The Ray Optics Module User's Guide
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Contents 1 Properties of Optical Systems
Contents 1 Properties of Optical Systems ............................................................................................................... 7 1.1 Optical Properties of a Single Spherical Surface ........................................................................... 7 1.1.1 Planar Refractive Surfaces .................................................................................................... 7 1.1.2 Spherical Refractive Surfaces ................................................................................................ 7 1.1.3 Reflective Surfaces .............................................................................................................. 10 1.1.4 Gaussian Imaging Equation ................................................................................................. 11 1.1.5 Newtonian Imaging Equation.............................................................................................. 13 1.1.6 The Thin Lens ...................................................................................................................... 13 1.2 Aperture and Field Stops ............................................................................................................ 14 1.2.1 Aperture Stop Definition ..................................................................................................... 14 1.2.2 Marginal and Chief Rays ...................................................................................................... 14 1.2.3 Vignetting ........................................................................................................................... -
Descartes' Optics
Descartes’ Optics Jeffrey K. McDonough Descartes’ work on optics spanned his entire career and represents a fascinating area of inquiry. His interest in the study of light is already on display in an intriguing study of refraction from his early notebook, known as the Cogitationes privatae, dating from 1619 to 1621 (AT X 242-3). Optics figures centrally in Descartes’ The World, or Treatise on Light, written between 1629 and 1633, as well as, of course, in his Dioptrics published in 1637. It also, however, plays important roles in the three essays published together with the Dioptrics, namely, the Discourse on Method, the Geometry, and the Meteorology, and many of Descartes’ conclusions concerning light from these earlier works persist with little substantive modification into the Principles of Philosophy published in 1644. In what follows, we will look in a brief and general way at Descartes’ understanding of light, his derivations of the two central laws of geometrical optics, and a sampling of the optical phenomena he sought to explain. We will conclude by noting a few of the many ways in which Descartes’ efforts in optics prompted – both through agreement and dissent – further developments in the history of optics. Descartes was a famously systematic philosopher and his thinking about optics is deeply enmeshed with his more general mechanistic physics and cosmology. In the sixth chapter of The Treatise on Light, he asks his readers to imagine a new world “very easy to know, but nevertheless similar to ours” consisting of an indefinite space filled everywhere with “real, perfectly solid” matter, divisible “into as many parts and shapes as we can imagine” (AT XI ix; G 21, fn 40) (AT XI 33-34; G 22-23). -
Chapter 19/ Optical Properties
Chapter 19 /Optical Properties The four notched and transpar- ent rods shown in this photograph demonstrate the phenomenon of photoelasticity. When elastically deformed, the optical properties (e.g., index of refraction) of a photoelastic specimen become anisotropic. Using a special optical system and polarized light, the stress distribution within the speci- men may be deduced from inter- ference fringes that are produced. These fringes within the four photoelastic specimens shown in the photograph indicate how the stress concentration and distribu- tion change with notch geometry for an axial tensile stress. (Photo- graph courtesy of Measurements Group, Inc., Raleigh, North Carolina.) Why Study the Optical Properties of Materials? When materials are exposed to electromagnetic radia- materials, we note that the performance of optical tion, it is sometimes important to be able to predict fibers is increased by introducing a gradual variation and alter their responses. This is possible when we are of the index of refraction (i.e., a graded index) at the familiar with their optical properties, and understand outer surface of the fiber. This is accomplished by the mechanisms responsible for their optical behaviors. the addition of specific impurities in controlled For example, in Section 19.14 on optical fiber concentrations. 766 Learning Objectives After careful study of this chapter you should be able to do the following: 1. Compute the energy of a photon given its fre- 5. Describe the mechanism of photon absorption quency and the value of Planck’s constant. for (a) high-purity insulators and semiconduc- 2. Briefly describe electronic polarization that re- tors, and (b) insulators and semiconductors that sults from electromagnetic radiation-atomic in- contain electrically active defects. -
Nikon Binocular Handbook
THE COMPLETE BINOCULAR HANDBOOK While Nikon engineers of semiconductor-manufactur- FINDING THE ing equipment employ our optics to create the world’s CONTENTS PERFECT BINOCULAR most precise instrumentation. For Nikon, delivering a peerless vision is second nature, strengthened over 4 BINOCULAR OPTICS 101 ZOOM BINOCULARS the decades through constant application. At Nikon WHAT “WATERPROOF” REALLY MEANS FOR YOUR NEEDS 5 THE RELATIONSHIP BETWEEN POWER, Sport Optics, our mission is not just to meet your THE DESIGN EYE RELIEF, AND FIELD OF VIEW The old adage “the better you understand some- PORRO PRISM BINOCULARS demands, but to exceed your expectations. ROOF PRISM BINOCULARS thing—the more you’ll appreciate it” is especially true 12-14 WHERE QUALITY AND with optics. Nikon’s goal in producing this guide is to 6-11 THE NUMBERS COUNT QUANTITY COUNT not only help you understand optics, but also the EYE RELIEF/EYECUP USAGE LENS COATINGS EXIT PUPIL ABERRATIONS difference a quality optic can make in your appre- REAL FIELD OF VIEW ED GLASS AND SECONDARY SPECTRUMS ciation and intensity of every rare, special and daily APPARENT FIELD OF VIEW viewing experience. FIELD OF VIEW AT 1000 METERS 15-17 HOW TO CHOOSE FIELD FLATTENING (SUPER-WIDE) SELECTING A BINOCULAR BASED Nikon’s WX BINOCULAR UPON INTENDED APPLICATION LIGHT DELIVERY RESOLUTION 18-19 BINOCULAR OPTICS INTERPUPILLARY DISTANCE GLOSSARY DIOPTER ADJUSTMENT FOCUSING MECHANISMS INTERNAL ANTIREFLECTION OPTICS FIRST The guiding principle behind every Nikon since 1917 product has always been to engineer it from the inside out. By creating an optical system specific to the function of each product, Nikon can better match the product attri- butes specifically to the needs of the user. -
Rays, Waves, and Scattering: Topics in Classical Mathematical Physics
chapter1 February 28, 2017 © Copyright, Princeton University Press. No part of this book may be distributed, posted, or reproduced in any form by digital or mechanical means without prior written permission of the publisher. Chapter One Introduction Probably no mathematical structure is richer, in terms of the variety of physical situations to which it can be applied, than the equations and techniques that constitute wave theory. Eigenvalues and eigenfunctions, Hilbert spaces and abstract quantum mechanics, numerical Fourier analysis, the wave equations of Helmholtz (optics, sound, radio), Schrödinger (electrons in matter) ... variational methods, scattering theory, asymptotic evaluation of integrals (ship waves, tidal waves, radio waves around the earth, diffraction of light)—examples such as these jostle together to prove the proposition. M. V. Berry [1] There is a theory which states that if ever anyone discovers exactly what the Universe is for and why it is here, it will instantly disappear and be replaced by something even more bizarre and inexplicable. There is another theory which states that this has already happened. Douglas Adams [155] Douglas Adams’s famous Hitchhiker trilogy consists of five books; coincidentally this book addresses the three topics of rays, waves, and scattering in five parts: (i) Rays, (ii) Waves, (iii) Classical Scattering, (iv) Semiclassical Scattering, and (v) Special Topics in Scattering Theory (followed by six appendices, some of which deal with more specialized topics). I have tried to present a coherent account of each of these topics by separating them insofar as it is possible, but in a very real sense they are inseparable. We are in effect viewing each phenomenon (e.g. -
Studying Charged Particle Optics: an Undergraduate Course
IOP PUBLISHING EUROPEAN JOURNAL OF PHYSICS Eur. J. Phys. 29 (2008) 251–256 doi:10.1088/0143-0807/29/2/007 Studying charged particle optics: an undergraduate course V Ovalle1,DROtomar1,JMPereira2,NFerreira1, RRPinho3 and A C F Santos2,4 1 Instituto de Fisica, Universidade Federal Fluminense, Av. Gal. Milton Tavares de Souza s/n◦. Gragoata,´ Niteroi,´ 24210-346 Rio de Janeiro, Brazil 2 Instituto de Fisica, Universidade Federal do Rio de Janeiro, Caixa Postal 68528, Rio de Janeiro, Brazil 3 Departamento de F´ısica–ICE, Universidade Federal de Juiz de Fora, Campus Universitario,´ 36036-900, Juiz de Fora, MG, Brazil E-mail: [email protected] (A C F Santos) Received 23 August 2007, in final form 12 December 2007 Published 17 January 2008 Online at stacks.iop.org/EJP/29/251 Abstract This paper describes some computer-based activities to bring the study of charged particle optics to undergraduate students, to be performed as a part of a one-semester accelerator-based experimental course. The computational simulations were carried out using the commercially available SIMION program. The performance parameters, such as the focal length and P–Q curves are obtained. The three-electrode einzel lens is exemplified here as a study case. Introduction For many decades, physicists have been employing charged particle beams in order to investigate elementary processes in nuclear, atomic and particle physics using accelerators. In addition, many areas such as biology, chemistry, engineering, medicine, etc, have benefited from using beams of ions or electrons so that their phenomenological aspects can be understood. Among all its applications, electron microscopy may be one of the most important practical applications of lenses for charged particles. -
Geodesic Conformal Transformation Optics: Manipulating Light With
Geodesic conformal transformation optics: manipulating light with continuous refractive index profile Lin Xu1 , Tomáš Tyc 2 and Huanyang Chen1* 1 Institute of Electromagnetics and Acoustics and Department of Electronic Science, Xiamen University Xiamen 361005, China 2Department of Theoretical Physics and Astrophysics, Masaryk University, Kotlarska 2, 61137 Brno, Czech Republic Conformal transformation optics provides a simple scheme for manipulating light rays with inhomogeneous isotropic dielectrics. However, there is usually discontinuity for refractive index profile at branch cuts of different virtual Riemann sheets, hence compromising the functionalities. To deal with that, we present a special method for conformal transformation optics based on the concept of geodesic lens. The requirement is a continuous refractive index profile of dielectrics, which shows almost perfect performance of designed devices. We demonstrate such a proposal by achieving conformal transparency and reflection. We can further achieve conformal invisible cloaks by two techniques with perfect electromagnetic conductors. The geodesic concept may also find applications in other waves that obey the Helmholtz equation in two dimensions. Introduction.-Based on covariance of Maxwell’s equations and multi-linear constitutive equations, optical property of virtual space and physical space could be connected by a coordinate mapping [1]. In 2006, Leonhardt [2] presented that a conformal coordinate mapping between two complex planes could be performed for scalar field of refractive index of dielectrics such that light rays could be manipulated freely. Coincidentally, Pendry et al [3] provided a general method for controlling electromagnetic field in space of three dimensions. These two seminal papers launched a new research field named transformation optics (TO) [4-7], which originally mainly focused on optical invisibility. -
Geometric Optics 1 7.1 Overview
Contents III OPTICS ii 7 Geometric Optics 1 7.1 Overview...................................... 1 7.2 Waves in a Homogeneous Medium . 2 7.2.1 Monochromatic, Plane Waves; Dispersion Relation . ........ 2 7.2.2 WavePackets ............................... 4 7.3 Waves in an Inhomogeneous, Time-Varying Medium: The Eikonal Approxi- mationandGeometricOptics . .. .. .. 7 7.3.1 Geometric Optics for a Prototypical Wave Equation . ....... 8 7.3.2 Connection of Geometric Optics to Quantum Theory . ..... 11 7.3.3 GeometricOpticsforaGeneralWave . .. 15 7.3.4 Examples of Geometric-Optics Wave Propagation . ...... 17 7.3.5 Relation to Wave Packets; Breakdown of the Eikonal Approximation andGeometricOptics .......................... 19 7.3.6 Fermat’sPrinciple ............................ 19 7.4 ParaxialOptics .................................. 23 7.4.1 Axisymmetric, Paraxial Systems; Lenses, Mirrors, Telescope, Micro- scopeandOpticalCavity. 25 7.4.2 Converging Magnetic Lens for Charged Particle Beam . ....... 29 7.5 Catastrophe Optics — Multiple Images; Formation of Caustics and their Prop- erties........................................ 31 7.6 T2 Gravitational Lenses; Their Multiple Images and Caustics . ...... 39 7.6.1 T2 Refractive-Index Model of Gravitational Lensing . 39 7.6.2 T2 LensingbyaPointMass . .. .. 40 7.6.3 T2 LensingofaQuasarbyaGalaxy . 42 7.7 Polarization .................................... 46 7.7.1 Polarization Vector and its Geometric-Optics PropagationLaw. 47 7.7.2 T2 GeometricPhase .......................... 48 i Part III OPTICS ii Optics Version 1207.1.K.pdf, 28 October 2012 Prior to the twentieth century’s quantum mechanics and opening of the electromagnetic spectrum observationally, the study of optics was concerned solely with visible light. Reflection and refraction of light were first described by the Greeks and further studied by medieval scholastics such as Roger Bacon (thirteenth century), who explained the rain- bow and used refraction in the design of crude magnifying lenses and spectacles. -
Coulomb's Law Thu January 12, 2017 Ch16
Matching Objectives from AAMC report Scientific Foundations for Future Week Day Date Reading Content MCAT Content Categories Physicians 4C. Electrostatics:: Charge, conductors, charge conservation 1 Tue January 10, 2017 Ch16 - Electrostatics I 16.1-16.3 Electric Charge/ Coulomb's Law 4C. Electrostatics:: Insulators E1-2c. Use spatial reasoning to interpret multidimensional numerical and visual data (e.g., protein structure or geographic information or electric/magnetic 4C. Electrostatics:: Electric field: field lines Thu January 12, 2017 Ch16 - Electrostatics I 16.4 Electric Field fields). 4C. Electrostatics:: Electric field due to charge distribution E4-3a. Distinguish between ionic interactions, van derWaals interactions, hydrogen bonding, and hydrophobic interactions. Electric Field due to charge 2 Tue January 17, 2017 Ch16 - Electrostatics I 16.5 4C. Electrostatics:: Electric field due to charge distribution distributions Thu January 19, 2017 Ch16 - Electrostatics I 16.6 Gauss' Law 3 Tue January 24, 2017 Ch16 - Electrostatics I 16.7 Gauss' Law 4C. Electrostatics:: Electric field due to charge distribution Thu January 26, 2017 Ch17 - Electrostatics II 17.1-17.3 Electric Potential, Equipotential 4C. Electrostatics:: Potential difference, absolute potential at a location 4C. Circuit Elements:: Capacitance 4C. Circuit Elements:: Parallel plate capacitor Capacitors, Capacitor Combinations 4C. Circuit Elements:: Dielectrics 4 Tue January 31, 2017 Ch17 - Electrostatics II 17.4-17.7 and Dielectrics 4C. Circuit Elements:: Capacitors in series 4C. Circuit Elements:: Capacitors in parallel 4C. Circuit Elements:: Energy of charged capacitor 4C. Circuit Elements:: Current, sign conventions, units E3-2c. Apply understanding of electrical principles to the hazards of electrical Thu February 2, 2017 Ch18 - Moving Charges 18.1-18.3 Current and Resistance 4C. -
Geometrical Optics Notation & Sign Conventions
EELE 481/582 Optical Design Montana State University – S15 J. A. Shaw Geometrical Optics Notation & Sign Conventions Physics textbook convention (e.g. Hecht’s Optics) … not used in this class Object distances are positive to the left, negative to the right Image distances are negative to the left, positive to the right Optical engineering convention …what we will use Directed distances are positive to the right, negative to the left Angles are positive when they have positive slope relative to the local optical axis and negative when they have negative slope relative to the local optical axis. Curvature is positive when the center of curvature lies to the right Curvature is negative when the center of curvature lies to the left Index of refraction changes sign on reflection (e.g., air index = -1 after reflection) Effective focal length is positive if initially parallel rays are caused to converge; effective focal length is negative if initially parallel rays are caused to diverge Greivenkamp (Field Guide to Geometrical Optics) Thin lenses object n f n΄ image space space h (+) u (+) u΄ (-) h΄ (-) z (-) z΄ (+) L h' z' u Transverse magnification in air m h z u' n' Longitudinal magnification m m2 n 1 1 1 Image & object locations z' z f 1 Effective focal length f f EFL ( = optical power) E (sign denotes converging/diverging) Page 1 of 5 EELE 481/582 Optical Design Montana State University – S15 J. A. Shaw n Front focal length (directed distance) f nf F E n' Rear focal length (directed distance) f ' n' f R E f f ' Effective focal length from front or rear focal lengths f F R E n n' ☼ Note: the front and rear focal lengths are directed distances (signs determined by direction), but the effective focal length is not (its sign is determined by whether the surface or element causes incoming parallel rays to converge or diverge). -
Chapter 3 Geometrical Optics (A.K.A. Ray Optics
Chapter 3 Geometrical Optics (a.k.a. Ray Optics 3.1 Wavefront Geometrical optics is based on the wave theory of light, and it may be though of a tool that explain the behavior of light, and helps to predict what will happen with light in different situations. It's also the basis of constructing many types of optical devices, such as, e.g., photographic cameras, micro- scopes, telescopes, fiber light guides, and many others. Geometric optics is an extensive field, there is enough material in it to “fill” an entire academic course, even a two-term course. In Ph332, out of necessity, we can only devote to this material three class hours at the mos, so we have to limit ourselves to the most fundamental aspects of this field of optics. As mentioned, geometrical optics is based on the wave theory of light. We have already talked about waves, but only about the most simple ones, propagating in one direction along a single axis. But this is only a special case { in fact, there is a whole lot of other possible situations. A well- known scenario is a circular wave, which can be excited simply by throwing a stone into quiet lake water, as shown, e.g., in this Youtube clip. There are spherical waves { for instance, if an electronic speaker or any other small device generates a sound, the sound propagates in all direction, forming a spherical acoustic wave. In addition to that, the functions describing more complicated waves are 1 no longer as simple as those we used in Chapter 2, namely: 2π 2π ∆y(t) = A sin x − t λ T In the case of a circular wave spreading over a plane (e.g., on the lake surface), we need two coordinates to describe the position on the plane. -
Transmittance of Optical Glass TIE-35
Technical Information 1 Advanced Optics Version November 2020 TIE-35 Transmittance of optical glass Introduction 1. Theoretical background ......................... 1 Optical glasses are optimized to provide excellent transmit- tance throughout the total visible range from 380 to 780 nm 2. Wavelength dependence of transmittance ....... 2 (perception range of the human eye). Usually the transmit- 3. Measurement and specification.................. 7 tance range spreads also into the near UV and IR regions. As a general trend lowest refractive index glasses show high trans- 4. Literature........................................ 9 mittance far down to short wavelengths in the UV. Going to higher index glasses the UV absorption edge moves closer to the visible range. For highest index glass and larger thickness past. And for special applications where best transmittance the absorption edge already reaches into the visible range. is required SCHOTT offers improved quality grades like for This UV-edge shift with increasing refractive index is explained SF57 the grade SF57HTultra. by the general theory of absorbing dielectric media. So it may not be overcome in general. However, due to improved The aim of this technical information is to give the optical melting technology high refractive index glasses are offered designer a deeper understanding on the transmittance prop- nowadays with better blue-violet transmittance than in the erties of optical glass. 1. Theoretical background A light beam with the intensity I0 falls onto a glass plate having The beam reflected at the exit surface returns to the entrance a thickness d (figure 1). At the entrance surface part of the surface and is divided into a transmitted and a reflected part.