Cameras, lenses and sensors

Size: px
Start display at page:

Download "Cameras, lenses and sensors"

Transcription

1 Cameras, lenses and sensors Marc Pollefeys COMP 256

2 Cameras, lenses and sensors Camera Models Pinhole Perspective Projection Affine Projection Camera with Lenses Sensing The Human Eye Reading: Chapter.

3 Images are two-dimensional patterns of brightness values. Figure from US Navy Manual of Basic Optics and Optical Instruments, prepared by Bureau of Naval Personnel. Reprinted by Dover Publications, Inc., 969. They are formed by the projection of 3D objects.

4 Animal eye: a looonnng time ago. Photographic camera: Niepce, 86. Pinhole perspective projection: Brunelleschi, XV th Century. Camera obscura: XVI th Century.

5 Distant objects appear smaller

6 Parallel lines meet vanishing point

7 Vanishing points H VPL VPR VP VP 2 To different directions correspond different vanishing points VP 3

8 Geometric properties of projection Points go to points Lines go to lines Planes go to whole image or half-plane Polygons go to polygons Degenerate cases: line through focal point yields point plane through focal point yields line

9 Pinhole Perspective Equation x' y' f f x ' z y ' z

10 Affine projection models: Weak perspective projection x' mx y' my where m f z 0 ' is the magnification. When the scene relief is small compared its distance from the Camera, m can be taken constant: weak perspective projection.

11 Affine projection models: Orthographic projection x' y' x y When the camera is at a (roughly constant) distance from the scene, take m.

12 Planar pinhole perspective Orthographic projection Spherical pinhole perspective

13 Limits for pinhole cameras

14 Camera obscura + lens

15 Lenses Snell s law n sin α n 2 sin α 2 Descartes law

16 Paraxial (or first-order) optics Snell s law: n sin α n 2 sin α 2 Small angles: n α n 2 α 2 R n n d n d n R γ β α h d h R β γ α d h h R R d h h n h d h n

17 Thin Lenses ) 2( and ' n R f f z z R n n * + R n n + ' * R n n * ' R n R n spherical lens surfaces; incoming light ± parallel to axis; thickness << radii; same refractive index on both sides ' * R n n R n n d n d n

18 Thin Lenses x' y' z' z' x z y z where z' z f and f R 2( n )

19 Thick Lens

20 The depth-of-field

21 The depth-of-field f o i + + Δ i i i f f i i o yields d b i i i Δ + Δ i i b d b Δ f b d f f o o o / ) ( 0 o o + Δ Similar formula for o o o Δ + + ) ( / b d d i i f f o o i ) ( 0 o b d f b d f o +

22 The depth-of-field f b d f f + Δ / ) ( decreases with d, increases with 0 strike a balance between incoming light and sharp depth range

23 Deviations from the lens model 3 assumptions :. all rays from a point are focused onto image point 2. all image points in a single plane 3. magnification is constant deviations from this ideal are aberrations

24 Aberrations 2 types :. geometrical 2. chromatic geometrical : small for paraxial rays study through 3 rd order optics chromatic : refractive index function of wavelength

25 Geometrical aberrations spherical aberration astigmatism distortion coma aberrations are reduced by combining lenses

26 Spherical aberration rays parallel to the axis do not converge outer portions of the lens yield smaller focal lenghts

27 Astigmatism Different focal length for inclined rays

28 Distortion magnification/focal length different for different angles of inclination pincushion (tele-photo) barrel (wide-angle) Can be corrected! (if parameters are know)

29 Coma point off the axis depicted as comet shaped blob

30 Chromatic aberration rays of different wavelengths focused in different planes cannot be removed completely sometimes achromatization is achieved for more than 2 wavelengths

31 Lens materials reference wavelengths : λ F 486.3nm λ d nm λ C nm lens characteristics :. refractive index n d 2. Abbe number V d (n d -) / (n F -n C ) typically, both should be high allows small components with sufficient refraction notation : e.g. glass BK7(57642) n d.57 and V d 64.2

32 Lens materials Crown Glass Fused Quartz & Fused Silica Calcium Fluoride 9000 Germanium 4000 inc Selenide Saphire Plastic (PMMA) WAVELENGTH (nm) additional considerations : humidity and temperature resistance, weight, price,...

33 Vignetting Darkening of images near the corner The white openings in the top illustrations denote the entrance pupil, which is the image of the aperture stop seen through all lens elements in front of it and from a position on the optical axis. The bottom illustrations show the lens from the semifield angle. Here, the white openings correspond to the clear aperture for light that is heading for the image corner. Figure from

34 Photographs (Niepce, La Table Servie, 822) Milestones: Daguerreotypes (839) Photographic Film (Eastman,889) Cinema (Lumière Brothers,895) Color Photography (Lumière Brothers, 908) Television (Baird, Farnsworth, worykin, 920s) Collection Harlingue-Viollet. CCD Devices (970) more recently CMOS

35 Cameras we consider 2 types :. CCD 2. CMOS

36 CCD separate photo sensor at regular positions no scanning charge-coupled devices (CCDs) area CCDs and linear CCDs 2 area architectures : interline transfer and frame transfer photosensitive storage

37 The CCD camera

38 CMOS Same sensor elements as CCD Each photo sensor has its own amplifier More noise (reduced by subtracting black image) Lower sensitivity (lower fill rate) Uses standard CMOS technology Allows to put other components on chip Smart pixels Foveon 4k x 4k sensor 0.8μ process 70M transistors

39 CCD vs. CMOS Mature technology Specific technology High production cost High power consumption Higher fill rate Blooming Sequential readout Recent technology Standard IC technology Cheap Low power Less sensitive Per pixel amplification Random pixel access Smart pixels On chip integration with other components

40 Color cameras We consider 3 concepts:. Prism (with 3 sensors) 2. Filter mosaic 3. Filter wheel and X3

41 Prism color camera Separate light in 3 beams using dichroic prism Requires 3 sensors & precise alignment Good color separation

42 Prism color camera

43 Filter mosaic Coat filter directly on sensor Demosaicing (obtain full colour & full resolution image)

44 Filter wheel Rotate multiple filters in front of lens Allows more than 3 colour bands Only suitable for static scenes

45 Prism vs. mosaic vs. wheel approach Prism Mosaic Wheel # sensors 3 Separation High Average Good Cost High Low Average Framerate High High Low Artefacts Low Aliasing Motion Bands or more High-end cameras Low-end cameras Scientific applications

46 three layers of pixels. The layers of pixels are embedded in silicon to take advantage of the fact that red, green, and blue light penetrate silicon to different depths Computer new color CMOS sensor Foveon s X3 better image quality smarter pixels

47 The Human Eye Reproduced by permission, the American Society of Photogrammetry and Remote Sensing. A.L. Nowicki, Stereoscopy. Manual of Photogrammetry, Thompson, Radlinski, and Speert (eds.), third edition, 966. Helmoltz s Schematic Eye

48 The distribution of rods and cones across the retina Reprinted from Foundations of, by B. Wandell, Sinauer Associates, Inc., (995). 995 Sinauer Associates, Inc. Cones in the fovea Rods and cones in the periphery Reprinted from Foundations of, by B. Wandell, Sinauer Associates, Inc., (995). 995 Sinauer Associates, Inc.

49 Next class Radiometry: lights and surfaces

Image Formation: Camera Model

Image Formation: Camera Model Image Formation: Camera Model Ruigang Yang COMP 684 Fall 2005, CS684-IBMR Outline Camera Models Pinhole Perspective Projection Affine Projection Camera with Lenses Digital Image Formation The Human Eye

More information

CS 443: Imaging and Multimedia Cameras and Lenses

CS 443: Imaging and Multimedia Cameras and Lenses CS 443: Imaging and Multimedia Cameras and Lenses Spring 2008 Ahmed Elgammal Dept of Computer Science Rutgers University Outlines Cameras and lenses! 1 They are formed by the projection of 3D objects.

More information

Image Formation III Chapter 1 (Forsyth&Ponce) Cameras Lenses & Sensors

Image Formation III Chapter 1 (Forsyth&Ponce) Cameras Lenses & Sensors Image Formation III Chapter 1 (Forsyth&Ponce) Cameras Lenses & Sensors Guido Gerig CS-GY 6643, Spring 2017 (slides modified from Marc Pollefeys, UNC Chapel Hill/ ETH Zurich, With content from Prof. Trevor

More information

Announcements. Image Formation: Outline. The course. How Cameras Produce Images. Earliest Surviving Photograph. Image Formation and Cameras

Announcements. 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 information

Building a Real Camera

Building a Real Camera Building a Real Camera Home-made pinhole camera Slide by A. Efros http://www.debevec.org/pinhole/ Shrinking the aperture Why not make the aperture as small as possible? Less light gets through Diffraction

More information

Building a Real Camera. Slides Credit: Svetlana Lazebnik

Building a Real Camera. Slides Credit: Svetlana Lazebnik Building a Real Camera Slides Credit: Svetlana Lazebnik Home-made pinhole camera Slide by A. Efros http://www.debevec.org/pinhole/ Shrinking the aperture Why not make the aperture as small as possible?

More information

Cameras, lenses, and sensors

Cameras, lenses, and sensors Cameras, lenses, and sensors Reading: Chapter 1, Forsyth & Ponce Optional: Section 2.1, 2.3, Horn. 6.801/6.866 Profs. Bill Freeman and Trevor Darrell Sept. 10, 2002 Today s lecture How many people would

More information

Cameras. CSE 455, Winter 2010 January 25, 2010

Cameras. CSE 455, Winter 2010 January 25, 2010 Cameras CSE 455, Winter 2010 January 25, 2010 Announcements New Lecturer! Neel Joshi, Ph.D. Post-Doctoral Researcher Microsoft Research neel@cs Project 1b (seam carving) was due on Friday the 22 nd Project

More information

Image Formation and Capture

Image Formation and Capture Figure credits: B. Curless, E. Hecht, W.J. Smith, B.K.P. Horn, A. Theuwissen, and J. Malik Image Formation and Capture COS 429: Computer Vision Image Formation and Capture Real world Optics Sensor Devices

More information

Image Formation and Capture. Acknowledgment: some figures by B. Curless, E. Hecht, W.J. Smith, B.K.P. Horn, and A. Theuwissen

Image Formation and Capture. Acknowledgment: some figures by B. Curless, E. Hecht, W.J. Smith, B.K.P. Horn, and A. Theuwissen Image Formation and Capture Acknowledgment: some figures by B. Curless, E. Hecht, W.J. Smith, B.K.P. Horn, and A. Theuwissen Image Formation and Capture Real world Optics Sensor Devices Sources of Error

More information

CPSC 425: Computer Vision

CPSC 425: Computer Vision 1 / 55 CPSC 425: Computer Vision Instructor: Fred Tung ftung@cs.ubc.ca Department of Computer Science University of British Columbia Lecture Notes 2015/2016 Term 2 2 / 55 Menu January 7, 2016 Topics: Image

More information

CS6670: Computer Vision

CS6670: Computer Vision CS6670: Computer Vision Noah Snavely Lecture 4a: Cameras Source: S. Lazebnik Reading Szeliski chapter 2.2.3, 2.3 Image formation Let s design a camera Idea 1: put a piece of film in front of an object

More information

Lecture 7: Camera Models

Lecture 7: Camera Models Lecture 7: Camera Models Professor Stanford Vision Lab 1 What we will learn toda? Pinhole cameras Cameras & lenses The geometr of pinhole cameras Reading: [FP]Chapters 1 3 [HZ] Chapter 6 2 What we will

More information

VC 14/15 TP2 Image Formation

VC 14/15 TP2 Image Formation VC 14/15 TP2 Image Formation Mestrado em Ciência de Computadores Mestrado Integrado em Engenharia de Redes e Sistemas Informáticos Miguel Tavares Coimbra Outline Computer Vision? The Human Visual System

More information

Acquisition. Some slides from: Yung-Yu Chuang (DigiVfx) Jan Neumann, Pat Hanrahan, Alexei Efros

Acquisition. Some slides from: Yung-Yu Chuang (DigiVfx) Jan Neumann, Pat Hanrahan, Alexei Efros Acquisition Some slides from: Yung-Yu Chuang (DigiVfx) Jan Neumann, Pat Hanrahan, Alexei Efros Image Acquisition Digital Camera Film Outline Pinhole camera Lens Lens aberrations Exposure Sensors Noise

More information

Optical Components for Laser Applications. Günter Toesko - Laserseminar BLZ im Dezember

Optical Components for Laser Applications. Günter Toesko - Laserseminar BLZ im Dezember Günter Toesko - Laserseminar BLZ im Dezember 2009 1 Aberrations An optical aberration is a distortion in the image formed by an optical system compared to the original. It can arise for a number of reasons

More information

VC 11/12 T2 Image Formation

VC 11/12 T2 Image Formation VC 11/12 T2 Image Formation Mestrado em Ciência de Computadores Mestrado Integrado em Engenharia de Redes e Sistemas Informáticos Miguel Tavares Coimbra Outline Computer Vision? The Human Visual System

More information

Applied Optics. , Physics Department (Room #36-401) , ,

Applied 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 information

OPTICAL SYSTEMS OBJECTIVES

OPTICAL 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 information

Projection. Announcements. Müller-Lyer Illusion. Image formation. Readings Nalwa 2.1

Projection. Announcements. Müller-Lyer Illusion. Image formation. Readings Nalwa 2.1 Announcements Mailing list (you should have received messages) Project 1 additional test sequences online Projection Readings Nalwa 2.1 Müller-Lyer Illusion Image formation object film by Pravin Bhat http://www.michaelbach.de/ot/sze_muelue/index.html

More information

Lenses, exposure, and (de)focus

Lenses, exposure, and (de)focus Lenses, exposure, and (de)focus http://graphics.cs.cmu.edu/courses/15-463 15-463, 15-663, 15-862 Computational Photography Fall 2017, Lecture 15 Course announcements Homework 4 is out. - Due October 26

More information

Optical Systems: Pinhole Camera Pinhole camera: simple hole in a box: Called Camera Obscura Aristotle discussed, Al-Hazen analyzed in Book of Optics

Optical Systems: Pinhole Camera Pinhole camera: simple hole in a box: Called Camera Obscura Aristotle discussed, Al-Hazen analyzed in Book of Optics Optical Systems: Pinhole Camera Pinhole camera: simple hole in a box: Called Camera Obscura Aristotle discussed, Al-Hazen analyzed in Book of Optics 1011CE Restricts rays: acts as a single lens: inverts

More information

Lecture 2: Geometrical Optics. Geometrical Approximation. Lenses. Mirrors. Optical Systems. Images and Pupils. Aberrations.

Lecture 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 information

VC 16/17 TP2 Image Formation

VC 16/17 TP2 Image Formation VC 16/17 TP2 Image Formation Mestrado em Ciência de Computadores Mestrado Integrado em Engenharia de Redes e Sistemas Informáticos Hélder Filipe Pinto de Oliveira Outline Computer Vision? The Human Visual

More information

LENSES. INEL 6088 Computer Vision

LENSES. INEL 6088 Computer Vision LENSES INEL 6088 Computer Vision Digital camera A digital camera replaces film with a sensor array Each cell in the array is a Charge Coupled Device light-sensitive diode that converts photons to electrons

More information

Lecture 2: Geometrical Optics. Geometrical Approximation. Lenses. Mirrors. Optical Systems. Images and Pupils. Aberrations.

Lecture 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 information

CS6670: Computer Vision

CS6670: Computer Vision CS6670: Computer Vision Noah Snavely Lecture 5: Cameras and Projection Szeliski 2.1.3-2.1.6 Reading Announcements Project 1 assigned, see projects page: http://www.cs.cornell.edu/courses/cs6670/2011sp/projects/projects.html

More information

Chapters 1 & 2. Definitions and applications Conceptual basis of photogrammetric processing

Chapters 1 & 2. Definitions and applications Conceptual basis of photogrammetric processing Chapters 1 & 2 Chapter 1: Photogrammetry Definitions and applications Conceptual basis of photogrammetric processing Transition from two-dimensional imagery to three-dimensional information Automation

More information

Lecture 4: Geometrical Optics 2. Optical Systems. Images and Pupils. Rays. Wavefronts. Aberrations. Outline

Lecture 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 information

IMAGE SENSOR SOLUTIONS. KAC-96-1/5" Lens Kit. KODAK KAC-96-1/5" Lens Kit. for use with the KODAK CMOS Image Sensors. November 2004 Revision 2

IMAGE SENSOR SOLUTIONS. KAC-96-1/5 Lens Kit. KODAK KAC-96-1/5 Lens Kit. for use with the KODAK CMOS Image Sensors. November 2004 Revision 2 KODAK for use with the KODAK CMOS Image Sensors November 2004 Revision 2 1.1 Introduction Choosing the right lens is a critical aspect of designing an imaging system. Typically the trade off between image

More information

CSE 473/573 Computer Vision and Image Processing (CVIP)

CSE 473/573 Computer Vision and Image Processing (CVIP) CSE 473/573 Computer Vision and Image Processing (CVIP) Ifeoma Nwogu inwogu@buffalo.edu Lecture 4 Image formation(part I) Schedule Last class linear algebra overview Today Image formation and camera properties

More information

Lenses. Overview. Terminology. The pinhole camera. Pinhole camera Lenses Principles of operation Limitations

Lenses. Overview. Terminology. The pinhole camera. Pinhole camera Lenses Principles of operation Limitations Overview Pinhole camera Principles of operation Limitations 1 Terminology The pinhole camera The first camera - camera obscura - known to Aristotle. In 3D, we can visualize the blur induced by the pinhole

More information

Laboratory experiment aberrations

Laboratory experiment aberrations Laboratory experiment aberrations Obligatory laboratory experiment on course in Optical design, SK2330/SK3330, KTH. Date Name Pass Objective This laboratory experiment is intended to demonstrate the most

More information

Image Formation. Light from distant things. Geometrical optics. Pinhole camera. Chapter 36

Image 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 information

Waves & Oscillations

Waves & Oscillations Physics 42200 Waves & Oscillations Lecture 33 Geometric Optics Spring 2013 Semester Matthew Jones Aberrations We have continued to make approximations: Paraxial rays Spherical lenses Index of refraction

More information

COURSE NAME: PHOTOGRAPHY AND AUDIO VISUAL PRODUCTION (VOCATIONAL) FOR UNDER GRADUATE (FIRST YEAR)

COURSE NAME: PHOTOGRAPHY AND AUDIO VISUAL PRODUCTION (VOCATIONAL) FOR UNDER GRADUATE (FIRST YEAR) COURSE NAME: PHOTOGRAPHY AND AUDIO VISUAL PRODUCTION (VOCATIONAL) FOR UNDER GRADUATE (FIRST YEAR) PAPER TITLE: BASIC PHOTOGRAPHIC UNIT - 3 : SIMPLE LENS TOPIC: LENS PROPERTIES AND DEFECTS OBJECTIVES By

More information

Announcement A total of 5 (five) late days are allowed for projects. Office hours

Announcement A total of 5 (five) late days are allowed for projects. Office hours Announcement A total of 5 (five) late days are allowed for projects. Office hours Me: 3:50-4:50pm Thursday (or by appointment) Jake: 12:30-1:30PM Monday and Wednesday Image Formation Digital Camera Film

More information

ECEG105/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 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 information

IMAGE FORMATION. Light source properties. Sensor characteristics Surface. Surface reflectance properties. Optics

IMAGE FORMATION. Light source properties. Sensor characteristics Surface. Surface reflectance properties. Optics IMAGE FORMATION Light source properties Sensor characteristics Surface Exposure shape Optics Surface reflectance properties ANALOG IMAGES An image can be understood as a 2D light intensity function f(x,y)

More information

Chapter 25 Optical Instruments

Chapter 25 Optical Instruments Chapter 25 Optical Instruments Units of Chapter 25 Cameras, Film, and Digital The Human Eye; Corrective Lenses Magnifying Glass Telescopes Compound Microscope Aberrations of Lenses and Mirrors Limits of

More information

Unit 1: Image Formation

Unit 1: Image Formation Unit 1: Image Formation 1. Geometry 2. Optics 3. Photometry 4. Sensor Readings Szeliski 2.1-2.3 & 6.3.5 1 Physical parameters of image formation Geometric Type of projection Camera pose Optical Sensor

More information

Chapter 36. Image Formation

Chapter 36. Image Formation Chapter 36 Image Formation Image of Formation Images can result when light rays encounter flat or curved surfaces between two media. Images can be formed either by reflection or refraction due to these

More information

CHAPTER 18 REFRACTION & LENSES

CHAPTER 18 REFRACTION & LENSES Physics Approximate Timeline Students are expected to keep up with class work when absent. CHAPTER 18 REFRACTION & LENSES Day Plans for the day Assignments for the day 1 18.1 Refraction of Light o Snell

More information

Colorado School of Mines. Computer Vision. Professor William Hoff Dept of Electrical Engineering &Computer Science.

Colorado School of Mines. Computer Vision. Professor William Hoff Dept of Electrical Engineering &Computer Science. Professor William Hoff Dept of Electrical Engineering &Computer Science http://inside.mines.edu/~whoff/ 1 Sensors and Image Formation Imaging sensors and models of image formation Coordinate systems Digital

More information

CSE 527: Introduction to Computer Vision

CSE 527: Introduction to Computer Vision CSE 527: Introduction to Computer Vision Week 2 - Class 2: Vision, Physics, Cameras September 7th, 2017 Today Physics Human Vision Eye Brain Perspective Projection Camera Models Image Formation Digital

More information

Chapter 36. Image Formation

Chapter 36. Image Formation Chapter 36 Image Formation Notation for Mirrors and Lenses The object distance is the distance from the object to the mirror or lens Denoted by p The image distance is the distance from the image to the

More information

Lecture 2 Camera Models

Lecture 2 Camera Models Lecture 2 Camera Models Professor Silvio Savarese Computational Vision and Geometr Lab Silvio Savarese Lecture 2 - -Jan-8 Lecture 2 Camera Models Pinhole cameras Cameras lenses The geometr of pinhole cameras

More information

GEOMETRICAL OPTICS AND OPTICAL DESIGN

GEOMETRICAL 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 information

INTRODUCTION THIN LENSES. Introduction. given by the paraxial refraction equation derived last lecture: Thin lenses (19.1) = 1. Double-lens systems

INTRODUCTION THIN LENSES. Introduction. given by the paraxial refraction equation derived last lecture: Thin lenses (19.1) = 1. Double-lens systems Chapter 9 OPTICAL INSTRUMENTS Introduction Thin lenses Double-lens systems Aberrations Camera Human eye Compound microscope Summary INTRODUCTION Knowledge of geometrical optics, diffraction and interference,

More information

Astronomy 80 B: Light. Lecture 9: curved mirrors, lenses, aberrations 29 April 2003 Jerry Nelson

Astronomy 80 B: Light. Lecture 9: curved mirrors, lenses, aberrations 29 April 2003 Jerry Nelson Astronomy 80 B: Light Lecture 9: curved mirrors, lenses, aberrations 29 April 2003 Jerry Nelson Sensitive Countries LLNL field trip 2003 April 29 80B-Light 2 Topics for Today Optical illusion Reflections

More information

brief history of photography foveon X3 imager technology description

brief history of photography foveon X3 imager technology description brief history of photography foveon X3 imager technology description imaging technology 30,000 BC chauvet-pont-d arc pinhole camera principle first described by Aristotle fourth century B.C. oldest known

More information

Projection. Readings. Szeliski 2.1. Wednesday, October 23, 13

Projection. Readings. Szeliski 2.1. Wednesday, October 23, 13 Projection Readings Szeliski 2.1 Projection Readings Szeliski 2.1 Müller-Lyer Illusion by Pravin Bhat Müller-Lyer Illusion by Pravin Bhat http://www.michaelbach.de/ot/sze_muelue/index.html Müller-Lyer

More information

Lecture 02 Image Formation 1

Lecture 02 Image Formation 1 Institute of Informatics Institute of Neuroinformatics Lecture 02 Image Formation 1 Davide Scaramuzza http://rpg.ifi.uzh.ch 1 Lab Exercise 1 - Today afternoon Room ETH HG E 1.1 from 13:15 to 15:00 Work

More information

Cameras. Shrinking the aperture. Camera trial #1. Pinhole camera. Digital Visual Effects Yung-Yu Chuang. Put a piece of film in front of an object.

Cameras. Shrinking the aperture. Camera trial #1. Pinhole camera. Digital Visual Effects Yung-Yu Chuang. Put a piece of film in front of an object. Camera trial #1 Cameras Digital Visual Effects Yung-Yu Chuang scene film with slides by Fredo Durand, Brian Curless, Steve Seitz and Alexei Efros Put a piece of film in front of an object. Pinhole camera

More information

TSBB09 Image Sensors 2018-HT2. Image Formation Part 1

TSBB09 Image Sensors 2018-HT2. Image Formation Part 1 TSBB09 Image Sensors 2018-HT2 Image Formation Part 1 Basic physics Electromagnetic radiation consists of electromagnetic waves With energy That propagate through space The waves consist of transversal

More information

Explanation of Aberration and Wavefront

Explanation of Aberration and Wavefront Explanation of Aberration and Wavefront 1. What Causes Blur? 2. What is? 4. What is wavefront? 5. Hartmann-Shack Aberrometer 6. Adoption of wavefront technology David Oh 1. What Causes Blur? 2. What is?

More information

Ch 24. Geometric Optics

Ch 24. Geometric Optics text concept Ch 24. Geometric Optics Fig. 24 3 A point source of light P and its image P, in a plane mirror. Angle of incidence =angle of reflection. text. Fig. 24 4 The blue dashed line through object

More information

Announcements. The appearance of colors

Announcements. The appearance of colors Announcements Introduction to Computer Vision CSE 152 Lecture 6 HW1 is assigned See links on web page for readings on color. Oscar Beijbom will be giving the lecture on Tuesday. I will not be holding office

More information

Cameras. Steve Rotenberg CSE168: Rendering Algorithms UCSD, Spring 2017

Cameras. Steve Rotenberg CSE168: Rendering Algorithms UCSD, Spring 2017 Cameras Steve Rotenberg CSE168: Rendering Algorithms UCSD, Spring 2017 Camera Focus Camera Focus So far, we have been simulating pinhole cameras with perfect focus Often times, we want to simulate more

More information

AST Lab exercise: aberrations

AST Lab exercise: aberrations AST2210 - Lab exercise: aberrations 1 Introduction This lab exercise will take you through the most common types of aberrations. 2 Chromatic aberration Chromatic aberration causes lens to have dierent

More information

INDEX OF REFRACTION index of refraction n = c/v material index of refraction n

INDEX OF REFRACTION index of refraction n = c/v material index of refraction n INDEX OF REFRACTION The index of refraction (n) of a material is the ratio of the speed of light in vacuuo (c) to the speed of light in the material (v). n = c/v Indices of refraction for any materials

More information

Introduction. Geometrical Optics. Milton Katz State University of New York. VfeWorld Scientific New Jersey London Sine Singapore Hong Kong

Introduction. 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 information

The Camera : Computational Photography Alexei Efros, CMU, Fall 2008

The Camera : Computational Photography Alexei Efros, CMU, Fall 2008 The Camera 15-463: Computational Photography Alexei Efros, CMU, Fall 2008 How do we see the world? object film Let s design a camera Idea 1: put a piece of film in front of an object Do we get a reasonable

More information

Lens Design II Seminar 6 (Solutions)

Lens Design II Seminar 6 (Solutions) 2017-01-04 Prof. Herbert Gross Yi Zhong, Norman G. Worku Friedrich Schiller University Jena Institute of Applied Physics Albert-Einstein-Str 15 07745 Jena Lens Design II Seminar 6 (Solutions) 6.1. Correction

More information

Projection. Projection. Image formation. Müller-Lyer Illusion. Readings. Readings. Let s design a camera. Szeliski 2.1. Szeliski 2.

Projection. Projection. Image formation. Müller-Lyer Illusion. Readings. Readings. Let s design a camera. Szeliski 2.1. Szeliski 2. Projection Projection Readings Szeliski 2.1 Readings Szeliski 2.1 Müller-Lyer Illusion Image formation object film by Pravin Bhat http://www.michaelbach.de/ot/sze_muelue/index.html Let s design a camera

More information

Converging and Diverging Surfaces. Lenses. Converging Surface

Converging and Diverging Surfaces. Lenses. Converging Surface Lenses Sandy Skoglund 2 Converging and Diverging s AIR Converging If the surface is convex, it is a converging surface in the sense that the parallel rays bend toward each other after passing through the

More information

Image Formation and Camera Design

Image Formation and Camera Design Image Formation and Camera Design Spring 2003 CMSC 426 Jan Neumann 2/20/03 Light is all around us! From London & Upton, Photography Conventional camera design... Ken Kay, 1969 in Light & Film, TimeLife

More information

Performance Factors. Technical Assistance. Fundamental Optics

Performance Factors.   Technical Assistance. Fundamental Optics Performance Factors After paraxial formulas have been used to select values for component focal length(s) and diameter(s), the final step is to select actual lenses. As in any engineering problem, this

More information

30 Lenses. Lenses change the paths of light.

30 Lenses. Lenses change the paths of light. Lenses change the paths of light. A light ray bends as it enters glass and bends again as it leaves. Light passing through glass of a certain shape can form an image that appears larger, smaller, closer,

More information

VISUAL PHYSICS ONLINE DEPTH STUDY: ELECTRON MICROSCOPES

VISUAL PHYSICS ONLINE DEPTH STUDY: ELECTRON MICROSCOPES VISUAL PHYSICS ONLINE DEPTH STUDY: ELECTRON MICROSCOPES Shortly after the experimental confirmation of the wave properties of the electron, it was suggested that the electron could be used to examine objects

More information

Lecture 2 Camera Models

Lecture 2 Camera Models Lecture 2 Camera Models Professor Silvio Savarese Computational Vision and Geometr Lab Silvio Savarese Lecture 2-4-Jan-4 Announcements Prerequisites: an questions? This course requires knowledge of linear

More information

EE119 Introduction to Optical Engineering Spring 2002 Final Exam. Name:

EE119 Introduction to Optical Engineering Spring 2002 Final Exam. Name: EE119 Introduction to Optical Engineering Spring 2002 Final Exam Name: SID: CLOSED BOOK. FOUR 8 1/2 X 11 SHEETS OF NOTES, AND SCIENTIFIC POCKET CALCULATOR PERMITTED. TIME ALLOTTED: 180 MINUTES Fundamental

More information

Chapter 18 Optical Elements

Chapter 18 Optical Elements Chapter 18 Optical Elements GOALS When you have mastered the content of this chapter, you will be able to achieve the following goals: Definitions Define each of the following terms and use it in an operational

More information

Lecture 7: Camera Models

Lecture 7: Camera Models Lecture 7: Camera Models Professor Fei- Fei Li Stanford Vision Lab Lecture 7 -! 1 What we will learn toda? Pinhole cameras Cameras & lenses The geometr of pinhole cameras Reading: [FP] Chapters 1 3 [HZ]

More information

Exam Preparation Guide Geometrical optics (TN3313)

Exam 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 information

LENSES. a. To study the nature of image formed by spherical lenses. b. To study the defects of spherical lenses.

LENSES. a. To study the nature of image formed by spherical lenses. b. To study the defects of spherical lenses. Purpose Theory LENSES a. To study the nature of image formed by spherical lenses. b. To study the defects of spherical lenses. formation by thin spherical lenses s are formed by lenses because of the refraction

More information

Chapter 25. Optical Instruments

Chapter 25. Optical Instruments Chapter 25 Optical Instruments Optical Instruments Analysis generally involves the laws of reflection and refraction Analysis uses the procedures of geometric optics To explain certain phenomena, the wave

More information

Lecture 8. Lecture 8. r 1

Lecture 8. Lecture 8. r 1 Lecture 8 Achromat Design Design starts with desired Next choose your glass materials, i.e. Find P D P D, then get f D P D K K Choose radii (still some freedom left in choice of radii for minimization

More information

Image Formation. Dr. Gerhard Roth. COMP 4102A Winter 2015 Version 3

Image Formation. Dr. Gerhard Roth. COMP 4102A Winter 2015 Version 3 Image Formation Dr. Gerhard Roth COMP 4102A Winter 2015 Version 3 1 Image Formation Two type of images Intensity image encodes light intensities (passive sensor) Range (depth) image encodes shape and distance

More information

Chapter 29/30. Wave Fronts and Rays. Refraction of Sound. Dispersion in a Prism. Index of Refraction. Refraction and Lenses

Chapter 29/30. Wave Fronts and Rays. Refraction of Sound. Dispersion in a Prism. Index of Refraction. Refraction and Lenses Chapter 29/30 Refraction and Lenses Refraction Refraction the bending of waves as they pass from one medium into another. Caused by a change in the average speed of light. Analogy A car that drives off

More information

ECEN 4606, UNDERGRADUATE OPTICS LAB

ECEN 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 information

CS559: Computer Graphics. Lecture 2: Image Formation in Eyes and Cameras Li Zhang Spring 2008

CS559: Computer Graphics. Lecture 2: Image Formation in Eyes and Cameras Li Zhang Spring 2008 CS559: Computer Graphics Lecture 2: Image Formation in Eyes and Cameras Li Zhang Spring 2008 Today Eyes Cameras Light Why can we see? Visible Light and Beyond Infrared, e.g. radio wave longer wavelength

More information

Physics 11. Unit 8 Geometric Optics Part 2

Physics 11. Unit 8 Geometric Optics Part 2 Physics 11 Unit 8 Geometric Optics Part 2 (c) Refraction (i) Introduction: Snell s law Like water waves, when light is traveling from one medium to another, not only does its wavelength, and in turn the

More information

The Camera : Computational Photography Alexei Efros, CMU, Fall 2005

The Camera : Computational Photography Alexei Efros, CMU, Fall 2005 The Camera 15-463: Computational Photography Alexei Efros, CMU, Fall 2005 How do we see the world? object film Let s design a camera Idea 1: put a piece of film in front of an object Do we get a reasonable

More information

Computer Vision. The Pinhole Camera Model

Computer Vision. The Pinhole Camera Model Computer Vision The Pinhole Camera Model Filippo Bergamasco (filippo.bergamasco@unive.it) http://www.dais.unive.it/~bergamasco DAIS, Ca Foscari University of Venice Academic year 2017/2018 Imaging device

More information

Telecentric Imaging Object space telecentricity stop source: edmund optics The 5 classical Seidel Aberrations First order aberrations Spherical Aberration (~r 4 ) Origin: different focal lengths for different

More information

Lecture Outline Chapter 27. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

Lecture Outline Chapter 27. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc. Lecture Outline Chapter 27 Physics, 4 th Edition James S. Walker Chapter 27 Optical Instruments Units of Chapter 27 The Human Eye and the Camera Lenses in Combination and Corrective Optics The Magnifying

More information

Chapter 26. The Refraction of Light: Lenses and Optical Instruments

Chapter 26. The Refraction of Light: Lenses and Optical Instruments Chapter 26 The Refraction of Light: Lenses and Optical Instruments 26.1 The Index of Refraction Light travels through a vacuum at a speed c=3. 00 10 8 m/ s Light travels through materials at a speed less

More information

Mirrors and Lenses. Images can be formed by reflection from mirrors. Images can be formed by refraction through lenses.

Mirrors and Lenses. Images can be formed by reflection from mirrors. Images can be formed by refraction through lenses. Mirrors and Lenses Images can be formed by reflection from mirrors. Images can be formed by refraction through lenses. Notation for Mirrors and Lenses The object distance is the distance from the object

More information

Waves & Oscillations

Waves & Oscillations Physics 42200 Waves & Oscillations Lecture 27 Geometric Optics Spring 205 Semester Matthew Jones Sign Conventions > + = Convex surface: is positive for objects on the incident-light side is positive for

More information

Applications of Optics

Applications of Optics Nicholas J. Giordano www.cengage.com/physics/giordano Chapter 26 Applications of Optics Marilyn Akins, PhD Broome Community College Applications of Optics Many devices are based on the principles of optics

More information

Overview. Pinhole camera model Projective geometry Vanishing points and lines Projection matrix Cameras with Lenses Color Digital image

Overview. Pinhole camera model Projective geometry Vanishing points and lines Projection matrix Cameras with Lenses Color Digital image Camera & Color Overview Pinhole camera model Projective geometry Vanishing points and lines Projection matrix Cameras with Lenses Color Digital image Book: Hartley 6.1, Szeliski 2.1.5, 2.2, 2.3 The trip

More information

Lens Design I. Lecture 3: Properties of optical systems II Herbert Gross. Summer term

Lens 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 information

Two strategies for realistic rendering capture real world data synthesize from bottom up

Two strategies for realistic rendering capture real world data synthesize from bottom up Recap from Wednesday Two strategies for realistic rendering capture real world data synthesize from bottom up Both have existed for 500 years. Both are successful. Attempts to take the best of both world

More information

Geometric optics & aberrations

Geometric optics & aberrations Geometric optics & aberrations Department of Astrophysical Sciences University AST 542 http://www.northerneye.co.uk/ Outline Introduction: Optics in astronomy Basics of geometric optics Paraxial approximation

More information

25 cm. 60 cm. 50 cm. 40 cm.

25 cm. 60 cm. 50 cm. 40 cm. Geometrical Optics 7. The image formed by a plane mirror is: (a) Real. (b) Virtual. (c) Erect and of equal size. (d) Laterally inverted. (e) B, c, and d. (f) A, b and c. 8. A real image is that: (a) Which

More information

Phys 531 Lecture 9 30 September 2004 Ray Optics II. + 1 s i. = 1 f

Phys 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 information

BIOPHYSICS OF VISION GEOMETRIC OPTICS OF HUMAN EYE. Refraction media of the human eye. D eye = 63 diopter, D cornea =40, D lens = 15+

BIOPHYSICS OF VISION GEOMETRIC OPTICS OF HUMAN EYE. Refraction media of the human eye. D eye = 63 diopter, D cornea =40, D lens = 15+ BIOPHYSICS OF VISION THEORY OF COLOR VISION ELECTRORETINOGRAM Two problems: All cows are black in dark! Playing tennis in dark with illuminated lines, rackets, net, and ball! Refraction media of the human

More information

ME 297 L4-2 Optical design flow Analysis

ME 297 L4-2 Optical design flow Analysis ME 297 L4-2 Optical design flow Analysis Nayer Eradat Fall 2011 SJSU 1 Are we meeting the specs? First order requirements (after scaling the lens) Distortion Sharpness (diffraction MTF-will establish depth

More information

UNIVERSITY OF NAIROBI COLLEGE OF EDUCATION AND EXTERNAL STUDIES

UNIVERSITY OF NAIROBI COLLEGE OF EDUCATION AND EXTERNAL STUDIES UNIVERSITY OF NAIROBI COLLEGE OF EDUCATION AND EXTERNAL STUDIES COURSE TITLE: BED (SCIENCE) UNIT TITLE: WAVES AND OPTICS UNIT CODE: SPH 103 UNIT AUTHOR: PROF. R.O. GENGA DEPARTMENT OF PHYSICS UNIVERSITY

More information