OPTI-202R Geometrical and Instrumental Optics John E. Greivenkamp Midterm II Page 1/8 Spring 2017
|
|
- Catherine Bates
- 5 years ago
- Views:
Transcription
1 OPTI-0R Geometrical and Instrumental Optics John E. Greivenkamp Midterm II Page /8 Spring 07 Name SOLUTIONS Closed book; closed notes. Time limit: 50 minutes. An equation sheet is attached and can be removed. A spare raytrace sheet is also attached. Use the back sides i required. Assume thin lenses in air i not speciied. As usual, only the magnitude o a magniication or magniying power may be given. I a method o solution is speciied in the problem, that method must be used. Raytraces must be done on the raytrace orm. Be sure to indicate the initial conditions or your rays. You must show your work and/or method o solution in order to receive credit or partial credit or your answer. Provide your answers in a neat and orderly ashion. No credit i it can t be read/ollowed. Only a basic scientiic calculator may be used. This calculator must not have programming or graphing capabilities. An acceptable example is the TI-30 calculator. Each student is responsible or obtaining their own calculator. Note: On some quantities, only the magnitude o the quantity is provided. The proper sign convention must be applied. ) (0 points) An optical system is comprised o two elements separating indices o reraction n, n and n 3. Subscript designates element, subscript designates element, and quantities without subscripts (EP, XP, P and P ) are associated with the total system. n n n XP EP 3 Stop P P P P P P Circle the index o reraction (and thereore the corresponding optical space) associated with each o the ollowing: EP: n n n 3 XP: n n n 3 P : n n n 3 P : n n n 3 P : n n n 3 P : n n n 3 P : n n n 3 P : n n n 3
2 OPTI-0R Geometrical and Instrumental Optics John E. Greivenkamp Midterm II Page /8 Spring 07 ) (40 points) A 5X Keplerian telescope is comprised o two thin lenses separated by 0 mm. The objective lens has a ocal length o 00 mm and it is 50 mm in diameter. The eye lens has a ocal length o 0 mm and it is mm in diameter. This telescope is to be used with a human eye, and the eye is placed at the exit pupil o the telescope. The eye has a 4 mm diameter entrance pupil. For distant objects, what is the unvignetted object ield o view (in degrees) o this system including the eye? A blank raytrace sheet is on the next page. OBJ D OBJ 00mm 50mm D 0mm mm DEYE 4mm t 0mm OBJ EYE ER Because DOBJ 5D, the objective lens is the stop o the telescope. The eye relie is ound by imaging the objective through the eye lens: OBJ t 0mm ER OBJ ER 4mm D XP DOBJ 50mm 0mm MP 5 The exit pupil o the telescope (0 mm) is larger than the entrance pupil o the eye (4 mm). When the eye is included in the system, the eye serves as the system stop.
3 OPTI-0R Geometrical and Instrumental Optics John E. Greivenkamp Midterm II Page 3/8 Spring 07 These results can be conirmed by tracing a potential chie ray and a potential marginal ray. The potential chie ray starts at the center o the objective lens and will cross the axis at the XP o the telescope and determines the ER. The potential marginal ray is launched at the edge o the objective lens (y = 5 mm) with a ero slope. As expected the potential marginal ray has a height o -5 mm at the eye. The system marginal ray is ound by scaling the potential marginal ray to the radius o the eye pupil ( mm). The scale actor is mm Scale Factor 0.4 5mm The system EP is at the objective lens with a diameter o 0 mm. Continues
4 OPTI-0R Geometrical and Instrumental Optics John E. Greivenkamp Midterm II Page 4/8 Spring 07 Since vignetting cannot occur at a stop or pupil, the ield o view is limited by the eye lens. The condition or no vignetting must be satisied at the eye lens using a scaled chie ray: a y y y C y y.0mm y.0mm a D 6.0mm a 6.0mm.0mm C.0 C Scale Factor The scaled chie ray has a height o 4.0mm at the eye lens. The chie ray slope in object space is uo This slope can be converted into the unvignetted FOV o the system: FOV tan u O.9deg FOV.9deg 3.8deg Unvignetted FOV = +/-.9 degrees
5 OPTI-0R Geometrical and Instrumental Optics John E. Greivenkamp Midterm II Page 5/8 Spring 07 3) (5 points) A doubly telecentric system is constructed out o two thin lenses in air. The spacing between the lenses is 50 mm, and the magnitude o the magniication m is /4. a) Design and sketch the layout o the system. Provide the required ocal lengths. A doubly telecentric system must be aocal (two positive lenses) with the stop at the common ocal point. The system magniication must be negative. m 4 t 50mm 4 00mm 50mm STOP F F F F 00mm 00mm 50mm 50mm = 00 mm = 50 mm Continue to Part b
6 OPTI-0R Geometrical and Instrumental Optics John E. Greivenkamp Midterm II Page 6/8 Spring 07 b) A mm high object is located 00 mm to the let o the irst lens o this system. Determine the location and sie o the image. Cascaded imaging may not be used (you may not image through one lens and then use this image as an object or the other lens). Raytrace methods may not be used or this problem. h STOP F F s A 00mm F 00mm 50mm F A 50mm h For imaging, use the longitudinal magniication with the ocal points as the reerence points. s m m m 4 6 h mm h mh 3.0mm The object is 00 mm to the let o the irst lens: s 00mm 00mm m 6.5mm A s 50mm 6.5mm 56.5mm A A A The image is to the right o the second lens. The image is 56.5_ mm to the R o L. The image height is -3.0 mm.
7 OPTI-0R Geometrical and Instrumental Optics John E. Greivenkamp Midterm II Page 7/8 Spring 07 4) (5 points) A ixed ocus camera uses a detector with 0 m x 0 m pixels. The camera lens has a ocal length o 5 mm. Objects rom m to ininity are imaged with acceptable image quality. The acceptable blur on the detector equals the pixel width. Assume a thin lens with the stop at the lens. Determine the required /# o the lens Determine the location o the detector relative to the rear ocal point o the lens. The hyperocal condition must be met: 5mm B 0 m 0.0mm L m L L m 000mm NEAR NEAR L D B B L D D.33mm / # / D /.5 To determine the detector location, image the hyperocal distance: 000mm 5.3mm The detector should be located 0.3 mm or 3 m to the right o the rear ocal point o the lens. System /# =.5 The detector is located _0.3_ mm to the _R_ o Fˊ.
8 OPTI-0R Geometrical and Instrumental Optics John E. Greivenkamp Midterm II Page 8/8 Spring 07 5) (0 points) A 50 mm ocal length relay lens is to be added to a simple 0X Keplerian telescope. In addition to erecting the image, the relay lens will also increase the magniying power o the telescope to 0X. ow much longer will the new telescope be as compared to the original Kelperian telescope? The original Keplerian telescope: The desired inal MP is 0X MP 0 LK OBJ EYE MP MP mrmpk mr.0 MP R m R R R R 3 R 50mm R R R 75mm 50mm R R K L 5mm L 5mm R OBJ EYE R R OBJ EYE K The 0X relayed Keplerian telescope is 5 mm longer than the original 0X Keplerian telescope. Increase in the length o the telescope = 5 mm
OPTI-202R Geometrical and Instrumental Optics John E. Greivenkamp Final Exam Page 1/11 Spring 2017
Final Exam Page 1/11 Spring 2017 Name SOLUTIONS Closed book; closed notes. Time limit: 120 minutes. An equation sheet is attached and can be removed. A spare raytrace sheet is also attached. Use the back
More informationOPTI-202R Geometrical and Instrumental Optics John E. Greivenkamp Midterm II Page 1/7 Spring 2018
Midterm II Page 1/7 Spring 2018 Name SOUTIONS Closed book; closed notes. Time limit: 50 minutes. An equation sheet is attached and can be removed. A spare raytrace sheet is also attached. Use the back
More informationElementary Optical Systems. Section 13. Magnifiers and Telescopes
13-1 Elementary Optical Systems Section 13 Magniiers and Telescopes Elementary Optical Systems Many optical systems can be understood when treated as combinations o thin lenses. Mirror equivalents exist
More informationArea of the Secondary Mirror Obscuration Ratio = Area of the EP Ignoring the Obscuration
Compact Gregorian Telescope Design a compact 10X25 Gregorian telescope. The Gregorian telescope provides an erect image and consists of two concave mirrors followed by an eyepiece to produce an afocal
More informationActually, you only need to design one monocular of the binocular.
orro rism Binoculars Design a pair of 8X40 binoculars: Actually, you only need to design one monocular of the binocular. Specifications: Objective ocal Length = 200 mm Eye Relief = 15 mm The system stop
More informationSection 11. Vignetting
Copright 2018 John E. Greivenkamp 11-1 Section 11 Vignetting Vignetting The stop determines the sie of the bundle of ras that propagates through the sstem for an on-axis object. As the object height increases,
More informationPhy 212: General Physics II
Phy 212: General Physics II Chapter 34: Images Lecture Notes Geometrical (Ray) Optics Geometrical Optics is an approximate treatment o light waves as straight lines (rays) or the description o image ormation
More informationSection 3. Imaging With A Thin Lens
3-1 Section 3 Imaging With A Thin Lens Object at Infinity An object at infinity produces a set of collimated set of rays entering the optical system. Consider the rays from a finite object located on the
More informationThin Lens and Image Formation
Pre-Lab Quiz / PHYS 4 Thin Lens and Image Formation Name Lab Section. What do you investigate in this lab?. The ocal length o a bi-convex thin lens is 0 cm. To a real image with magniication o, what is
More informationPhysics 142 Lenses and Mirrors Page 1. Lenses and Mirrors. Now for the sequence of events, in no particular order. Dan Rather
Physics 142 Lenses and Mirrors Page 1 Lenses and Mirrors Now or the sequence o events, in no particular order. Dan Rather Overview: making use o the laws o relection and reraction We will now study ormation
More informationDefinition of light rays
Geometrical optics In this section we study optical systems involving lenses and mirrors, developing an understanding o devices such as microscopes and telescopes, and biological systems such as the human
More informationRefraction and Lenses
Reraction and Lenses The most common application o reraction in science and technology is lenses. The kind o lenses we typically think o are made o glass or plastic. The basic rules o reraction still apply
More informationCOMP 558 lecture 5 Sept. 22, 2010
Up to now, we have taken the projection plane to be in ront o the center o projection. O course, the physical projection planes that are ound in cameras (and eyes) are behind the center o the projection.
More informationLecture 21: Cameras & Lenses II. Computer Graphics and Imaging UC Berkeley CS184/284A
Lecture 21: Cameras & Lenses II Computer Graphics and Imaging UC Berkeley Real Lens Designs Are Highly Complex [Apple] Topic o next lecture Real Lens Elements Are Not Ideal Aberrations Real plano-convex
More informationMarketed and Distributed by FaaDoOEngineers.com
REFRACTION OF LIGHT GUPTA CLASSES For any help contact: 995368795, 968789880 Nishant Gupta, D-, Prashant vihar, Rohini, Delhi-85 Contact: 995368795, 968789880 Reraction o light:. The ratio o the sine o
More informationTutorials in Opto-mechanics The calculation of focal length using the nodal slide
Tutorials in Opto-mechanics The calculation o ocal length using the nodal slide Yen-Te Lee Dec 1, 2008 1. Abstract First order properties completely describe the mapping rom object space to image space.
More information9. THINK A concave mirror has a positive value of focal length.
9. THINK A concave mirror has a positive value o ocal length. EXPRESS For spherical mirrors, the ocal length is related to the radius o curvature r by r/2. The object distance p, the image distance i,
More informationlens Figure 1. A refractory focusing arrangement. Focal point
Laboratory 2 - Introduction to Lenses & Telescopes Materials Used: A set o our lenses, an optical bench with a centimeter scale, a white screen, several lens holders, a light source (with crossed arrows),
More informationThin Lenses. Consider the situation below in which you have a real object at distance p from a converging lens of focal length f.
Thin Lenses Consider the situation below in which you have a real object at distance rom a converging lens o ocal length. Lens Object Image I > then a real image o this object will be roduced at distance
More information24 Geometrical Optics &...
804 CHAPTER 24 GEOMETRICAL OPTICS & OPTICAL EQUIPMEMT 24 Geometrical Optics &... Answers to Discussion Questions 24. The ocal length increases because the rays are not bent as strongly at the water-glasnterace.
More informationSIMPLE LENSES. To measure the focal lengths of several lens and lens combinations.
SIMPLE LENSES PURPOSE: To measure the ocal lengths o several lens and lens combinations. EQUIPMENT: Three convex lenses, one concave lens, lamp, image screen, lens holders, meter stick. INTRODUCTION: Combinations
More information(b) By measuring the image height for various image distances (adjusted by sliding the tubes together or apart) a relationship can be determined.
(c) The image is smaller, upright, virtual, ann the same side o the lens. Applying Inquiry Skills 7. (a) (b) By measuring the image height or various image distances (adjusted by sliding the tubes together
More informationElementary Optical Systems. Section 13. Magnifiers and Telescopes
Elementary Optical Systems Section 13 Magniiers and Telescopes 13-1 Elementary Optical Systems Many optical systems can be nderstood when treated as combinations o thin lenses. Mirror eqivalents exist
More informationAnnouncements. Focus! Thin Lens Models. New Topic. Intensity Image Formation. Bi-directional: two focal points! Thin Lens Model
Focus! Models Lecture #17 Tuesda, November 1 st, 2011 Announcements Programming Assignment #3 Is due a week rom Tuesda Midterm #2: two weeks rom Tuesda GTA survers: https://www.survemonke.com/r/shpj7j3
More informationThe Basic Geometry Behind A Camera Lens And A Magnifying Glass
The Basic Geometry Behind A Camera Lens And A Magniying Glass by John Kennedy Mathematics Department Santa Monica College 1 Pico Blvd. Santa Monica, CA 45 rkennedy@ix.netcom.com THE BASIC GEOMETRY BEHIND
More informationHow Do I Use Ray Diagrams to Predict How an Image Will Look?
How Do I Use Ray Diagrams to Predict How an Image Will Look? Description: Students will create ray diagrams to predict the type o image ormed. Student Materials (per group): Ray Diagrams Worksheet Ruler
More information3. What kind of mirror could you use to make image distance less than object distance?
REFLETION REVIEW hoose one o the ollowing to answer questions 7-24. A response may be used more than once. a. plane mirror e. plane mirror or convex mirror b. concave mirror. concave mirror or convex mirror
More informationPhysics 54. Lenses and Mirrors. And now for the sequence of events, in no particular order. Dan Rather
Physics 54 Lenses and Mirrors And now or the seuence o events, in no articular order. Dan Rather Overview We will now study transmission o light energy in the ray aroximation, which assumes that the energy
More informationEP118 Optics. Content TOPIC 9 ABERRATIONS. Department of Engineering Physics University of Gaziantep. 1. Introduction. 2. Spherical Aberrations
EP118 Optics TOPI 9 ABERRATIONS Department o Engineering Physics Uniersity o Gaziantep July 2011 Saya 1 ontent 1. Introduction 2. Spherical Aberrations 3. hromatic Aberrations 4. Other Types o Aberrations
More informationLecture 4: Geometrical Optics 2. Optical Systems. Images and Pupils. Rays. Wavefronts. Aberrations. Outline
Lecture 4: Geometrical Optics 2 Outline 1 Optical Systems 2 Images and Pupils 3 Rays 4 Wavefronts 5 Aberrations Christoph U. Keller, Leiden University, keller@strw.leidenuniv.nl Lecture 4: Geometrical
More informationYour Comments. That test was brutal, but this is the last physics course I have to take here WOOOOOO!!!!!
Your Comments I'm kind o lost, this was a pretty heavy prelecture. I understand the equations and how we get them but I'm araid to say that I don't understand the concepts behind everything. Such as what
More informationUnit #3 - Optics. Activity: D21 Observing Lenses (pg. 449) Lenses Lenses
ist10_ch11.qxd Unit #3 - Optics 11.3 Lenses 7/22/09 3:53 PM Page 449 Night vision goggles use lenses to ocus light onto a device called an image intensiier. Inside the intensiier, the light energy releases
More informationLens Design I. Lecture 3: Properties of optical systems II Herbert Gross. Summer term
Lens Design I Lecture 3: Properties of optical systems II 205-04-8 Herbert Gross Summer term 206 www.iap.uni-jena.de 2 Preliminary Schedule 04.04. Basics 2.04. Properties of optical systrems I 3 8.04.
More informationLenses & Prism c c h c. A transparent sbstance bonded by two sraces o deinite geometrical shape is called Lens. pond ish 2. A lens may be considered to be made p o a nmber o small prisms pt together. 3.
More informationLens Design I. Lecture 3: Properties of optical systems II Herbert Gross. Summer term
Lens Design I Lecture 3: Properties of optical systems II 207-04-20 Herbert Gross Summer term 207 www.iap.uni-jena.de 2 Preliminary Schedule - Lens Design I 207 06.04. Basics 2 3.04. Properties of optical
More informationOpti 415/515. Introduction to Optical Systems. Copyright 2009, William P. Kuhn
Opti 415/515 Introduction to Optical Systems 1 Optical Systems Manipulate light to form an image on a detector. Point source microscope Hubble telescope (NASA) 2 Fundamental System Requirements Application
More informationPhysics 141 Lecture 26
Physics 141 Lecture 26 Today s Concept: A) Lenses Electricity & Magne/sm Lecture 26, Slide 1 Mirrors in Movies Duck Soup (1933) The Lady rom Shanghai (1947) Enter the Dragon (1973) and many more Reraction
More informationPHY385H1F Introductory Optics Term Test 2 November 6, 2012 Duration: 50 minutes. NAME: Student Number:.
PHY385H1F Introductory Optics Term Test 2 November 6, 2012 Duration: 50 minutes NAME: Student Number:. Aids allowed: A pocket calculator with no communication ability. One 8.5x11 aid sheet, written on
More informationLecture 17. Image formation Ray tracing Calculation. Lenses Convex Concave. Mirrors Convex Concave. Optical instruments
Lecture 17. Image formation Ray tracing Calculation Lenses Convex Concave Mirrors Convex Concave Optical instruments Image formation Laws of refraction and reflection can be used to explain how lenses
More information3: Microscopic imaging
Ouline 3: Microscopic imaging Microscope layou Three limis o resoluion Diracion Pixel size Aberraions Comparison o elescopes and microscopes Rober R. McLeod, Universiy o Colorado 35 Microscope layou Anaomy
More informationA. Focal Length. 3. Lens Maker Equation. 2. Diverging Systems. f = 2 R. A. Focal Length B. Lens Law, object & image C. Optical Instruments
Physics 700 Geometric Optics Geometric Optics (rough drat) A. Focal Length B. Lens Law, object & image C. Optical Instruments W. Pezzaglia Updated: 0Aug A. Focal Length 3. Converging Systems 4. Converging
More information11.3. Lenses. Seeing in the Dark
.3 Lenses Here is a summary o what you will learn in this section: Lenses reract light in useul ways to orm s. Concave lenses, which cause light to diverge, are usen multi-lens systems to help produce
More informationPHYS 160 Astronomy. When analyzing light s behavior in a mirror or lens, it is helpful to use a technique called ray tracing.
Optics Introduction In this lab, we will be exploring several properties of light including diffraction, reflection, geometric optics, and interference. There are two sections to this lab and they may
More information2.71 Optics Fall 05 QUIZ 1 Wednesday, Oct. 12, 2005
2.71 Quiz 1 MASSACHUSETTS INSTITUTE OF TECHNOLOGY 2.71 Optics Fall 05 QUIZ 1 Wednesday, Oct. 12, 2005 1. (60%) The optical instrument shown below is a telephoto lens. It consists of a combination of two
More informationMODERN OPTICS -1. Tutorial Solutions
MODERN OPTICS - Tutorial Solutions Reision and General Optics All questions ere are general background optics wic will be assumed in tis course. Problem 3 requires tecnical details o te microscope wic
More informationOpto Engineering S.r.l.
TUTORIAL #1 Telecentric Lenses: basic information and working principles On line dimensional control is one of the most challenging and difficult applications of vision systems. On the other hand, besides
More informationTangents. The f-stops here. Shedding some light on the f-number. by Marcus R. Hatch and David E. Stoltzmann
Tangents Shedding some light on the f-number The f-stops here by Marcus R. Hatch and David E. Stoltzmann The f-number has peen around for nearly a century now, and it is certainly one of the fundamental
More informationMagnification, stops, mirrors More geometric optics
Magnification, stops, mirrors More geometric optics D. Craig 2005-02-25 Transverse magnification Refer to figure 5.22. By convention, distances above the optical axis are taken positive, those below, negative.
More informationSpeed and Image Brightness uniformity of telecentric lenses
Specialist Article Published by: elektronikpraxis.de Issue: 11 / 2013 Speed and Image Brightness uniformity of telecentric lenses Author: Dr.-Ing. Claudia Brückner, Optics Developer, Vision & Control GmbH
More informationPhys 531 Lecture 9 30 September 2004 Ray Optics II. + 1 s i. = 1 f
Phys 531 Lecture 9 30 September 2004 Ray Optics II Last time, developed idea of ray optics approximation to wave theory Introduced paraxial approximation: rays with θ 1 Will continue to use Started disussing
More informationMidterm Exam. Lasers. Gases and pressure. Lenses so far. Lenses and Cameras 4/9/2017. Office hours
Lights. Action. Phys 00, Day : Cameras Reminders: HW 9 due NOW and 0pm tonight on DL Lab 8 today/tomorrow Email AB and EH by THURSDAY i you need to do a make up lab MT 3 on THURSDAY Exam Thursday in class
More informationOPTICAL IMAGING AND ABERRATIONS
OPTICAL IMAGING AND ABERRATIONS PARTI RAY GEOMETRICAL OPTICS VIRENDRA N. MAHAJAN THE AEROSPACE CORPORATION AND THE UNIVERSITY OF SOUTHERN CALIFORNIA SPIE O P T I C A L E N G I N E E R I N G P R E S S A
More informationLecture 2: Geometrical Optics. Geometrical Approximation. Lenses. Mirrors. Optical Systems. Images and Pupils. Aberrations.
Lecture 2: Geometrical Optics Outline 1 Geometrical Approximation 2 Lenses 3 Mirrors 4 Optical Systems 5 Images and Pupils 6 Aberrations Christoph U. Keller, Leiden Observatory, keller@strw.leidenuniv.nl
More informationLens Design I. Lecture 5: Advanced handling I Herbert Gross. Summer term
Lens Design I Lecture 5: Advanced handling I 2015-05-11 Herbert Gross Summer term 2015 www.iap.uni-jena.de 2 Preliminary Schedule 1 13.04. Basics 2 20.04. Properties of optical systrems I 3 27.05. Properties
More informationCHAPTER 1 Optical Aberrations
CHAPTER 1 Optical Aberrations 1.1 INTRODUCTION This chapter starts with the concepts of aperture stop and entrance and exit pupils of an optical imaging system. Certain special rays, such as the chief
More informationWarren J. Smith Chief Scientist, Consultant Rockwell Collins Optronics Carlsbad, California
Modern Optical Engineering The Design of Optical Systems Warren J. Smith Chief Scientist, Consultant Rockwell Collins Optronics Carlsbad, California Fourth Edition Me Graw Hill New York Chicago San Francisco
More informationPhysics II. Chapter 23. Spring 2018
Physics II Chapter 23 Spring 2018 IMPORTANT: Except for multiple-choice questions, you will receive no credit if you show only an answer, even if the answer is correct. Always show in the space on your
More informationLights. Action. Cameras. Shutter/Iris Lens With focal length f. Image Distance. Object. Distance
Lights. Action. Phys 1020, Day 17: Cameras, Blm 15.1 Reminders: HW 8 in/hw 9 out Make up lab week straight ater Sp.B. Check scores on CU learn 1 Object Cameras Shutter/Iris Lens With ocal length Dark Box
More informationOPTI-202R Final Exam Name Spring 2008
OPTI-202R Final Exam Name Spring 2008 Note: Closed book; closed notes. Eqation sheets are inclded. A spare ratrace sheet is also attached. Assme thin lenses in air if not specified. If a method of soltion
More informationLecture 2: Geometrical Optics. Geometrical Approximation. Lenses. Mirrors. Optical Systems. Images and Pupils. Aberrations.
Lecture 2: Geometrical Optics Outline 1 Geometrical Approximation 2 Lenses 3 Mirrors 4 Optical Systems 5 Images and Pupils 6 Aberrations Christoph U. Keller, Leiden Observatory, keller@strw.leidenuniv.nl
More informationIntroduction. THE OPTICAL ENGINEERING PROCESS. Engineering Support. Fundamental Optics
Introduction The process o solving virtually any optical engineering problem can be broken down into two main steps. First, paraxial calculations (irst order) are made to determine critical parameters
More informationThree-Mirror Anastigmat Telescope with an Unvignetted Flat Focal Plane
Three-Mirror Anastigmat Telescope with an Unvignetted Flat Focal Plane arxiv:astro-ph/0504514v1 23 Apr 2005 Kyoji Nariai Department of Physics, Meisei University, Hino, Tokyo 191-8506 nariai.kyoji@gakushikai.jp
More informationSection 20. Chromatic Effects
Section 0 Chromatic Eects 0- Chromatic Aberration For a thin lens: n C C Since the inex changes with wavelength, so will the ocal length. 3 0- Where o Re, Green (or Yellow) an Blue ocus? n F C Because
More informationLens Design I. Lecture 5: Advanced handling I Herbert Gross. Summer term
Lens Design I Lecture 5: Advanced handling I 2018-05-17 Herbert Gross Summer term 2018 www.iap.uni-jena.de 2 Preliminary Schedule - Lens Design I 2018 1 12.04. Basics 2 19.04. Properties of optical systems
More informationIntroduction. Geometrical Optics. Milton Katz State University of New York. VfeWorld Scientific New Jersey London Sine Singapore Hong Kong
Introduction to Geometrical Optics Milton Katz State University of New York VfeWorld Scientific «New Jersey London Sine Singapore Hong Kong TABLE OF CONTENTS PREFACE ACKNOWLEDGMENTS xiii xiv CHAPTER 1:
More informationECEN 4606, UNDERGRADUATE OPTICS LAB
ECEN 4606, UNDERGRADUATE OPTICS LAB Lab 2: Imaging 1 the Telescope Original Version: Prof. McLeod SUMMARY: In this lab you will become familiar with the use of one or more lenses to create images of distant
More informationPHYSICS 289 Experiment 8 Fall Geometric Optics II Thin Lenses
PHYSICS 289 Experiment 8 Fall 2005 Geometric Optics II Thin Lenses Please look at the chapter on lenses in your text before this lab experiment. Please submit a short lab report which includes answers
More informationCompact camera module testing equipment with a conversion lens
Compact camera module testing equipment with a conversion lens Jui-Wen Pan* 1 Institute of Photonic Systems, National Chiao Tung University, Tainan City 71150, Taiwan 2 Biomedical Electronics Translational
More informationBig League Cryogenics and Vacuum The LHC at CERN
Big League Cryogenics and Vacuum The LHC at CERN A typical astronomical instrument must maintain about one cubic meter at a pressure of
More informationRefractive Power of a Surface. Exposure Sources. Thin Lenses. Thick Lenses. High Pressure Hg Arc Lamp Spectrum
eractive Power o a Surace The reractive power P is measured in diopters when the radius is expressed in meters. n and n are the reractive indices o the two media. EE-57: icrofabrication n n P n n Exposure
More informationOPTI-502 Optical Design and Instrumentation I John E. Greivenkamp Homework Set 5 Fall, 2018
Homework Set 5 all, 2018 Assigned: 9/26/18 Lecture 11 Due: 10/3/18 Lecture 13 Midterm Exam: Wednesday October 24 (Lecture 19) 5-1) Te following combination of tin lenses in air is in a telepoto configuration:
More informationBreaking Down The Cosine Fourth Power Law
Breaking Down The Cosine Fourth Power Law By Ronian Siew, inopticalsolutions.com Why are the corners of the field of view in the image captured by a camera lens usually darker than the center? For one
More informationAlgebra Based Physics. Reflection. Slide 1 / 66 Slide 2 / 66. Slide 3 / 66. Slide 4 / 66. Slide 5 / 66. Slide 6 / 66.
Slide 1 / 66 Slide 2 / 66 Algebra Based Physics Geometric Optics 2015-12-01 www.njctl.org Slide 3 / 66 Slide 4 / 66 Table of ontents lick on the topic to go to that section Reflection Refraction and Snell's
More information28 Thin Lenses: Ray Tracing
28 Thin Lenses: Ray Tracing A lens is a piece of transparent material whose surfaces have been shaped so that, when the lens is in another transparent material (call it medium 0), light traveling in medium
More informationIntroduction THE OPTICAL ENGINEERING PROCESS ENGINEERING SUPPORT
Material Properties Optical Speciications Gaussian Beam Optics Introduction Even though several thousand dierent optical components are listed in this catalog, perorming a ew simple calculations will usually
More informationGEOMETRICAL OPTICS AND OPTICAL DESIGN
GEOMETRICAL OPTICS AND OPTICAL DESIGN Pantazis Mouroulis Associate Professor Center for Imaging Science Rochester Institute of Technology John Macdonald Senior Lecturer Physics Department University of
More informationOptics Practice. Version #: 0. Name: Date: 07/01/2010
Optics Practice Date: 07/01/2010 Version #: 0 Name: 1. Which of the following diagrams show a real image? a) b) c) d) e) i, ii, iii, and iv i and ii i and iv ii and iv ii, iii and iv 2. A real image is
More informationProperties of optical instruments. Projection optical systems
Properties of optical instruments Projection optical systems Instruments : optical systems designed for a specific function Projection systems: : real image (object real or at infinity) Examples: videoprojector,,
More information( ) Deriving the Lens Transmittance Function. Thin lens transmission is given by a phase with unit magnitude.
Deriving the Lens Transmittance Function Thin lens transmission is given by a phase with unit magnitude. t(x, y) = exp[ jk o ]exp[ jk(n 1) (x, y) ] Find the thickness function for left half of the lens
More informationPost PDR Optical Design Study. Robert Barkhouser JHU/IDG January 6, 2014
ARCTIC Post PDR Optical Design Study Robert Barkhouser JHU/IDG January 6, 2014 1 APO 3.5 m Telescope Model From Joe H. as part of f8v240 imager model. dl Note (1) curved focal surface and (2) limiting
More informationApplied Optics. , Physics Department (Room #36-401) , ,
Applied Optics Professor, Physics Department (Room #36-401) 2290-0923, 019-539-0923, shsong@hanyang.ac.kr Office Hours Mondays 15:00-16:30, Wednesdays 15:00-16:30 TA (Ph.D. student, Room #36-415) 2290-0921,
More informationActivity 6.1 Image Formation from Spherical Mirrors
PHY385H1F Introductory Optics Practicals Day 6 Telescopes and Microscopes October 31, 2011 Group Number (number on Intro Optics Kit):. Facilitator Name:. Record-Keeper Name: Time-keeper:. Computer/Wiki-master:..
More informationLens Design I Seminar 1
Xiang Lu, Ralf Hambach Friedrich Schiller University Jena Institute of Applied Physics Albert-Einstein-Str 15 07745 Jena Lens Design I Seminar 1 Warm-Up (20min) Setup a single, symmetric, biconvex lens
More informationABSTRACT 1. INTRODUCTION
The role of aberrations in the relative illumination of a lens system Dmitry Reshidko* and Jose Sasian College of Optical Sciences, University of Arizona, Tucson, AZ, 857, USA ABSTRACT Several factors
More informationOptical Design with Zemax
Optical Design with Zemax Lecture 9: Advanced handling 2014-06-13 Herbert Gross Sommer term 2014 www.iap.uni-jena.de 2 Preliminary Schedule 1 11.04. Introduction 2 25.04. Properties of optical systems
More informationECEG105/ECEU646 Optics for Engineers Course Notes Part 4: Apertures, Aberrations Prof. Charles A. DiMarzio Northeastern University Fall 2008
ECEG105/ECEU646 Optics for Engineers Course Notes Part 4: Apertures, Aberrations Prof. Charles A. DiMarzio Northeastern University Fall 2008 July 2003+ Chuck DiMarzio, Northeastern University 11270-04-1
More informationExam Preparation Guide Geometrical optics (TN3313)
Exam Preparation Guide Geometrical optics (TN3313) Lectures: September - December 2001 Version of 21.12.2001 When preparing for the exam, check on Blackboard for a possible newer version of this guide.
More informationSystem/Prescription Data
System/Prescription Data File : U:\alpi's designs\1.0 Meter\1.0 meter optical design\old Lenses- Design Stuff\LCOGT 1.0meter Telescope Design for UCSB.zmx Title: LCOGT 1.0 Meter Telescope Date : THU NOV
More informationAn electrically tunable optical zoom system using two composite liquid crystal lenses with a large zoom ratio
An electrically tunable optical zoom system using two composite liquid crystal lenses with a large zoom ratio Yi-Hsin Lin,* Ming-Syuan Chen, and Hung-Chun Lin Department o Photonics, National Chiao Tung
More informationChapter 3 Op,cal Instrumenta,on
Imaging by an Op,cal System Change in curvature of wavefronts by a thin lens Chapter 3 Op,cal Instrumenta,on 3-1 Stops, Pupils, and Windows 3-4 The Camera 3-5 Simple Magnifiers and Eyepieces 1. Magnifiers
More informationOPTICAL SYSTEMS OBJECTIVES
101 L7 OPTICAL SYSTEMS OBJECTIVES Aims Your aim here should be to acquire a working knowledge of the basic components of optical systems and understand their purpose, function and limitations in terms
More informationChapter 34 Geometric Optics
Chapter 34 Geometric Optics Lecture by Dr. Hebin Li Goals of Chapter 34 To see how plane and curved mirrors form images To learn how lenses form images To understand how a simple image system works Reflection
More informationAstro 500 A500/L-8! 1!
Astro 500 1! Optics! Review! Compound systems: Outline o Pupils, stops, and telecentricity Telescopes! Review! Two-mirror systems! Figures of merit Examples: WIYN & SALT 2! Review: The Thin Lens! s parallel
More informationPhysics 222, October 25
Physics 222, October 25 Key Concepts: Image formation by refraction Thin lenses The eye Optical instruments A single flat interface Images can be formed by refraction, when light traverses a boundary between
More informationSequential Ray Tracing. Lecture 2
Sequential Ray Tracing Lecture 2 Sequential Ray Tracing Rays are traced through a pre-defined sequence of surfaces while travelling from the object surface to the image surface. Rays hit each surface once
More informationImage Formation. Light from distant things. Geometrical optics. Pinhole camera. Chapter 36
Light from distant things Chapter 36 We learn about a distant thing from the light it generates or redirects. The lenses in our eyes create images of objects our brains can process. This chapter concerns
More informationDepartment of Physics & Astronomy Undergraduate Labs. Thin Lenses
Thin Lenses Reflection and Refraction When light passes from one medium to another, part of the light is reflected and the rest is transmitted. Light rays that are transmitted undergo refraction (bending)
More informationAnnouncements. Image Formation: Outline. The course. How Cameras Produce Images. Earliest Surviving Photograph. Image Formation and Cameras
Announcements Image ormation and Cameras CSE 252A Lecture 3 Assignment 0: Getting Started with Matlab is posted to web page, due Tuesday, ctober 4. Reading: Szeliski, Chapter 2 ptional Chapters 1 & 2 of
More informationPLANE MIRRORS. The simplest mirror is a plane mirror a flat, reflective surface, often consisting of a metal film covered in glass. 4/2/2018.
4/2/208 UNIT 6 Geometri and physial optis AP PHYSICS 2 PLANE MIRRORS CHAPTER 22 Mirrors and lenses Plane mirrors The simplest mirror is a plane mirror a lat, reletive surae, oten onsisting o a metal ilm
More informationAlgebra Based Physics. Reflection. Slide 1 / 66 Slide 2 / 66. Slide 3 / 66. Slide 4 / 66. Slide 5 / 66. Slide 6 / 66.
Slide 1 / 66 Slide 2 / 66 lgebra ased Physics Geometric Optics 2015-12-01 www.njctl.org Slide 3 / 66 Slide 4 / 66 Table of ontents lick on the topic to go to that section Reflection Refraction and Snell's
More information