Simulation of Atmospheric Phenomena

Total Page:16

File Type:pdf, Size:1020Kb

Simulation of Atmospheric Phenomena This article was originally published in a journal published by Elsevier, and the attached copy is provided by Elsevier for the author’s benefit and for the benefit of the author’s institution, for non-commercial research and educational use including without limitation use in instruction at your institution, sending it to specific colleagues that you know, and providing a copy to your institution’s administrator. All other uses, reproduction and distribution, including without limitation commercial reprints, selling or licensing copies or access, or posting on open internet sites, your personal or institution’s website or repository, are prohibited. For exceptions, permission may be sought for such use through Elsevier’s permissions site at: http://www.elsevier.com/locate/permissionusematerial ARTICLE IN PRESS Computers & Graphics 30 (2006) 994–1010 www.elsevier.com/locate/cag Technical Section Simulation of atmospheric phenomena Diego GutierrezÃ, Francisco J. Seron , Adolfo Munoz , Oscar Anson Department of Computer Science and Systems Engineering, University of Zaragoza, C/Maria de Luna 1, 50018 Zaragoza, Spain Received 19 January 2006; accepted 12 May 2006 Abstract This paper presents a physically based simulation of atmospheric phenomena. It takes into account the physics of non-homogeneous media in which the index of refraction varies continuously, creating curved light paths. As opposed to previous research on this area, we solve the physically based differential equation that describes the trajectory of light. We develop an accurate expression of the index of refraction in the atmosphere as a function of wavelength, based on real measured data. We also describe our atmosphere profile manager, which lets us mimic the initial conditions of real-world scenes for our simulations. The method is validated both visually (by comparing the images with the real pictures) and numerically (with the extensive literature from other areas of research such as optics or meteorology). The phenomena simulated include the inferior and superior mirages, the Fata Morgana, the Novaya–Zemlya, the Viking’s end of the world, the distortions caused by heat waves and the green flash. r 2006 Elsevier Ltd. All rights reserved. Keywords: Atmospheric phenomena; Nonlinear ray tracing; Inhomogeneous media 1. Introduction apply it here to simulate six different effects: the inferior and superior mirages, the Fata Morgana, the Novaya- Simulating natural phenomena has always been one of the Zemlya, the Viking’s end of the world and the green flash, most challenging goals of computer graphics. In particular, and propose several others, such as the distortions caused the effect of the atmosphere on sunlight, under certain by heat waves or fire. circumstances, causes a number of really spectacular phenomena; some are well-known, like the mirages, whereas 1.1. Overview some of them remain mostly unknown, such as the Fata Morgana or the Novaya-Zemlya. As far as the authors The atmosphere is a non-homogeneous medium, with its know some of the atmospheric phenomena presented in this properties varying continuously from point to point. The paper have never been simulated before, including the last most important property in terms of defining the light two mentioned above. This is due to the difficulty of first paths is the index of refraction, which in turn depends reproducing the exact, specific atmospheric conditions strongly on temperature, density and wavelength (and required to reproduce the effect and second, accurately more subtly on other parameters such as humidity). The calculating the nonlinear trajectories of light as it travels continuous variation of the light paths induced by the non- through the atmosphere under such conditions. homogeneous index of refraction can be described by a We present here our ray tracing method to reproduce differential equation, as will be shown in Section 3. some of these spectacular phenomena. The method is Our simulation is based on three main points: general and therefore can be applied to the simulation of any effect caused by nonlinear trajectories of light. We Fermat’s principle, which yields the physically based description of the light path through a non-homoge- ÃCorresponding author. Tel.: +34 976 762 354; fax: +34 976 761 914. E-mail addresses: [email protected] (D. Gutierrez), [email protected] neous medium (with a continuously varying index of (F.J. Seron), [email protected] (A. Munoz), [email protected] refraction), coupled with a fast, efficient numerical (O. Anson). resolution method. 0097-8493/$ - see front matter r 2006 Elsevier Ltd. All rights reserved. doi:10.1016/j.cag.2006.05.002 ARTICLE IN PRESS D. Gutierrez et al. / Computers & Graphics 30 (2006) 994–1010 995 An accurate model of the atmosphere, which includes sphere as seen from the space [4]. These works are based on temperature and pressure at every point, as well as the simplified models of the physics of the atmosphere, since equations that yield the index of refraction at every they are mainly focused on performance rather than differential point at every wavelength, needed for the realism. Related to them we can find others which rely correct application of Fermat’s principle. more on the physics of the atmosphere and therefore the Our Atmospheric Profile Manager (APM), a tool to color of the sky is more realistic and physically more recreate the necessary atmospheric conditions, based on accurate. For instance Irwin [5] takes into account functions whose predicted values match actual measured Rayleigh scattering (due to the air molecules), and Jacke` l data. and Walter [6] consider Mie scattering (due to the aerosols of the atmosphere). Mie scattering enables also cloud, rain All the simulations presented in this paper are physically and even rainbow simulations. In [7], by Riley et al., both based. The equations are justified either by comparing the Rayleigh and Mie scattering are considered, although results with measured data or by citing previous works many simplifications (like single scattering) are made in which have validated them. These references are mostly order to accelerate the render times by GPU. Dobashi et al. taken from other research areas such as optics or [8] also follow a similar approach. A very interesting survey meteorology, as it is our conviction that accurate simula- about all the possible scattering related phenomena in the tions of natural phenomena do require a multidisciplinary atmosphere is the work of Sloup [9], which presents approach. Finally, although for this paper we focus on the different approaches and different models and phase Earth’s atmosphere, our model is completely general and functions for aerosols, ozone and clear air, and therefore obviously valid for any medium. sets the basis for the simulation of phenomena like clouds, The rest of the work is organized as follows: the next halos or rainbows. section describes the previous work and helps contextualize this research. Section 3 presents our simulation method, including a brief description of the physical laws involved, 2.2. Refraction related the model of the atmosphere, the equation describing the path of light and the resolution method. Section 5 validates The first work considering the atmosphere as an the method, with rendered scenes shown in Section 4. inhomogeneous medium, in which the index of refraction Finally, Sections 6 and 7 discuss the conclusions and the varies at different heights, was developed by Berger et al. future work. [10]. As a consequence, the light path is modified not only by the interaction with different objects, but by the own 2. Previous work atmosphere as well. This way some effects like superior and inferior mirages can be simulated. Their model is based on Modeling nature has always been one of the most a set of layers of the atmosphere at different heights with ambitious goals of computer graphics. There are many different indexes of refraction, and while tracing a light ray phenomena that are caused by the varying non-homo- its path is refracted at the boundaries between two layers geneous properties of the atmosphere, and consequently applying Snell’s Law. On the other hand, Musgrave [11] there has been a lot of work aimed at simulating them. rejects the previous model based on refraction and These papers can be classified into two main categories: proposes a new one, based on total reflection. This model Absorption and scattering related: These aim to obtain is also able to simulate some mirages, although it is rather the color resulting from the interaction of light and the incomplete. atmosphere. They consider that the atmosphere is a The model for simulating the atmosphere by Lehn [12] is participating medium and therefore absorption and scat- more complete. It is similar to the proposed in [10] but tering events occur while light traverses it. Phenomena like instead of pure refractions it considers parabolic paths of clouds and rainbows are simulated this way. light inside the different layers, considering a set of per- Refraction related: These focus on the obtention of the layer individual properties. Lint¸u et al. [13] follow the work true shape of what is seen. They consider that the in [12], including also wavelength dependance, and conse- atmosphere is a non-homogeneous media, and therefore quently it is capable to simulate dispersion-based atmo- light does not follow straight paths while traversing it. spheric phenomena, like the green flash. However, all these Phenomena like mirages and sunset effects can be layer-based works are limited to one dimension variations simulated this way. This paper greatly contributes to this of the index of refraction and are not capable of simulating category. other atmospheric effects like the distortion caused by fire. A more general method is presented by Seron et al. [14]. 2.1. Absorption and scattering related It computes the path of light by calculating Fermat’s principle using Euler’s Method.
Recommended publications
  • Atmospheric Optics - II First Midterm Exam Is This Friday!
    Atmospheric Optics - II First midterm exam is this Friday! The exam will be in-class, during our regular lecture • this Friday September 28 at 9:30 am The exam will be CLOSED BOOK • ♦ No textbooks ♦ No calculators ♦ No cheat-sheets Alternate seating • The grades will be posted on WebCT • The exam covers Chapters 1,2,3,4,5, and 19. • The sections which are not covered are listed on the • Class Notes web page. RECAP • Human perception of color, white objects, black objects. Light scattering: light is sent in all directions –forward, sideways and • backward ♦ Geometric scattering: R>>λ (all wavelengths equally scattered) ♦ Mie scattering: R~λ (red is scattered more efficiently) ♦ Rayleigh scattering: R<<λ (blue is scattered more efficiently) Phenomena: white clouds, blue skies, hazy skies, crepuscular rays, colorful • sunsets, blue moon. TODAY: Refraction: the bending of the light ray as it travels from one medium to • another. It bends towards the vertical if it enters a more-dense medium and away from the vertical as it enters a less-dense medium. ♦ Phenomena: stars appear higher in the sky, twinkling, twilight. • Reflection: the angle of incidence is equal to the angle of reflection • Total internal reflection: mirages Dispersion: separation of colors when light travels through a medium. • ♦ rainbow Reflection and Refraction of Light The speed of light in vacuum • is c=300,000 km/s Snell’s law: The angle of • incidence is equal to the angle of reflection. Light that enters a more- • dense medium slows down and bends toward the normal. Light that exits a more- • dense medium speeds up and bends away from the normal.
    [Show full text]
  • Light Color and Atmospheric Light, Color, and Atmospheric Optics
    Light, Color, and Atmospheric Optics Chapter 19 April 28 and 30, 2009 Colors • Sunlight contains all colors (visible spectrum) Wavelength Ranges in µm UV-C: 0.25 - 0.29 UV-B: 0.29 - 0.32 UV-A: 0.32 - 0.38 Visible: 0.38 - 0.75 Near IR: 0.75 - 4 Mid IR: 4 - 8 Longwave IR: 8 - 100 Colors • If object is white then all colors are reflected • If object is red then only red is reflected and all others are absorbed From Malm (1999). Introduction to Visibility Blue Skies and Hazy days • Selective scattering – Scattering depends on wavelength of light • Rayleigh scattering – Very small particles, gases • Mie scattering – Particles the size of wavelength of visible light • Blue haze • Some particles from plants: terpenes, α- pinene Blue Ridge Mountains • Blue haze caused by scattering of blue light by fine particles Creppyuscular Rays • Scattering of sunlight by dust and haze produces white bands Selective Scattering: Sunset • Notice the effects of scattering on color as sunlight penetrates into the atmosphere Twinkling, Twilight, and the Green Flash • Light that travels from a less dense to a more dense medium loses speed and bends toward the normal, while light that enters a less dense medium increase speed and bends away from the normal. • Apparent position, scintillation, and green flash all depend of density variations in the athtmosphere • Scintillation also indicates the amount of turbulence in the atmosphere Bending of Light Paths from Atmosphere Green Flash • Green flash at top may be seen under circumstances of very cold (dense) air near the surface rapidly changing to warmer (less dense) air aloft Mirages •Miraggyges are caused by refraction of light due to strong density differences in atmospheric layers usually caused by strong temperature differences.
    [Show full text]
  • Why Doesn't the Sky Turn Green?
    Why Doesn't The Sky Turn Green? Rushi Shah 09 November 2015 I was leafing through the US Army Corps of Engineers' Manual on Remote Sensing and learned about how Rayleigh scattering creates blue skies during the day and redish-orange sunsets. Well, everybody knows about blue skies and red sunsets, was the title just click-bait, you ask? No, but I'll get to that. 1 The Basics of Rayleigh Scattering Let's start with this whole Rayleigh scattering thing. Basically the idea is that particles in the atmosphere (like Oxygen and Nitrogen particles) scatter rays of light as they enter the atmosphere. How much the light is scattered is heavily dependent on the wavelength of the light. Remember how ROY-G-BIV represents the colors of the rainbow (and thus the spectrum of visible light)? Well that spectrum of light starts with long wavelength rays (reds, oranges, and yellows) and ends with short wavelength rays (blues, indigos, and violets). 1 The amount of light that is scattered (denoted with the variable I) is highly inversely proportional to the wavelength of the light (denoted with the greek letter ). Put simply, as the wavelength goes down, the light waves are scattered more quickly. 1 I / λ4 When sunlight hits the earth directly during mid-day, it travels through a small amount of atmosphere, and thus we see the wavelengths of light that are immediately scattered. Based on the equation above, the blues, indigos, and violets would be scattered first (and they blend together into the blue sky we see). As the sun sets, it goes through more and more particles to reach us.
    [Show full text]
  • ESSENTIALS of METEOROLOGY (7Th Ed.) GLOSSARY
    ESSENTIALS OF METEOROLOGY (7th ed.) GLOSSARY Chapter 1 Aerosols Tiny suspended solid particles (dust, smoke, etc.) or liquid droplets that enter the atmosphere from either natural or human (anthropogenic) sources, such as the burning of fossil fuels. Sulfur-containing fossil fuels, such as coal, produce sulfate aerosols. Air density The ratio of the mass of a substance to the volume occupied by it. Air density is usually expressed as g/cm3 or kg/m3. Also See Density. Air pressure The pressure exerted by the mass of air above a given point, usually expressed in millibars (mb), inches of (atmospheric mercury (Hg) or in hectopascals (hPa). pressure) Atmosphere The envelope of gases that surround a planet and are held to it by the planet's gravitational attraction. The earth's atmosphere is mainly nitrogen and oxygen. Carbon dioxide (CO2) A colorless, odorless gas whose concentration is about 0.039 percent (390 ppm) in a volume of air near sea level. It is a selective absorber of infrared radiation and, consequently, it is important in the earth's atmospheric greenhouse effect. Solid CO2 is called dry ice. Climate The accumulation of daily and seasonal weather events over a long period of time. Front The transition zone between two distinct air masses. Hurricane A tropical cyclone having winds in excess of 64 knots (74 mi/hr). Ionosphere An electrified region of the upper atmosphere where fairly large concentrations of ions and free electrons exist. Lapse rate The rate at which an atmospheric variable (usually temperature) decreases with height. (See Environmental lapse rate.) Mesosphere The atmospheric layer between the stratosphere and the thermosphere.
    [Show full text]
  • Mystic Mountain © Mendip Hills AONB
    Viewpoint Mystic mountain © Mendip Hills AONB Time: 15 mins Region: South West England Landscape: rural Location: Ebbor Gorge, Somerset, BA5 3BA Grid reference: ST 52649 48742 Getting there: Park at Deer Leap car park and picnic area (on the road between Wookey Hole and Priddy) Keep an eye out for: Buzzards and other birds of prey soaring on the thermals below From this stunning vantage point we have sweeping views south across the flat land of the Somerset Levels. On a clear day, looking east you can see the dark line of hills marking out Exmoor National Park and if you look in a west south-west direction you can even spot the Bristol Channel glistening in the distance. As our eyes pan across the view they rest on a perfectly rounded knoll with a short tower on top. This is Glastonbury Tor. Claimed as the site of the legendary Vale of Avalon and the final resting place of King Arthur, the tor rises up above the flat land surrounding it and is visible for miles around. Why does the mystical Glastonbury Tor rise up out of the surrounding lowlands? First of all look straight ahead and in the middle distance you’ll see three hills which punctuate the flat landscape. From left to right they are Hay Hill, Ben Knowle Hill and Yarley Hill, part of a low ridge just south of the River Axe. Surrounding these hills the Somerset Levels are an area of low-lying farmland. The lowest point is just 0.2 metres above sea level.
    [Show full text]
  • The Min Min Light and the Fata Morgana Pettigrew
    C L I N I C A L A N D E X P E R I M E N T A L OPTOMETRYThe Min Min light and the Fata Morgana Pettigrew COMMENTARY The Min Min light and the Fata Morgana An optical account of a mysterious Australian phenomenon Clin Exp Optom 2003; 86: 2: 109–120 John D Pettigrew BSc(Med) MSc MBBS Background: Despite intense interest in this mysterious Australian phenomenon, the FRS Min Min light has never been explained in a satisfactory way. Vision Touch and Hearing Research Methods and Results: An optical explanation of the Min Min light phenomenon is of- Centre, University of Queensland fered, based on a number of direct observations of the phenomenon, as well as a field demonstration, in the Channel Country of Western Queensland. This explanation is based on the inverted mirage or Fata Morgana, where light is refracted long distances over the horizon by the refractive index gradient that occurs in the layers of air during a temperature inversion. Both natural and man-made light sources can be involved, with the isolated light source making it difficult to recognise the features of the Fata Morgana that are obvious in daylight and with its unsuspected great distance contribut- ing to the mystery of its origins. Submitted: 11 September 2002 Conclusion: Many of the strange properties of the Min Min light are explicable in terms Revised: 2 December 2002 of the unusual optical conditions of the Fata Morgana, if account is also taken of the Accepted for publication: 3 December human factors that operate under these highly-reduced stimulus conditions involving a 2002 single isolated light source without reference landmarks.
    [Show full text]
  • 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
    [Show full text]
  • 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.
    [Show full text]
  • The Antarctic Sun, December 17, 2006
    December 17, 2006 New fi nds in Dry Valleys indicate ancient tundra By Peter Rejcek Sun staff Flannel shirts and jeans – or perhaps a light fleece – may have been the norm in the McMurdo Dry Valleys of Antarctica about 14 mil- lion years ago. Fossil records and glacial history in an area of the western Olympus Range near Mount Boreas indi- cate that during the middle of the Miocene epoch (about 14 million years ago) climatic conditions were warm and wet enough to support plant and insect life, according to a team of scientists that returned this season to continue its research. The story began when Adam Lewis, a post-doctoral fellow at The Antarctic The Sun Byrd Polar Research Center at The Ohio State University, traversed a roughly 100-square-kilometer Allan Ashworth picks through a pile of area of the Olympus Range sev- Peter Rejcek / eral years ago while working on shale looking for fossils and other his doctorate. His thesis involved fleshing out the glacial history evidence of a tundra environment that he and of eight valleys between various mountain peaks. others believe disappeared in the McMurdo Dry “In the process of doing that, I discovered these lake deposits,” Valleys about 14 million years ago. explained Lewis shortly before he headed into the field via helicop- See related story on page 8 See CLIMATE on page 9 Blowin’ in the Wind Quote of the Week USAP looks to harness alternative energy for McMurdo, South Pole “So, are you originally from By Steve Martaindale Programs for the National Science Foundation.
    [Show full text]
  • The Fata Morgana. by Professor FA Forel, Morges
    1911-12.] The Fata Morgana. 175 XV.—The Fata Morgana. By Professor F. A. Forel, Morges, Switzerland. Abstract of an Address delivered before the Society on July II,., 1911; translated by Professor C. G. Knott. AMONG optical phenomena which originate over the surface of water there is one so ill-defined and ill-observed as to be still mysterious; till now it has received no valid explanation. The Italians call it the Fata Morgana. Under conditions still lacking precise description, there appear on the far side of the Straits of Messina certain fantastic visions, fortresses and castles of unknown cities, which seem to emerge from the sea, soon to vanish again. These are the "palaces" of the "fairy Morgana," which appear and dis- appear at the capricious stroke of the magician's wand. Most of the accounts of the phenomenon are founded on the extravagant description and the amazing picture published in 1773 by the Dominican friar Don Antonio Minasi, professor of botany at the Roman College of Sapienzia. This drawing, with its incoherent groupings of castles and boats, reflected and refracted at random in a manner quite inconsistent with physical possibilities, was largely the creation of the distorted imagination of an artist who did not understand in the least the wonderful illusion. To appreciate the confusion which reigns in the scientific world in regard to this phenomenon, the reader need only refer to the chapter on the Fata Morgana in Pernter's admirable work on Meteorological Optics (Vienna, 1910). There he will be impressed with the uncertainty of the conclusions reached by the author after a study of the insufficient and contradictory documents to which he had access.
    [Show full text]
  • How to Format a SCCG Papaer
    Chasing the Green Flash: a Global Illumination Solution for Inhomogeneous Media D. Gutierrez F.J. Seron O. Anson A. Muñoz University of Zaragoza University of Zaragoza University of Zaragoza University of Zaragoza [email protected] [email protected] [email protected] [email protected] restrictions on the scenes and effects that can be Abstract reproduced, including some of the phenomena that occur in our atmosphere. Several natural phenomena, such as mirages or the Most of the media are in fact inhomogeneous to one green flash, are owed to inhomogeneous media in degree or another, with properties varying continuously which the index of refraction is not constant. This from point to point. The atmosphere, for instance, is in makes the light rays travel a curved path while going fact inhomogeneous since pressure, temperature and through those media. One way to simulate global other properties do vary from point to point, and illumination in inhomogeneous media is to use a therefore its optic characterization, given by the index curved ray tracing algorithm, but this approach of refraction, is not constant. presents some problems that still need to be solved. A light ray propagating in a straight line would then be This paper introduces a full solution to the global accurate only in two situations: either there is no media illumination problem, based on what we have called through which the light travels (as in outer space, for curved photon mapping, that can be used to simulate instance), or the media are homogeneous. But with several natural atmospheric phenomena. We also inhomogeneous media, new phenomena occur.
    [Show full text]
  • 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 .
    [Show full text]