A6525 Fall 2015 Solutions to Problem Set #2. This is the case of a single plano-convex lens. The specifications are:

Size: px
Start display at page:

Download "A6525 Fall 2015 Solutions to Problem Set #2. This is the case of a single plano-convex lens. The specifications are:"

Transcription

1 A655 Fall 05 Solutions to Problem Set # Problem : This is the case o a single plano-convex lens. The speciications are: Focal length ~ 5 cm Diameter D = 0 cm Index o reraction n =. Size o aperture stop s = 9 cm Thickness o lens t = cm a) From the lensmaker s equation = ( n ) r r with r, r = ( n ) Thus, r = -. 5 = 6.5 cm b) Do a system plot and spot diagram with ray trace program. BFD = 3.66 cm Figure -: Let is system plot o the p-c lens. On the right is a spot diagram. Full scale is cm. File is: pc with conic surace ( = 5).ray c) rms (on-axis) = 0.56 cm, rms ( deg. o-axis) = d) Vary eccentricity to minimize the rms spot size. Eccentricity =.0 rms (on-axis) = 0.0 cm Best case - see Figure - below. rms ( deg. o-axis) = 0.09 cm A PS-

2 PC with conic surace Sm_RMS EC_03 Figure -: Optimization plot o smallest rms vs. eccentricity o the curved surace o the plano-convex lens. Dierent symbols represent dierent distances o-axis (rom 0 to.0 degree). The best eccentricity is.. e) Show spot diagrams or the eccentricity optimized case. Figure -3: Spot diagram or p-c lens with e =.. The source is one degree o-axis. The on-axis case gives a perect image. The ull scale is 0.5 cm. A PS-

3 ) Do the same calculations or a convex plano-lens. Figure -4: Let is system plot o the c-p lens. On the right is a spot diagram. Full scale is 0.5 cm. File is: cp with conic surace ( = 5).ray rms (on-axis) = cm, rms ( deg. o-axis) = Vary eccentricity to minimize the rms spot size. Eccentricity =.09 rms (on-axis) = cm Best case - see Figure -5 below. rms ( deg. o-axis) = cm CP with conic surace 0.0 Sm_RMS EC_0 Figure -5: Optimization plot o smallest rms vs. eccentricity o the curved surace o A PS-3

4 the convex-plano lens. Dierent symbols represent dierent distances o-axis (rom 0 to.0 degree). The best eccentricity is.. Show spot diagrams or the eccentricity optimized case. Figure -6: Spot diagram or c-p lens with e =.09. The source is one degree o-axis. The onaxis case gives a near perect image. The ull scale is 0.05 cm. g) Which case is better? Clearly the C-P lens is better both with and w/o optimization. Table a summarizes the cases below. Table a: Summary o P-C/C-P comparison Case Eccentricity Rms spot size θ = 0 θ = P-C P-C C-P C-P A PS-4

5 Problem : A summary o results is given in Table a: Table a: Ray-trace results or double lens system First Lens Second Lens rms spot size Case r e r e r e r e θ = 0 θ = a Cases:. As designed rom two-lens, thin lens, and lensmakers equations.. Did a hand search starting with both eccentricities equal to Bent lenses to reduce spot size 4. Same as case 3 but optimized by varying eccentricity o suraces o second lens a. Did a grid search with variation window Details o the Solution: For a two lens system separated by a distance d, the object a distance o rom the irst (letmost) vertex and the image a distance i rom the rightmost vertex, we have i o d( + o) o o + ( d)( + o) + d d = = d d Where the irst limit is or the object at minus ininity and the second limit has the two ocal lengths set equal. We can solve the above equation or the ocal length, = i + d / + ( i + d / ) id The principal plane will be located at the stop because o the symmetry o the system so the ocal length,, o the doublet will be i+d/. Putting this into the above equation yields the ocal length o the individual lenses in terms o the total ocal length and lens separation. = + ( d / ) d Since d = cm and we want = 5 cm, = 9.04 cm. For a plano-convex lens the lensmakers equation simpliies r = ( n ) or the curved surace and so or n =., we have r = 3.9 cm. A PS-5

6 Case : I we used the back ocal distance, i = 5 cm instead o we get = 3.03 cm and r = 34.4 cm. As per the instructions in the problem, we will us these latter numbers. The results o a trace with 000 rays are given in Table a and spot diagrams or on-axis and one degree o-axis are shown below. The back ocal distance is 3.39 cm. Figure -: A diagram o the starting coniguration o the doublet system. Figure -: Spot diagrams or Case (lenses are plano-convex with spherical suraces). Let: On-axis, right: one degree o-axis. Full scale is 0.5 cm. A PS-6

7 Case : Using the variation window, we now search or a better spot size by varying the eccentricity o suraces and 4. The results are given in Table - (Case ). Note that there is a partial degeneracy between the two eccentricities. Spot diagrams are given in Figure -3. The spherical aberration is basically gone and residual coma is evident. Figure -3: Spot diagrams or Case (lenses are plano-convex with conic suraces). Let: On-axis, right: one degree o-axis. Full scale is 0. cm. Case 3: Now we try optimizing by bending the lenses (starting rom Case ). Initially the search was done with bending to two lenses (surace & together and surace 4 and 5 together) rom -0.4 to 0.4 (cm - ) about the nominal (Case ) values. The search space was then narrowed. The spot diagrams are shown in Figure -4 and the results rms spot sizes are list in Table -. A system plot is shown in Figure -5. Figure -4: Spot diagrams or Case 3 (lenses are bent with spherical suraces). Let: Onaxis, right: one degree o-axis. Full scale is 0.05 cm. A PS-7

8 Figure -5: Schematic o optical system ater bending lenses and to minimize the rms spot size (Case 4). Case 4: We now vary the eccentricity o the suraces o the second lens. This basically can be used to get rid o spherical aberration. Figure -6 shows the resulting spot diagrams. There is still residual coma in the system. There is also signiicant ield curvature and we have not worried about chromatic aberrations, so this system still has a ways to go. Note that the rms spot size or degree o-axis is about 0.9 arcminutes. Not great but much better than the original doublet. Figure -6: Spot diagrams or Case 4 (lenses are bent with conic suraces). The source is one degree o-axis. The on-axis case gives a near perect image. Full scale is 0.05 cm. A PS-8

9 0.8 Optimized doublet (bending & ecc <> 0) 0.6 EC_ EC_04 Figure -7: Optimization plot o smallest rms vs. eccentricity suraces 4 and 5 or Case 4. The smallest rms is e = 0.7 or surace 4 and e = 0.0 or surace 5. This optimization is done or an on-axis source. There is not much dierence or a source one degree oaxis. Ray-trace iles used: File pc with conic surace ( = 5).ray cp with conic surace ( = 5).ray Description Plano-convex lens with eccentricity optimization Same or convex-plano lens doublet (pc-cp, conics) ( = 5).ray Case, set ecc = 0 to get case doublet - optimized ( = 5).ray Case 4, set ecc = 0 to get case 3 A PS-9

11/13/2018. Lenses. Lenses. Light refracts at both surfaces. Non-parallel surfaces results in net bend.

11/13/2018. Lenses. Lenses. Light refracts at both surfaces. Non-parallel surfaces results in net bend. Light reracts at both suraces. Non-parallel suraces results in net bend. Focusing power o the lens is unction o radius o curvature o each surace and index o reraction o lens. Converging lenses are thicker

More information

Lenses & Prism Consider light entering a prism At the plane surface perpendicular light is unrefracted Moving from the glass to the slope side light

Lenses & Prism Consider light entering a prism At the plane surface perpendicular light is unrefracted Moving from the glass to the slope side light Lenses & Prism Consider light entering a prism At the plane surace perpendicular light is unreracted Moving rom the glass to the slope side light is bent away rom the normal o the slope Using Snell's law

More information

Outline F. OPTICS. Objectives. Introduction. Wavefronts. Light Rays. Geometrical Optics. Reflection and Refraction

Outline F. OPTICS. Objectives. Introduction. Wavefronts. Light Rays. Geometrical Optics. Reflection and Refraction F. OPTICS Outline 22. Spherical mirrors 22.2 Reraction at spherical suraces 22.3 Thin lenses 22. Geometrical optics Objectives (a) use the relationship = r/2 or spherical mirrors (b) draw ray agrams to

More information

Chapter 34: Geometrical Optics

Chapter 34: Geometrical Optics Chapter 34: Geometrical Optics Mirrors Plane Spherical (convex or concave) Lenses The lens equation Lensmaker s equation Combination of lenses E! Phys Phys 2435: 22: Chap. 34, 3, Pg Mirrors New Topic Phys

More information

Chapter 26 Geometrical Optics

Chapter 26 Geometrical Optics Chapter 26 Geometrical Optics 1 Overview of Chapter 26 The Reflection of Light Forming Images with a Plane Mirror Spherical Mirrors Ray Tracing and the Mirror Equation The Refraction of Light Ray Tracing

More information

Chapter 3: Mirrors and Lenses

Chapter 3: Mirrors and Lenses Chapter 3: Mirrors and Lenses Chapter 3: Mirrors and Lenses Lenses Refraction Converging rays Diverging rays Converging Lens Ray tracing rules Image formation Diverging Lens Ray tracing Image formation

More information

Ray Tracing II 2. Ray Tracing with Ray

Ray Tracing II 2. Ray Tracing with Ray Ray Tracing II Astronomy 6525 Lecture 3: Part 2 Ray Tracing with Ray Ray tracing with Ray Introduction to Ray Using the program Worked example HBO example Ray Tracing II 2 1 Starting ray Entering the prescription

More information

Lab 9 - GEOMETRICAL OPTICS

Lab 9 - GEOMETRICAL OPTICS 161 Name Date Partners Lab 9 - GEOMETRICAL OPTICS OBJECTIVES Optics, developed in us through study, teaches us to see - Paul Cezanne Image rom www.weidemyr.com To examine Snell s Law To observe total internal

More information

Algebra Based Physics

Algebra Based Physics Slide 1 / 66 Slide 2 / 66 Algebra Based Physics Geometric Optics 2015-12-01 www.njctl.org Table of ontents Slide 3 / 66 lick on the topic to go to that section Reflection Spherical Mirror Refraction and

More information

GEOMETRICAL OPTICS OBJECTIVES

GEOMETRICAL OPTICS OBJECTIVES Geometrical Optics 207 Name Date Partners OBJECTIVES OVERVIEW GEOMETRICAL OPTICS To examine Snell s Law and observe total internal relection. To understand and use the lens equations. To ind the ocal length

More information

Chapter 5: Light and Vision CHAPTER 5: LIGHT AND VISION

Chapter 5: Light and Vision CHAPTER 5: LIGHT AND VISION CHAPTER 5: LIGHT AND VISION These notes have been compiled in a way to make it easier or revision. The topics are not in order as per the syllabus. 5.1 Mirrors and Lenses 5.1.1 Image Characteristics Image

More information

PHYS 202 Notes, Week 9

PHYS 202 Notes, Week 9 PHYS 202 Notes, Week 9 Greg Christian March 22 & 24, 206 Last updated: 03/24/206 at 2:23:56 This week we learn about images by mirrors, refraction, and thin lenses. Images Spherical Mirrors First let s

More information

DEPARTMENT OF ELECTRICAL AND COMPUTER ENGINEERING NORTHEASTERN UNIVERSITY ECEU646/ECEG105 OPTICS FOR ENGINEERS FALL 2008.

DEPARTMENT OF ELECTRICAL AND COMPUTER ENGINEERING NORTHEASTERN UNIVERSITY ECEU646/ECEG105 OPTICS FOR ENGINEERS FALL 2008. DEPARTMENT OF ELECTRICAL AND COMPUTER ENGINEERING NORTHEASTERN UNIVERSITY ECEU646/ECEG105 OPTICS FOR ENGINEERS FALL 2008 Solutions This homework set includes problems for both ECEU646 and ECEG105. Problems

More information

Thin Lenses. Lecture 23. Chapter 34. Ray Optics. Physics II. Course website:

Thin Lenses. Lecture 23. Chapter 34. Ray Optics. Physics II. Course website: Lecture 23 Chapter 34 Physics II Ray Optics Thin Lenses Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsii Today we are going to discuss: Chapter 34: Section 34.5-6 Thin Lenses There

More information

Advanced Lens Design

Advanced Lens Design Advanced Lens Design Lecture : Introduction 3--5 Herbert Gross Winter term 3 www.iap.uni-jena.de Overview Time: Tuesday, 8.5 9.45 Location: PaPool, Helmholtweg 4 Web page on IAP homepage under learning/materials

More information

6. Lecture, 21 September 1999

6. Lecture, 21 September 1999 6. Lecture, 21 September 1999 6.1 Computer ray tracing RayTrace version 5.0 (by J.R. Houck and T.L. Herter, professors of astronomy at Cornell) is a computer program that traces rays through optical systems

More information

Physics 2C: Optics. refraction, Snell s law, polarization, images, thin mirrors, thin lenses July 11,

Physics 2C: Optics. refraction, Snell s law, polarization, images, thin mirrors, thin lenses July 11, Physics C: Optics Relection, reraction, Snell s law, polarization, images, thin mirrors, thin lenses July, 0 4 Relection: specularand diuse Size o objects a>>λ, treat waves as rays Light strikes medium,

More information

Light, Photons, and MRI

Light, Photons, and MRI Light, Photons, and MRI When light hits an object, some of it will be reflected. The reflected light can form an image. We usually want to be able to characterize the image given what we know about the

More information

Chapter 36. Image Formation

Chapter 36. Image Formation Chapter 36 Image Formation Apr 22, 2012 Light from distant things 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

More information

AP Physics: Curved Mirrors and Lenses

AP Physics: Curved Mirrors and Lenses The Ray Model of Light Light often travels in straight lines. We represent light using rays, which are straight lines emanating from an object. This is an idealization, but is very useful for geometric

More information

PHYSICS. Chapter 34 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT

PHYSICS. Chapter 34 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT PHYSICS FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E Chapter 34 Lecture RANDALL D. KNIGHT Chapter 34 Ray Optics IN THIS CHAPTER, you will learn about and apply the ray model of light Slide 34-2

More information

THIN LENSES: BASICS. There are at least three commonly used symbols for object and image distances:

THIN LENSES: BASICS. There are at least three commonly used symbols for object and image distances: THN LENSES: BASCS BJECTVE: To study and veriy some o the laws o optics applicable to thin lenses by determining the ocal lengths o three such lenses ( two convex, one concave) by several methods. THERY:

More information

Reflection and Refraction

Reflection and Refraction Relection and Reraction Object To determine ocal lengths o lenses and mirrors and to determine the index o reraction o glass. Apparatus Lenses, optical bench, mirrors, light source, screen, plastic or

More information

Ch. 26: Geometrical Optics

Ch. 26: Geometrical Optics Sec. 6-1: The Reflection of Light Wave Fronts and Rays Ch. 6: Geometrical Optics Wave front: a surface on which E is a maximum. Figure 5-3: Plane Wave *For this wave, the wave fronts are a series of planes.

More information

Reflection and Refraction. Geometrical Optics

Reflection and Refraction. Geometrical Optics Reflection and Refraction Geometrical Optics Reflection Angle of incidence = Angle of reflection The angle of incidence,i, is always equal to the angle of reflection, r. The incident ray, reflected ray

More information

Application note Fast focusing for machine vision applications With Optotune s focus tunable lens EL C

Application note Fast focusing for machine vision applications With Optotune s focus tunable lens EL C Application note Fast focusing for machine vision applications With Optotune s focus tunable lens EL-10-30-C Page 1 of 8 Introduction Flexible and fast focusing solutions with electrically tunable lenses

More information

OPTI-502 Midterm Exam John E. Greivenkamp Page 1/12 Fall, 2016

OPTI-502 Midterm Exam John E. Greivenkamp Page 1/12 Fall, 2016 Page 1/12 Fall, 2016 October 19, 2016 Lecture 17 Name SOLUTIONS Closed book; closed notes. Time limit: 75 minutes. An equation sheet is attached and can be removed. A spare raytrace sheet is also attached.

More information

LENSES DDC TECHNOLOGIES

LENSES DDC TECHNOLOGIES LENSES Optical Glass Plano-convex Lenses... 2 Optical Glass Plano-concave Lenses... 3 Optical Glass Bi-convex Lenses... 4 Optical Glass Bi-concave Lenses... 5 Fused Silica Plano-convex Lenses... 6 Fused

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 205-04-27 Herbert Gross Summer term 205 www.iap.uni-jena.de 2 Preliminary Schedule 3.04. Basics 2 20.04. Properties of optical systems I 3 27.05.

More information

Ray Optics. Physics 11. Sources of Light Rays: Self-Luminous Objects. The Ray Model of Light

Ray Optics. Physics 11. Sources of Light Rays: Self-Luminous Objects. The Ray Model of Light Physics 11 Ray Optics Ray Model of Light Reflection Plane Mirrors Spherical Mirrors Ray Tracing Images from a Concave Mirror Images from a Convex Mirror Slide 18-3 The Ray Model of Light Sources of Light

More information

Essential Physics I. Lecture 13:

Essential Physics I. Lecture 13: Essential Physics I E I Lecture 13: 11-07-16 Reminders No lecture: Monday 18th July (holiday) Essay due: Monday 25th July, 4:30 pm 2 weeks!! Exam: Monday 1st August, 4:30 pm Announcements 250 word essay

More information

Chapter 34. Images. Two Types of Images. A Common Mirage. Plane Mirrors, Extended Object. Plane Mirrors, Point Object

Chapter 34. Images. Two Types of Images. A Common Mirage. Plane Mirrors, Extended Object. Plane Mirrors, Point Object Capter Images One o te most important uses o te basic laws governing ligt is te production o images. Images are critical to a variety o ields and industries ranging rom entertainment, security, and medicine

More information

Section 3. Imaging With A Thin Lens

Section 3. Imaging With A Thin Lens Section 3 Imaging Wit A Tin Lens 3- at Ininity An object at ininity produces a set o collimated set o rays entering te optical system. Consider te rays rom a inite object located on te axis. Wen te object

More information

References Photography, B. London and J. Upton Optics in Photography, R. Kingslake The Camera, The Negative, The Print, A. Adams

References Photography, B. London and J. Upton Optics in Photography, R. Kingslake The Camera, The Negative, The Print, A. Adams Page 1 Camera Simulation Eect Cause Field o view Depth o ield Motion blur Exposure Film size, stops and pupils Aperture, ocal length Shutter Film speed, aperture, shutter Reerences Photography, B. London

More information

EE119 Homework 3. Due Monday, February 16, 2009

EE119 Homework 3. Due Monday, February 16, 2009 EE9 Homework 3 Professor: Jeff Bokor GSI: Julia Zaks Due Monday, February 6, 2009. In class we have discussed that the behavior of an optical system changes when immersed in a liquid. Show that the longitudinal

More information

The Law of Reflection

The Law of Reflection If the surface off which the light is reflected is smooth, then the light undergoes specular reflection (parallel rays will all be reflected in the same directions). If, on the other hand, the surface

More information

Optics Course (Phys 311) Geometrical Optics Refraction through Lenses

Optics Course (Phys 311) Geometrical Optics Refraction through Lenses Optics Course (Phys ) Geometrical Optics Refraction through Lenses Lecturer: Dr Zeina Hashim Slide 1 Objectives covered in this lesson : 1. Refraction through single spherical refracting surfaces. 2. Lenses:

More information

LIGHT & OPTICS. Fundamentals of Physics 2112 Chapter 34 1

LIGHT & OPTICS. Fundamentals of Physics 2112 Chapter 34 1 LIGHT & OPTICS Fundamentals of Physics 22 Chapter 34 Chapter 34 Images. Two Types of Images 2. Plane Mirrors 3. Spherical Mirrors 4. Images from Spherical Mirrors 5. Spherical Refracting Surfaces 6. Thin

More information

Lecture Outline Chapter 26. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

Lecture Outline Chapter 26. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc. Lecture Outline Chapter 26 Physics, 4 th Edition James S. Walker Chapter 26 Geometrical Optics Units of Chapter 26 The Reflection of Light Forming Images with a Plane Mirror Spherical Mirrors Ray Tracing

More information

L ENSES. Lenses Spherical refracting surfaces. n 1 n 2

L ENSES. Lenses Spherical refracting surfaces. n 1 n 2 Lenses 2 L ENSES 2. Sherical reracting suraces In order to start discussing lenses uantitatively, it is useul to consider a simle sherical surace, as shown in Fig. 2.. Our lens is a semi-ininte rod with

More information

OPTI 201R Homework 9 Solutions

OPTI 201R Homework 9 Solutions OPTI 20R Homework 9 Solutions. Unknown thick lens system measured with reciprocal magnification technique. At the first position where the object is sharply focused on the image plane m = 2. The lens needs

More information

Light: Geometric Optics (Chapter 23)

Light: Geometric Optics (Chapter 23) Light: Geometric Optics (Chapter 23) Units of Chapter 23 The Ray Model of Light Reflection; Image Formed by a Plane Mirror Formation of Images by Spherical Index of Refraction Refraction: Snell s Law 1

More information

Reflections. I feel pretty, oh so pretty

Reflections. I feel pretty, oh so pretty Reflections I feel pretty, oh so pretty Objectives By the end of the lesson, you should be able to: Draw an accurate reflective angle Determine the focal length of a spherical mirror Light Review Light

More information

DESIGNING A SIMPLE OPTICAL SYSTEM IN LIGHTTOOLS

DESIGNING A SIMPLE OPTICAL SYSTEM IN LIGHTTOOLS DESIGNING A SIMPLE OPTICAL SYSTEM IN LIGHTTOOLS Liliana Ruiz Diaz December 08, 2016 College of Optical Sciences, University of Arizona, Tucson, AZ USA 85721 WHAT IS LIGHTTOOLS LightTools is a 3D optical

More information

Physics 1C Lecture 26A. Beginning of Chapter 26

Physics 1C Lecture 26A. Beginning of Chapter 26 Physics 1C Lecture 26A Beginning of Chapter 26 Mirrors and Lenses! As we have noted before, light rays can be diverted by optical systems to fool your eye into thinking an object is somewhere that it is

More information

Lens Conventions From Jenkins & White: Fundamentals of Optics, pg 50 Incident rays travel left to right Object distance s + if left to vertex, - if

Lens Conventions From Jenkins & White: Fundamentals of Optics, pg 50 Incident rays travel left to right Object distance s + if left to vertex, - if Len Convention From Jenkin & White: Fundamental o Optic, pg 50 Incident ray travel let to right Object ditance + i let to vertex, - i right to vertex Image ditance ' + i right to vertex, - i let to vertex

More information

3. LENSES & PRISM

3. LENSES & PRISM 3. LENSES & PRISM. A transparent substance bounded by two surfaces of definite geometrical shape is called lens.. A lens may be considered to be made up of a number of small prisms put together. 3. Principal

More information

Chapter 23. Geometrical Optics (lecture 1: mirrors) Dr. Armen Kocharian

Chapter 23. Geometrical Optics (lecture 1: mirrors) Dr. Armen Kocharian Chapter 23 Geometrical Optics (lecture 1: mirrors) Dr. Armen Kocharian Reflection and Refraction at a Plane Surface The light radiate from a point object in all directions The light reflected from a plane

More information

Lens Design I. Lecture 4: Properties of optical systems III Herbert Gross. Summer term

Lens Design I. Lecture 4: Properties of optical systems III Herbert Gross. Summer term Lens Design I Lecture 4: Properties of optical systems III 018-05-03 Herbert Gross Summer term 018 www.iap.uni-jena.de Preliminary Schedule - Lens Design I 018 1 1.04. Basics 19.04. Properties of optical

More information

Lenses lens equation (for a thin lens) = (η η ) f r 1 r 2

Lenses lens equation (for a thin lens) = (η η ) f r 1 r 2 Lenses lens equation (for a thin lens) 1 1 1 ---- = (η η ) ------ - ------ f r 1 r 2 Where object o f = focal length η = refractive index of lens material η = refractive index of adjacent material r 1

More information

LECTURE 17 MIRRORS AND THIN LENS EQUATION. Instructor: Kazumi Tolich

LECTURE 17 MIRRORS AND THIN LENS EQUATION. Instructor: Kazumi Tolich LECTURE 17 MIRRORS AND THIN LENS EQUATION Instructor: Kazumi Tolich Lecture 17 2 18.6 Image formation with spherical mirrors Concave mirrors Convex mirrors 18.7 The thin-lens equation Sign conventions

More information

OPTI-502 Optical Design and Instrumentation I John E. Greivenkamp Final Exam In Class Page 1/12 Fall, 2017

OPTI-502 Optical Design and Instrumentation I John E. Greivenkamp Final Exam In Class Page 1/12 Fall, 2017 Final Exam In Class Page / Fall, 07 Name SOLUTIONS Closed book; closed notes. Time limit: 0 minutes. An equation sheet is attached and can be removed. Spare raytrace sheets are attached. Use the back sides

More information

Lens Conventions From Jenkins & White: Fundamentals of Optics, pg 50 Incident rays travel left to right Object distance s + if left to vertex, - if

Lens Conventions From Jenkins & White: Fundamentals of Optics, pg 50 Incident rays travel left to right Object distance s + if left to vertex, - if Len Convention From Jenkin & White: Fundamental o Optic, pg 50 Incident ray travel let to right Object ditance + i let to vertex, - i right to vertex Image ditance ' + i right to vertex, - i let to vertex

More information

Chapter 33 Continued Properties of Light. Law of Reflection Law of Refraction or Snell s Law Chromatic Dispersion Brewsters Angle

Chapter 33 Continued Properties of Light. Law of Reflection Law of Refraction or Snell s Law Chromatic Dispersion Brewsters Angle Chapter 33 Continued Properties of Light Law of Reflection Law of Refraction or Snell s Law Chromatic Dispersion Brewsters Angle Dispersion: Different wavelengths have different velocities and therefore

More information

Chapter 23. Light Geometric Optics

Chapter 23. Light Geometric Optics Chapter 23. Light Geometric Optics There are 3 basic ways to gather light and focus it to make an image. Pinhole - Simple geometry Mirror - Reflection Lens - Refraction Pinhole Camera Image Formation (the

More information

34.2: Two Types of Image

34.2: Two Types of Image Chapter 34 Images 34.2: Two Types of Image For you to see an object, your eye intercepts some of the light rays spreading from the object and then redirect them onto the retina at the rear of the eye.

More information

2/26/2016. Chapter 23 Ray Optics. Chapter 23 Preview. Chapter 23 Preview

2/26/2016. Chapter 23 Ray Optics. Chapter 23 Preview. Chapter 23 Preview Chapter 23 Ray Optics Chapter Goal: To understand and apply the ray model of light. Slide 23-2 Chapter 23 Preview Slide 23-3 Chapter 23 Preview Slide 23-4 1 Chapter 23 Preview Slide 23-5 Chapter 23 Preview

More information

Outline The Refraction of Light Forming Images with a Plane Mirror 26-3 Spherical Mirror 26-4 Ray Tracing and the Mirror Equation

Outline The Refraction of Light Forming Images with a Plane Mirror 26-3 Spherical Mirror 26-4 Ray Tracing and the Mirror Equation Chapter 6 Geometrical Optics Outline 6-1 The Reflection of Light 6- Forming Images with a Plane Mirror 6-3 Spherical Mirror 6-4 Ray Tracing and the Mirror Equation 6-5 The Refraction of Light 6-6 Ray Tracing

More information

Contrast Optimization: A faster and better technique for optimizing on MTF ABSTRACT Keywords: INTRODUCTION THEORY

Contrast Optimization: A faster and better technique for optimizing on MTF ABSTRACT Keywords: INTRODUCTION THEORY Contrast Optimization: A faster and better technique for optimizing on MTF Ken Moore, Erin Elliott, Mark Nicholson, Chris Normanshire, Shawn Gay, Jade Aiona Zemax, LLC ABSTRACT Our new Contrast Optimization

More information

Welcome to: Physics I. I m Dr Alex Pettitt, and I ll be your guide!

Welcome to: Physics I. I m Dr Alex Pettitt, and I ll be your guide! Welcome to: Physics I I m Dr Alex Pettitt, and I ll be your guide! Physics I: x Mirrors and lenses Lecture 13: 6-11-2018 Last lecture: Reflection & Refraction Reflection: Light ray hits surface Ray moves

More information

Refraction of Light. This bending of the ray is called refraction

Refraction of Light. This bending of the ray is called refraction Refraction & Lenses Refraction of Light When a ray of light traveling through a transparent medium encounters a boundary leading into another transparent medium, part of the ray is reflected and part of

More information

Optics Course (Phys 311) Geometrical Optics Refraction through Lenses

Optics Course (Phys 311) Geometrical Optics Refraction through Lenses Optics Course (Phys ) Geometrical Optics Refraction through Lenses Lecturer: Dr Zeina Hashim Slide 1 Objectives covered in this lesson : 1. The refracting power of a thin lens. 2. Thin lens combinations.

More information

Refractive Optical Design Systems Any lens system is a tradeoff of many factors Add optical elements (lens/mirrors) to balance these Many different

Refractive Optical Design Systems Any lens system is a tradeoff of many factors Add optical elements (lens/mirrors) to balance these Many different Refractive Optical Design Systems Any lens system is a tradeoff of many factors Add optical elements (lens/mirrors) to balance these Many different types of lens systems used Want to look at each from

More information

Light & Optical Systems Reflection & Refraction. Notes

Light & Optical Systems Reflection & Refraction. Notes Light & Optical Systems Reflection & Refraction Notes What is light? Light is electromagnetic radiation Ultra-violet + visible + infra-red Behavior of Light Light behaves in 2 ways particles (photons)

More information

Refractive Optical Design Systems Any lens system is a tradeoff of many factors Add optical elements (lens/mirrors) to balance these Many different

Refractive Optical Design Systems Any lens system is a tradeoff of many factors Add optical elements (lens/mirrors) to balance these Many different Refractive Optical Design Systems Any lens system is a tradeoff of many factors Add optical elements (lens/mirrors) to balance these Many different types of lens systems used Want to look at each from

More information

Snell s Law n i sin! i = n r sin! r

Snell s Law n i sin! i = n r sin! r Mr. Rawson Physics Snell s Law n i sin! i = n r sin! r Angle o Reraction n glass = 1.5 Angle o Incidence n air = 1.00 32 o 32 o 1 Mr. Rawson Physics 4 Mr. Rawson Physics 2 Mr. Rawson Physics 3 !"#$%&&&&

More information

2.3 Additional Relations

2.3 Additional Relations 3 2.3 Additional Relations Figure 2.3 identiies additional relations, indicating te locations o te object and image, and te ratio o teir eigts (magniication) and orientations. Ray enters te lens parallel

More information

Figure 1 - Refraction

Figure 1 - Refraction Geometrical optics Introduction Refraction When light crosses the interface between two media having different refractive indices (e.g. between water and air) a light ray will appear to change its direction

More information

Unit 11 Light and Optics Holt Chapter 14 Student Outline Light and Refraction

Unit 11 Light and Optics Holt Chapter 14 Student Outline Light and Refraction Holt Chapter 14 Student Outline Light and Refraction Variables introduced or used in chapter: Quantity Symbol Units Speed of light frequency wavelength angle Object Distance Image Distance Radius of Curvature

More information

Exercise 12 Geometrical and Technical Optics WS 2013/2014

Exercise 12 Geometrical and Technical Optics WS 2013/2014 Exercise 12 Geometrical and Technical Optics WS 213/214 Slide projector and Köhler illumination In this exercise a simplified slide projector (or LCD projector) will be designed and simulated with ray

More information

Lecture PowerPoint. Chapter 25 Physics: Principles with Applications, 6 th edition Giancoli

Lecture PowerPoint. Chapter 25 Physics: Principles with Applications, 6 th edition Giancoli Lecture PowerPoint Chapter 25 Physics: Principles with Applications, 6 th edition Giancoli 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the

More information

Lec. 7: Ch. 2 - Geometrical Optics. 1. Shadows 2. Reflection 3. Refraction 4. Dispersion. 5. Mirages, sun dogs, etc.

Lec. 7: Ch. 2 - Geometrical Optics. 1. Shadows 2. Reflection 3. Refraction 4. Dispersion. 5. Mirages, sun dogs, etc. Lec. 7: h. 2 - Geometrical Optics We are here 1. Shadows 2. Reflection 3. Refraction 4. Dispersion We only covered the first 44 vugraphs. 5. Mirages, sun dogs, etc. Read hapter 3, skip 3.3 and skip 3.5D

More information

Lasers PH 645/ OSE 645/ EE 613 Summer 2010 Section 1: T/Th 2:45-4:45 PM Engineering Building 240

Lasers PH 645/ OSE 645/ EE 613 Summer 2010 Section 1: T/Th 2:45-4:45 PM Engineering Building 240 Lasers PH 645/ OSE 645/ EE 613 Summer 2010 Section 1: T/Th 2:45-4:45 PM Engineering Building 240 John D. Williams, Ph.D. Department of Electrical and Computer Engineering 406 Optics Building - UAHuntsville,

More information

Part Images Formed by Flat Mirrors. This Chapter. Phys. 281B Geometric Optics. Chapter 2 : Image Formation. Chapter 2: Image Formation

Part Images Formed by Flat Mirrors. This Chapter. Phys. 281B Geometric Optics. Chapter 2 : Image Formation. Chapter 2: Image Formation Phys. 281B Geometric Optics This Chapter 3 Physics Department Yarmouk University 21163 Irbid Jordan 1- Images Formed by Flat Mirrors 2- Images Formed by Spherical Mirrors 3- Images Formed by Refraction

More information

Homework Set 3 Due Thursday, 07/14

Homework Set 3 Due Thursday, 07/14 Homework Set 3 Due Thursday, 07/14 Problem 1 A room contains two parallel wall mirrors, on opposite walls 5 meters apart. The mirrors are 8 meters long. Suppose that one person stands in a doorway, in

More information

Final Exam. Today s Review of Optics Polarization Reflection and transmission Linear and circular polarization Stokes parameters/jones calculus

Final Exam. Today s Review of Optics Polarization Reflection and transmission Linear and circular polarization Stokes parameters/jones calculus Physics 42200 Waves & Oscillations Lecture 40 Review Spring 206 Semester Matthew Jones Final Exam Date:Tuesday, May 3 th Time:7:00 to 9:00 pm Room: Phys 2 You can bring one double-sided pages of notes/formulas.

More information

Review Session 1. Dr. Flera Rizatdinova

Review Session 1. Dr. Flera Rizatdinova Review Session 1 Dr. Flera Rizatdinova Summary of Chapter 23 Index of refraction: Angle of reflection equals angle of incidence Plane mirror: image is virtual, upright, and the same size as the object

More information

Physics 11 Chapter 18: Ray Optics

Physics 11 Chapter 18: Ray Optics Physics 11 Chapter 18: Ray Optics "... Everything can be taken from a man but one thing; the last of the human freedoms to choose one s attitude in any given set of circumstances, to choose one s own way.

More information

SIMG Solution Set #6

SIMG Solution Set #6 SIMG-0-200 Solution Set #6. An optical system consists of thin lenses L (f 00mm)andL 2 (f 2 200mm) separated by d 800mm. Locate and describe the image of an object that is 50 mm high located 50 mm in front

More information

LECTURE 25 Spherical Refracting Surfaces. Geometric Optics

LECTURE 25 Spherical Refracting Surfaces. Geometric Optics LECTURE 25 Spherical Refracting Surfaces Geometric ptics When length scales are >> than the light s wavelength, light propagates as rays incident ray reflected ray θ θ r θ 2 refracted ray Reflection: Refraction:

More information

Light: Geometric Optics

Light: Geometric Optics Light: Geometric Optics 23.1 The Ray Model of Light Light very often travels in straight lines. We represent light using rays, which are straight lines emanating from an object. This is an idealization,

More information

Waves & Oscillations

Waves & Oscillations Physics 42200 Waves & Oscillations Lecture 40 Review Spring 2016 Semester Matthew Jones Final Exam Date:Tuesday, May 3 th Time:7:00 to 9:00 pm Room: Phys 112 You can bring one double-sided pages of notes/formulas.

More information

Chapter 34. Images. In this chapter we define and classify images, and then classify several basic ways in which they can be produced.

Chapter 34. Images. In this chapter we define and classify images, and then classify several basic ways in which they can be produced. Chapter 34 Images One of the most important uses of the basic laws governing light is the production of images. Images are critical to a variety of fields and industries ranging from entertainment, security,

More information

Chapter 23. Images and Mirrors 3/23/11. Mirrors and Lenses QUESTIONS? PLEASE ASK! Types of Images for Mirrors and Lenses.

Chapter 23. Images and Mirrors 3/23/11. Mirrors and Lenses QUESTIONS? PLEASE ASK! Types of Images for Mirrors and Lenses. 3/23/ LIGO mirror Announcements LIGO mirror Two exams down, one to go! No HW this week. Credit: LIGO Laboratory, Caltech Office hours: My office hours today from 2-3 pm (or make an appointment) Chapter

More information

Experiment 7 Geometric Optics

Experiment 7 Geometric Optics Physics 263 Experiment 7 Geometric Optics In this laboratory, we will perform several experiments on geometric optics. A pictorial diagram of the various components to be used is shown in Figure 5. 1 Refraction

More information

Thick Lenses and the ABCD Formalism

Thick Lenses and the ABCD Formalism Thick Lenses and the ABCD Formalism Thursday, 10/12/2006 Physics 158 Peter Beyersdorf Document info 12. 1 Class Outline Properties of Thick Lenses Paraxial Ray Matrices General Imaging Systems 12. 2 Thick

More information

Chapter 26 Geometrical Optics

Chapter 26 Geometrical Optics Chapter 26 Geometrical Optics The Reflection of Light: Mirrors: Mirrors produce images because the light that strikes them is reflected, rather than absorbed. Reflected light does much more than produce

More information

AP* Optics Free Response Questions

AP* Optics Free Response Questions AP* Optics Free Response Questions 1978 Q5 MIRRORS An object 6 centimeters high is placed 30 centimeters from a concave mirror of focal length 10 centimeters as shown above. (a) On the diagram above, locate

More information

Reflection and Refraction

Reflection and Refraction Reflection and Refraction Theory: Whenever a wave traveling in some medium encounters an interface or boundary with another medium either (or both) of the processes of (1) reflection and (2) refraction

More information

Contents. Ray Intersection Patterns Spherical Coma Field Curvature and astigmatism Distortion Aplanatic Points How to reduce aberrations

Contents. Ray Intersection Patterns Spherical Coma Field Curvature and astigmatism Distortion Aplanatic Points How to reduce aberrations Contents Ray Intersection Patterns Spherical Coma Field Curvature and astigmatism Distortion Aplanatic Points How to reduce aberrations ECE 4616 Tolis Deslis Contents Contents Ray Intersection Patterns

More information

Waves & Oscillations

Waves & Oscillations Physics 42200 Waves & Oscillations Lecture 41 Review Spring 2013 Semester Matthew Jones Final Exam Date:Tuesday, April 30 th Time:1:00 to 3:00 pm Room: Phys 112 You can bring two double-sided pages of

More information

arxiv: v1 [physics.class-ph] 11 Feb 2012

arxiv: v1 [physics.class-ph] 11 Feb 2012 arxiv:202.2404v [physics.class-ph] Feb 202 Refractive index of a transparent liquid measured with a concave mirror Introduction Amitabh Joshi and Juan D Serna 2 Department of Physics, Eastern Illinois

More information

Geometry of image formation

Geometry of image formation Geometry of image formation discussing here... mirrors definition of mirror types of mirrors aspects of plane mirror aspects of curved mirrors what is mirror? glass sheet with silvery / metallic coating

More information

Optics. a- Before the beginning of the nineteenth century, light was considered to be a stream of particles.

Optics. a- Before the beginning of the nineteenth century, light was considered to be a stream of particles. Optics 1- Light Nature: a- Before the beginning of the nineteenth century, light was considered to be a stream of particles. The particles were either emitted by the object being viewed or emanated from

More information

Chapter 26 Geometrical Optics

Chapter 26 Geometrical Optics Chapter 26 Geometrical Optics 26.1 The Reflection of Light 26.2 Forming Images With a Plane Mirror 26.3 Spherical Mirrors 26.4 Ray Tracing and the Mirror Equation 26.5 The Refraction of Light 26.6 Ray

More information

Optics and Images. Lenses and Mirrors. Matthew W. Milligan

Optics and Images. Lenses and Mirrors. Matthew W. Milligan Optics and Images Lenses and Mirrors Light: Interference and Optics I. Light as a Wave - wave basics review - electromagnetic radiation II. Diffraction and Interference - diffraction, Huygen s principle

More information

Physics 1C. Lecture 23A. "If Dracula can t see his reflection in the mirror, how come his hair is always so neatly combed?

Physics 1C. Lecture 23A. If Dracula can t see his reflection in the mirror, how come his hair is always so neatly combed? Physics 1C Lecture 23A "If Dracula can t see his reflection in the mirror, how come his hair is always so neatly combed?" --Steven Wright Mirror Equation You can mathematically relate the object distance,

More information

Physics 9 Wednesday, February 17, 2016

Physics 9 Wednesday, February 17, 2016 Physics 9 Wednesday, February 7, 206 On Wednesday, I will be out of town. Zoey Davidson will be here, in my place, to work some mirror and lens examples with you, probably on worksheets: try ray-tracing;

More information

Lecture Notes (Geometric Optics)

Lecture Notes (Geometric Optics) Lecture Notes (Geometric Optics) Intro: - plane mirrors are flat, smooth surfaces from which light is reflected by regular reflection - light rays are reflected with equal angles of incidence and reflection

More information

General Physics II. Mirrors & Lenses

General Physics II. Mirrors & Lenses General Physics II Mirrors & Lenses Nothing New! For the next several lectures we will be studying geometrical optics. You already know the fundamentals of what is going on!!! Reflection: θ 1 = θ r incident

More information