Atmospheric Optics
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Atmospheric Phenomena by Feist
Atmospheric optical phenomena An introductory guide by Mike Feist Effects caused by water droplets— rainbows and coronae The most well known optical sky effect is the rainbow. This, as most people know, sometimes occurs when the Sun is out and it is raining. To see a rainbow you must stand with your back to the Sun with the raindrops in front of you. It does not have to be raining where you are standing but in the direction that you are looking. The arc of the primary (main) bow is centred on the antisolar point, the spot directly oppo- site the Sun, and has a radius of 42°. The antisolar point is actually centred on the shadow of your head. If the Sun is rising or setting and therefore on the horizon, the primary rainbow will be a complete semi- circle and the top will be 42° up in the sky. If, on the other hand, the Sun is 42° up in the sky, the primary bow will be on the horizon, the top just rising or setting. Con- ventionally the rainbow is said to have John Constable. Hampstead Heath with a Rainbow (1836). seven colours but all we need to remember seen in the spray near waterfalls and artifi- ous forms but with a six-sided shape. They is that, in the primary bow, the red is on cial rainbows can be made using a garden may be as flat hexagonal plates or long the outside and the blue on the inside. Out- hose. Rainbows are one of the easiest opti- hexagonal prisms or as a combination of side the primary bow sometimes there is cal effects to photograph although they the two. -
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 . -
References: Snel's Law and Refraction Index of Refraction For
ESCI 340 - Cloud Physics and Precipitation Processes Lesson 13 - Atmospheric Optical Phenomena Dr. DeCaria References: One of the best sources for information about atmospheric optics is the Atmospheric Optics website, http://www.atoptics.co.uk Snel's Law and Refraction • The index of refraction for a medium is defined as m = c=c;~ (1) where c is the speed of light in a vacuum, andc ~ is the speed of light in the medium.1 • As light passes from one medium into another, there is both reflection and refraction. • Refraction occurs because the wave fronts bend as they cross from one medium into another, causing a ray of light to bend. The ray bends toward the medium that has the slower speed of light (highest index of refraction). • The bending of the ray is quantified by Snel's Law, which is stated mathematically as sin θ m 1 = 2 ; (2) sin θ2 m1 where θ1 is the angle of incidence (and reflection), θ2 is the angle of refraction, and m1 and m2 are the indices of refraction in the two mediums (see Fig. 1). • The amount by which a ray of light is deflected due to refraction can be quantified in one of two ways. { The bending angle, θ0, is the interior angle between the initial and final rays. { The deviation angle, θ00, is the complement of the bending angle, θ00 = 180◦ −θ0. { The relationship between bending angle and deviation angle is illustrated in Fig. 2. Index of Refraction for Air • Light travels faster through warm air than it does through cold air. -
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. -
Residents Complete Emergency Response
The Westfield NewsSearch for The Westfield News Westfield350.com The WestfieldNews Serving Westfield, Southwick, and surrounding Hilltowns “TIME IS THE ONLY WEATHER CRITIC WITHOUT TONIGHT AMBITION.” Partly Cloudy. JOHN STEINBECK Low of 55. www.thewestfieldnews.com VOL. 86 NO. 151 $1.00 TUESDAY,TUESDAY, APRIL JUNE 27, 20, 2017 2021 VOL.75 cents 90 NO. 92 Westfield High School offers credit recovery opportunity this week By AMY PORTER Staff Writer WESTFIELD – Westfield High School Principal Charles Jendrysik said the school will be offering students who failed certain required courses the first semester an opportunity to make up the credits during April vacation week. The program, a first for the high school, will be targeting a number Graduation was held Saturday for new members of the Westfield Community Emergency Response Team (CERT). Front of one-semester courses, includ- row: Matt Warren, Al Giguere, Jr., Kathy Dubuque, Jason Polan, and Charlie Smith; back row: Kathy Hillman, Shannon ing several English language arts Chiba, Assistant Director Melissa Blain, Director Steve Malochleb, Jain Makepeace, and Alfiya K. (MARC ST.ONGE/THE courses, physical education and WESTFIELD NEWS) financial literacy. “A lot of them are school requirements. We wanted to help students with the courses we knew they needed to pass in order to CERT: Residents complete graduate,” Jendrysik said. The school will run full days Tuesday to Saturday, due to the Patriot’s Day Monday holiday. emergency response training Jendrysik said he was encour- CHARLES aged by having over 50 students JENDRYSIK By HOPE E. TREMBLAY “My hope is to have at least 50 mem- Psychology 101 to not only deal with the sign up for the week. -
Atmospheric Refraction: a History
Atmospheric refraction: a history Waldemar H. Lehn and Siebren van der Werf We trace the history of atmospheric refraction from the ancient Greeks up to the time of Kepler. The concept that the atmosphere could refract light entered Western science in the second century B.C. Ptolemy, 300 years later, produced the first clearly defined atmospheric model, containing air of uniform density up to a sharp upper transition to the ether, at which the refraction occurred. Alhazen and Witelo transmitted his knowledge to medieval Europe. The first accurate measurements were made by Tycho Brahe in the 16th century. Finally, Kepler, who was aware of unusually strong refractions, used the Ptolemaic model to explain the first documented and recognized mirage (the Novaya Zemlya effect). © 2005 Optical Society of America OCIS codes: 000.2850, 010.4030. 1. Introduction the term catoptrics became reserved for reflection Atmospheric refraction, which is responsible for both only, and the term dioptrics was adopted to describe astronomical refraction and mirages, is a subject that the study of refraction.2 The latter name was still in is widely dispersed through the literature, with very use in Kepler’s time. few works dedicated entirely to its exposition. The same must be said for the history of refraction. Ele- ments of the history are scattered throughout numer- 2. Early Greek Theories ous references, many of which are obscure and not Aristotle (384–322 BC) was one of the first philoso- readily available. It is our objective to summarize in phers to write about vision. He considered that a one place the development of the concept of atmo- transparent medium such as air or water was essen- spheric refraction from Greek antiquity to the time of tial to transmit information to the eye, and that vi- Kepler, and its use to explain the first widely known sion in a vacuum would be impossible. -
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Chaotic Modeling and Simulation (CMSIM) 2: 159-171, 2018 Chaotic dynamics of ice crystals scattering sun light 1 2 1 Alberto Tufaile , Timm A. Vanderelli , and Adriana P. B. Tufaile 1 Soft Matter Lab, Escola de Artes, Ciências e Humanidades, Universidade de São Paulo, São Paulo, Brazil (E-mail: [email protected]) 2 Ferrocell USA, 739 Route 259, Ligonier, Pennsylvania, 15658, USA (E-mail: [email protected]) 1 Soft Matter Lab, Escola de Artes, Ciências e Humanidades, Universidade de São Paulo, São Paulo, Brazil (E-mail: [email protected]) Abstract. We are reporting the existence of the nonlinear dynamics in some curious phenomena observed in the context of atmospheric optics: jumping sundogs, halo formation and the miracle of the Sun. A possible connection between these atmospheric patterns of the atmospheric optics and light scattering in particles with the same size of the ice crystals could be based in the concept of diffracted rays. Keywords: Chaotic Modelling, Jumping Sundogs, Ferrofluids, Parlaseric circle. 1 Introduction There are some interesting phenomena involving atmospheric optics, for example, the jumping sundog is an amazing band of light continuously oscillating over the sky [1], sweeping downward and jumping up again, as it is shown in Fig. 1. Besides this phenomenon, Wirowski [2, 3] studied the bizarre effect known as “the miracle of the Sun”, in which many people observed oscillations in the size of the Sun, as it is shown in Fig. 2, and suggested the dynamical system describing this effect. These phenomena lasted a few minutes and some of them were recorded by some amateur observers.