (or the tangent planes to analogous surfaces) and the behaviour of straight lines in a given direction or through a given point .and inflected at the curve or surface at equal angles to the tangent at the point of in- cidence. Problems of the other class, in which it was required to make an ar- rangement of mirrors or a mirror with a special curvature, such that a *Institute for the History and Philosophy of Science and Technology, Victoria College, Univer- sity of Toronto, Toronto, Canada MSS 1K7. -
Superior Mirage: Aesthetic Recollections of the Great Lakes
Rochester Institute of Technology RIT Scholar Works Theses 12-2014 Superior Mirage: Aesthetic Recollections of the Great Lakes S Caswell Follow this and additional works at: https://scholarworks.rit.edu/theses Recommended Citation Caswell, S, "Superior Mirage: Aesthetic Recollections of the Great Lakes" (2014). Thesis. Rochester Institute of Technology. Accessed from This Thesis is brought to you for free and open access by RIT Scholar Works. It has been accepted for inclusion in Theses by an authorized administrator of RIT Scholar Works. For more information, please contact [email protected]. Superior Mirage {Aesthetic Recollections of the Great Lakes} By S. Caswell December 2014 A Thesis Submitted in Candidacy for the Degree of Master of Fine Arts-Fine Arts Studio School of Art College of Imaging Arts and Sciences Rochester Institute of Technology Rochester, N.Y. Thesis Approval Superior Mirage By S. Caswell Dr. Tom Lightfoot Date Committee Chair Professor Luvon Sheppard Date Committee Member Professor Elizabeth Kronfield Date Committee Member Acknowledgements I would like to thank the committee of Dr. Tom Lightfoot, Prof. Luvon Sheppard, and Prof. Elizabeth Kronfield for their inspiration, guidance and support in the fruition of this thesis work. Each of your guidance has propelled my work to a higher level due to your individual input and depth of knowledge both artistically and intellectually. This is also the place to thank those who mentored me at Roberts Wesleyan College who were monumental in shaping the way I see as an artist. Thank you to Prof. Scot Bennett, Prof. Douglas Giebel, Prof. Jill Kepler, and Prof Alice Drew. -
Analysis of an Infrared Mirage Sequence
Analysis of an infrared mirage sequence Waldemar H. Lehn Infrared observations of seaborne thermal sources are subject to the effects of atmospheric refraction. For low elevation angles at long ranges, out to the limit of visibility, the inevitable atmospheric temper- ature gradients frequently produce mirages. I present an analysis of a 22-min sequence of images recorded on 18 February 1994 at the U.S. Naval Surface Warfare Center at Wallops Island, Virginia. The infrared target is a heat source carried on a ship moving in a straight line toward the camera. The images show a quasi-periodic variation of the horizon elevation, as well as an extended range of visibility. A model that reasonably reproduces the observed features consists of a small temperature inversion in a slightly sloped atmosphere, with an atmospheric gravity wave moving across the line of sight. © 1997 Optical Society of America Key words: Infrared mirage, atmospheric refraction. 1. Introduction ~i! parallel to shore at a nominal bearing angle of 199° All long-range optical observations are affected by toward a fixed station, where the target was a heat refraction in the atmosphere. A well-known exam- source that could be moved up or down a mast ~ele- ple is astronomical refraction that creates a small vations 4.4–26.6 m above mean sea level! and ~ii! apparent vertical displacement of a star or distant directly out to sea at nominal bearing 130°, observing object. Refraction within the surface layer, how- a heat source target on a ship sailing directly toward ever, is not always uniform and on occasion can cause or away from the test site, with two possible target considerable distortion. -
Mirage in Geometrical Optics and the Horizontal Ray
STUDENT JOURNAL OF PHYSICS Mirage in geometrical optics and the horizontal ray Dhiman Biswas1 ,∗ Simran Chourasia2 ,y Rathindra Nath Das1 ,z Rajesh B. Khaparde3 ,x Ajit M. Srivastava4 { 1. B.Sc. final year, Ramakrishna Mission Residential College Narendrapur, Kolkata - 700103 2. M.Sc. 3rd year, National Institute of Science Education and Research, Bhubaneswar 3. Homi Bhabha Centre for Science Education, TIFR, Mankhurd, MUMBAI – 400088 4. Institute of Physics, Bhubaneswar 751005 Abstract. Mirage forms when light rays traversing a medium with spatially varying refractive index bend and undergo total internal reflection. Typical example is when downward going light rays bend upward when heated air in contact with hot earth surface leads to vertical gradient of refractive index with refractive index increasing in upward direction. A conceptual issue arises when considering the part of the light trajectory where light ray becomes horizontal. With refractive index varying only in the vertical direction, one will expect from symmetry considerations that a horizontal ray should not bend, contrary to the observed phenomenon of mirage. This issue has been discussed in literature, e.g. by Raman and Pancharatnam and by Berry. We discuss their arguments and argue that there are subtle conceptual issues in understanding mirage strictly in the framework of geometrical optics. In particular, we consider a horizontally moving light ray and argue that within geometrical optics, such a ray should continue to move horizontally. Bending of such a ray, as required by the mirage phenomenon, must require considerations of wave nature of light. Keywords: Mirage, geometrical optics, wave optics, Fermat’s principle, horizontal ray 1. -
Optics of the Atmosphere and Seeing
Optics of the Atmosphere and Seeing Cristobal Petrovich Department of Astrophysical Sciences Princeton University 03/23/2011 Outline Review general concepts: Airmass Atmospheric refraction Atmospheric dispersion Seeing General idea Theory how does image look like? How it depends on physical sites time Other sources: dome and mirror seeing Summary Airmass Zenith distance z Airmass (X): mass column density to that at the zenith at sea level, i.e., the sea-level airmass at the zenith is 1. X = sec(z) for small z X = sec(z) − 0.001817(sec(z) −1) − 0.002875(sec(z) −1)2 − 0.0008083(sec(z) −1)3 for X > 2 For values of z approaching 90º there are several interpolative formulas: - X is around 40 for z=90º http://en.wikipedia.org/wiki/Airmass Atmospheric refraction Direction of light changes as it passes through the atmosphere. Start from Snell´s law µ1 sin(θ1) = µ2 sin(θ2 ) Top of the atmosphere Define sin(z ) µ 0 = N z0 : true zenith distance sin(zN ) 1 z : observed zenith distance Induction using infinitesimal layers zn : observed zenith distance at layer n sin(z ) µ sin(z ) µ n = n −1 , n −1 = n −2 sin(zn −1) µn sin(zn −2 ) µn sin(z ) µ ⇒ n = n −2 and so on... to get sin(zn −2) µn sin(z0) = µ sin(z) Refraction depends only on refraction index near earth´s surface Atmospheric refraction We define the astronomical refraction r as the angular displacement: sin(z + r) = µ sin(z) In most cases r is small sin(z) + rcos(z) = µ sin(z) ⇒ r = (µ −1)tan(z) ≡ Rtan(z) For red light R is around 1 arc minute Atmospheric dispersion Since R depends on frequency: atmospheric Lambda R dispersion (A) (arcsec) 3000 63.4 Location of an object depends of wavelength: 4000 61.4 implications for multiobjects spectrographs , where 5000 60.6 slits are placed on objects to accuracy of an 6000 60.2 arcsecond 7000 59.9 10000 59.6 40000 59.3 An image of Venus, showing chromatic dispersion. -
Some Readings in the Early History of Light
Paul Avery PHY 3400 Aug. 23, 1999 Some Readings in the Early History of Light The Greeks In optics, Euclid's textbook (called the Optics) set the precedent. Euclid postulated visual rays to be straight lines, and he defined the apparent size of an object in terms of the angle formed by the rays drawn from the top and the bottom of the object to the observer's eye. He then proved, for example, that nearer objects appear larger and appear to move faster and showed how to measure the height of distant objects from their shadows or reflected images, and so on. Other textbooks set out theorems on the phenomena of reflection and refraction (the field called catoptrics). The most extensive survey of optical phenomena is a treatise attributed to the astronomer Ptolemy (2nd century AD), which survives only in the form of an incomplete Latin translation (12th century) based on a lost Arabic translation. It covers the fields of geometric optics and catoptrics, as well as experimental areas, such as binocular vision, and more general philosophical principles (the nature of light, vision, and colour). Of a somewhat different sort are the studies of burning mirrors by Diocles (late 2nd century BC), who proved that the surface that reflects the rays from the Sun to a single point is a paraboloid of revolution. Constructions of such devices remained of interest as late as the 6th century AD, when Anthemius of Tralles, best known for his work as architect of the Hagia Sophia at Constantinople, compiled a survey of remarkable mirror configurations. -
Optics History As Effective Instrument for Education in Optics and Photonics
ETOP 2009 1 Optics history as effective instrument for education in optics and photonics S.K. Stafeef and M.G. Tomilin St.-Petersburg University of Information Technologies, Mechanics and Optics, St.- Petersburg, 197101, Kronverksky Pr. 49, Russia ABSTRACT The education problem in optics and photonics is to draw young generation on the side of light, optical science and technology. The main goal is to prove the slogan that “physics is a small part of optics”: during the thousand years optics formulated the clear worldview for humanity. In fact optics is itself presents multidisciplinary collection of independent scientific arias from one hand and was a generator of new fields of knowledge from the other hand. Optics and photonics are the regions where the fundamental problems of our reality have to be solved. The mentioned functions belonged to optics during the period of civilizations development. This is a basic idea of books serial by S. Stafeev and M. Tomilin “Five Millennium of Optics” including 3 volumes. The first volume devoted to optics prehistory was edit in 2006 in Russian. Its main chapters devoted to relations between Sun and Life, the beginnings of human intelligence, megalithic viewfinders, gnomons and ancient temples orientation, archaic optical materials and elements. It also consist the optical riddles of that period. The volume II is devoted to Greek and Roman antiquity and is in the process of publishing. It consist the chapters on the beginning of optics, mathematical fundaments and applied optics evolution. Volume III would be devoted to Medieval and Renaissance optics history. The materials are used at our university in a course “The Modern Natural Science Conceptions” for students and graduate students. -
Bibliography
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