Image Formation Principle

Save this PDF as:

Size: px
Start display at page:

Transcription

1 Image Formation Principle Michael Biddle Robert Dawson Department of Physics and Astronomy The University of Georgia, Athens, Georgia (Dated: December 8, 2015) The aim of this project was to demonstrate the image formation principle. Image formation occurs when an object is viewed or projected through a lens, and the principles describing how this happens are encapsulated in the Thin Lens, Magnification, and Lens Maker s equations. A custom instrument was built to hold a lens, object, and camera in order to obtain a final image height created by this system. A lens was also imaged from a side view to determine the radius of curvature and verify the Lens Maker s equation. Data gathered using both a converging and diverging lens was analyzed using derived relationships, and found to match the predicted values very well. The experimenters therefore demonstrate the efficacy of aforementioned equations in describing image formation. π I. PHYSICS If you place some kind of non-refractive, transparent sheet in front of an object, the image appears to be the exact same size (and located in the exact same place) as the original object. However, when a lens is placed in front of an object, the observed image is altered. If a converging (or diverging) lens is placed in front of an object, the image may appear inverted as well as larger or smaller (or consequently seem farther away) than the actual object. This effect is known as the image formation principle of a lens. Three equations that are important to this principle are presented below. M 1 + (1) (2) (3) Eq. (1) is the Lens Equation. It relates the focal length of a lens (π) to the distance of the object from the lens (do) and the distance of the formed image from the lens (di). Eq. (2) is the Magnification Equation. It states that the magnification of a lens (for a certain object distance) can be described in terms of the object and image heights as well as the object and image distances. The idea for this comes from the same method used to relate triangles of similar shapes. The equation is simply the ratio of the side lengths of triangles drawn from the lens to the image and object. This formula can also be applied to a system of lenses, which we will make use of later in our experiment. For a system of two lenses, the total magnification, π, is, β β π π (4) β β π π where image and object heights and distances for the second lens are denoted with a prime. However, in Eq. (4) β ππ  equal to β, and π can be re-written in terms of S (the distance between our lenses) and π. Eq. (3) is the Lens Maker s Equation. This equation shows how the focal length of a lens can be described in terms of its index of refraction (as well as the index of refraction of the outside medium), the radius of curvature of the outside radius of the lens, and the radius of curvature of the inside radius of the lens. An image can be classified as either real or virtual. A real image can be projected onto a screen, because the image is formed by intersecting light rays that have passed through the lens. A virtual image, however, cannot be projected onto a screen. This is because a virtual image is not directly formed from light rays intersecting, but rather by tracing back the path of the formed rays to a point where they would intersect, as can be seen in FIG. 1. FIG. 1: A diverging lens bends light rays so that they do not intersect, but appear to have a common source. FIG. 2: A converging lens bends light rays so that they intersect to form a real image.

2 II. INSTRUMENT DESIGN We designed our instrument to be able to hold an object, a lens, and a phone to allow us to study the image formation of a lens. Our instrument consists of a long, narrow track of Lego bricks with a Lego lens holder (for use with either a diverging or converging lens, both made from BK7 glass) in its center. The instrument is also designed to allow us to accurately take certain measurements by using Lego studs as a reference; the half Lego stud is defined as 4 mm (see Section III). Our instrument was split into four components: the object side, the measurement side, the lens holder, and the phone holder. The object side was measured to be 72 half Lego studs long, the lens holder to be 4 half Lego studs long, the measurement side to be 62 half Lego studs long, and the spacing in the phone holder to be 1.5 Lego studs long. The total dimensions of our instrument measured to be: Base structure: 144x34 half Lego studs (576x136 mm) Object Side: 72x4 half Lego studs (288x16 mm) Measurement Side: 62x4 half Lego studs (248x16 mm) Lens Holder: 4x8 half Lego studs (16x32 mm) Phone Holder: 8x10 half Lego studs (32x40 mm) with a ~1.5 half Lego stud space (~6 mm) to hold the cell phone The lenses, purchased from Thorlabs, are made of BK-7 glass with an index of refraction of and a focal length of +/- 50mm (positive for the converging lens and negative for the diverging lens). The total cost of our instrument was \$ FIG. 3: Our experimental instrument. The object side is highlighted in red, the measurement side in yellow, the lens holder in blue, and the phone holder in green. FIG. 4: In this figure you can see the phone holder propping up a cell phone for imaging purposes, and the lens in the lens holder. FIG. 5: The ray diagram for a system of two converging lenses (above) and the ray diagram for a system of one diverging and one converging lens (below). III. CALIBRATION For our experiments, we need to be able to relate measurements from our phone (in pixels) to measurements in the real world (in millimeters). This proved challenging; instead we found a way to directly relate our data on the phone to measurements in the real world without having to convert pixels to millimeters and without having to use some object of known dimensions as a reference. To do this, we examined ratios of our data. We also need to be able to account for the fact that our phone is also an imaging device and part of our system. For this we need the focal length of the lens in an iphone 5s, which we looked up and found to be 4.12 mm. This will all be covered further in the data analysis section. Finally, we defined a half Lego stud (or just half stud) as the distance from the edge of a Lego block to the center of the first stud, a length of 4 mm. This allowed us to record several important measurements with respect to Lego studs and later convert these values to millimeters. This method

3 is an increase in precision over using a ruler and helps to reduce error. IV. EXPERIMENTAL PROCEDURE To test the Lens and Magnification equations for a converging and diverging lens, we first placed our lens in the lens holder and a small red Lego brick on the object side, 55 half studs (220 mm) from the lens. Then we placed our cellphone in the phone holder such that that the phone s camera was lined up with the lens and object. We took pictures at object distance increments of 4 half studs (16 mm). We defined our object as the space between two studs on our brick. For the case of the Lens Maker s Equation, we captured a profile view of our converging lens on camera. However, due to the shape of the diverging lens and a lack of materials, we were unable to complete this procedure for the diverging lens. FIG. 6: A model using Eq. (6) for our converging lens. The data appears to follow an inverse of the model we predicted. V. DATA ANALYSIS The data analysis for this lab appears to be very straight forward (and for the Lens Maker s Equation, it actually is), but proved to be trickier than one might initially imagine. Image heights are determined by gradually slicing pixels from the raw image, until the two studs surrounding our object are just outside the range. This range of pixels is what we use for the image height. To begin with, we considered modeling the image heights found on the camera versus an equation found from combing Eq. (1) and Eq. (2). The resulting model was: h (5) However, our current setup does not allow us to relate the size of the image on the screen (which is in pixels) to millimeters, rendering this equation effectively useless. Instead, we came up with a clever trick to get around this. We measured how changing the object distance would affect the image height measured by the camera: we took ratios of image heights obtained at different object distances. From Eq. (5), we derive: h d f h d f (6) where the prime symbol represents the height or object distance for an image that was measured one object distance increment from the previous image. By analyzing this ratio rather than the actual image height, we were able to simultaneously test the Lens and Magnification equations without having to relate the size of our image on the phone to millimeters. FIG. 7: A model using Eq. (6) for our diverging lens. The data appears to follow an inverse of the model we predicted. Unfortunately, the data we collected does not fit our model. We realized that Eq. (6) was modeled after a single lens experiment, and this is not the actual experiment we conducted. By including our phone in the experiment, there is a second lens in the system that must be accounted for. The image captured with the camera is not the same image produced by the first lens. In fact, one might notice that the data we collected somewhat mirrors our predicted model (this would actually make sense because, shown in FIG. 6, the phone s camera inverts the image we originally collected). But overall our results from the previous attempt are ineffective in demonstrating anything. To account for the cell phone s camera, we will once again combine Eq. (1) and Eq. (2) in some fashion so as to find the height of our image in terms of the focal length of our lens, the focal length of our camera lens, the original

4 object distance, and distance between the lens and the camera. We will once again take ratios of this equation to avoid conflicting units. We can modify Eq. (4) to simplify it further, using the fact that β β and π + π π , where s is the spacing between the lens and our camera: M β (s π ) π (7) β π π It is important to note that in the above and following expression, primed quantities do not represent a new trial (object distance), but rather are quantities with regard to the camera lens. This notation will also be used to differentiate focal lengths. Once again we will combine Eq. (1), Eq. (2), and Eq. (7) to find the height of the image on our camera in terms of the focal length of our lens, camera lens, object distance, object height, and spacing between our lens and camera. Substitutions and subsequent algebra yield a less than elegant expression: π π π π β π β π π π  π π π (8) π Therefore if the Lens and Magnification equations are true, we should be able to relate the ratio of image heights captured by our camera to the ratio of this equation for one object distance to another. And in fact by using Eq. (8) to generate models for converging and diverging lenses we notice that our new models fit the data much better (FIG. 8, 9). The model for the converging lens fits the data almost perfectly, and while the diverging lens fit is less than ideal, the data follows the overall trend of the model. To evaluate the Lens Maker s Equation, we uploaded a photo of our lens into python (FIG. 10). We then found the radius of curvature of the converging lens in pixels, and used the adjacent Lego blocks of known height to determine a conversion from pixels to mm. The original Lens Maker s equation can be simplified for a planoconvex lens since there is only one radius of curvature. We therefore modify Eq. (3) by taking the limit as π goes to infinity, giving: FIG. 8: The ratios of our image heights for different trials for a converging lens as compared to a model derived from Eq. (8) 1 FIG. 9: The ratios of our image heights for different trials for a diverging lens as compared to a model derived from Eq. (8). (9) with π being the index of refraction of BK7 glass and π the index of refraction of air. A circle of radius 313 pixels was used to fit the lens, which is equivalent to a real radius of ~ mm. Evaluating the Lens Maker s equation with this information yields a focal length of ~50.33 mm, extremely close to our expected value with a percent difference of only ~0.65%. FIG. 10: Fitting used to find radius of curvature for converging lens, Lego bricks for scale.

5 VI. DISCUSSIONS AND CONCLUSIONS After evaluating our data and comparing it to predictive models, we determined this experiment to be an overall success. In all cases, once everything was accounted for, our models were effective at predicting the data obtained. We found that our initial model using Eq. (6) appeared to mirror the data. If we consider the Lens and Magnification equations in tandem with the ray diagrams presented in FIG. 5, then this relationship makes sense because Eq. (6) does not account for the second lens, which is responsible for inverting the image generated by the first lens. After taking into consideration the effect of the second lens and arriving at Eq. (8), we found that our new models fit the data much more closely. There were a few discrepancies. In the case of the converging lens, when the object distance was close to the focal length (where we change from having a virtual image to a real image) we were getting a difference of approximately 10% between the model and the data. In addition, several areas of the diverging lens data noticeably wander from the model, though differences never reach 10%. The source of these errors is unclear. General sources of error include mistakes made when measuring the image height and object distances, which likely contributed to the above discrepancies. The Lens Maker s equation successfully determined the focal length with no difficulty. Overall, we successfully demonstrated that the image formation principles of a lens are well described by the Lens and Magnification equations, or more specifically, that a combination of these equations can accurately predict properties of formed images. to motion, including rotating about their center of gravity. This effects the quality of the data we obtain, and eliminating this kind of error could lead to better behaved data. VII. SYSTEM EVALUATION While the results from this experiment were very successful, there are still ways for us to improve our instrument. Firstly, the main goal would be to increase the overall size of the instrument. While we were taking measurements, we often found locations at which measurements were impossible. There were some locations where the virtual image generated by the lens was too large to be captured in the field of view, which led to us being unable to measure the image height for that object distance. This would involve increasing the size of the lens as well as the size and width of the track. We would also choose to use lenses with larger focal lengths, particularly a converging lens with a larger focal length, in order to have more available object distances within the focal length to produce virtual images. Secondly, it would be very beneficial to improve the quality of our lens and phone holders. Because our current holders are not very secure, the phone and lens are subject

Geometric Optics Converging Lenses and Mirrors Physics Lab IV

Objective Geometric Optics Converging Lenses and Mirrors Physics Lab IV In this set of lab exercises, the basic properties geometric optics concerning converging lenses and mirrors will be explored. The

Lab #1: Geometric Optics

Physics 123 Union College Lab #1: Geometric Optics I. Introduction In geometric optics, the ray approximation is combined with the laws of reflection and refraction and geometry to determine the location

Determination of Focal Length of A Converging Lens and Mirror

Physics 41- Lab 5 Determination of Focal Length of A Converging Lens and Mirror Objective: Apply the thin-lens equation and the mirror equation to determine the focal length of a converging (biconvex)

EXPERIMENT 6 OPTICS: FOCAL LENGTH OF A LENS

EXPERIMENT 6 OPTICS: FOCAL LENGTH OF A LENS The following website should be accessed before coming to class. Text reference: pp189-196 Optics Bench a) For convenience of discussion we assume that the light

Physics Laboratory: Lenses

Physics Laboratory: Lenses We have already seen how Snell s Law describes the refraction of light as it passes through media with different indices of refraction. Lenses are made of materials that generally

Ray Tracing: the Law of Reflection, and Snell s Law

Ray Tracing: the Law of Reflection, and Snell s Law Each of the experiments is designed to test or investigate the basic ideas of reflection and the ray-like behavior of light. The instructor will explain

Convex Mirrors. Ray Diagram for Convex Mirror

Convex Mirrors Center of curvature and focal point both located behind mirror The image for a convex mirror is always virtual and upright compared to the object A convex mirror will reflect a set of parallel

Home Work 14. Sol 17. (a) The mirror is concave. (b) f = +20 cm (positive, because the mirror is concave). (c) r = 2f = 2(+20 cm) = +40 cm.

Home Work 14 14-1 More mirrors. Object O stands on the central axis of a spherical or plane mirror. For this situation, each problem in the Table refers to (a) the type of mirror, (b) the focal distance

GEOMETRICAL OPTICS. Lens Prism Mirror

GEOMETRICAL OPTICS Geometrical optics is the treatment of the passage of light through lenses, prisms, etc. by representing the light as rays. A light ray from a source goes in a straight line through

Chapter 36 - Lenses. A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University

Chapter 36 - Lenses A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University 2007 Objectives: After completing this module, you should be able to: Determine

Chapter 23. The Refraction of Light: Lenses and Optical Instruments

Chapter 23 The Refraction of Light: Lenses and Optical Instruments Lenses Converging and diverging lenses. Lenses refract light in such a way that an image of the light source is formed. With a converging

Lecture PowerPoints. Chapter 23 Physics: Principles with Applications, 7 th edition Giancoli

Lecture PowerPoints Chapter 23 Physics: Principles with Applications, 7 th edition Giancoli This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching

Chapter 3: Mirrors and Lenses

Chapter 3: Mirrors and Lenses The Lens Equation Calculating image location Calculating magnification Special Lenses Ball lens retroreflector Fresnel lens Multiple Lenses Ray tracing Lens equation Aberrations

Experiment 3 Lenses and Images

Experiment 3 Lenses and Images Who shall teach thee, unless it be thine own eyes? Euripides (480?-406? BC) OBJECTIVES To examine the nature and location of images formed by es. THEORY Lenses are frequently

Lecture PowerPoints. Chapter 23 Physics: Principles with Applications, 7th edition Giancoli

Lecture PowerPoints Chapter 23 Physics: Principles with Applications, 7th edition Giancoli This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching

PHYSICS 262 GEOMETRIC OPTICS

PHYSICS 262 GEOMETRIC OPTICS Part I Position and Size of Image: Cardinal Points If the indices of refraction of all elements are known, together with the positions and radii of curvature of all surfaces,

The Thin Convex Lens convex lens focal point thin lens thin convex lens real images

1 The Thin Convex Lens In the previous experiment, we observed the phenomenon of refraction for a rectangular piece of glass. The bending or refraction of the light was observed for two parallel interfaces,

SPH3UW Unit 7.8 Multiple Lens Page 1 of 5

SPH3UW Unit 7.8 Multiple Lens Page of 5 Notes Physics Tool box Thin Lens is an optical system with two refracting surfaces. The most simplest thin lens contain two spherical surfaces that are close enough

Geometric Optics Physics 118/198/212. Geometric Optics

Background Geometric Optics This experiment deals with image formation with lenses. We will use what are referred to as thin lenses. Thin lenses are ordinary lenses like eyeglasses and magnifiers, but

Lesson 29: Lenses. Double Concave. Double Convex. Planoconcave. Planoconvex. Convex meniscus. Concave meniscus

Lesson 29: Lenses Remembering the basics of mirrors puts you half ways towards fully understanding lenses as well. The same sort of rules apply, just with a few modifications. Keep in mind that for an

General Science 1110L Lab Lab 7: CONVEX LENS

General Science 1110L Lab Lab 7: CONVEX LENS OBJECTIVE: To investigate the image formed by a certain thin convex lens and to determine its focal length. APPARATUS: Convex lens, optical bench, light source,

A STUDY OF LENSES INTRODUCTION. LAB LIGH.1 From Laboratory Manual of Elementary Physics, Westminster College

A STUDY OF LENSES LAB LIGH.1 From Laboratory Manual of Elementary Physics, Westminster College INTRODUCTION A lens is a piece of transparent material bounded by two curved surfaces or a curved surface

PROPERTIES OF THIN LENSES. Paraxial-ray Equations

PROPERTIES OF THIN LENSES Object: To measure the focal length of lenses, to verify the thin lens equation and to observe the more common aberrations associated with lenses. Apparatus: PASCO Basic Optical

Thin Lenses Drawing Ray Diagrams

Drawing Ray Diagrams Fig. 1a Fig. 1b In this activity we explore how light refracts as it passes through a thin lens. Eyeglasses have been in use since the 13 th century. In 1610 Galileo used two lenses

Thin Lenses. Physics 102 Workshop #7. General Instructions

Thin Lenses Physics 102 Workshop #7 Name: Lab Partner(s): Instructor: Time of Workshop: General Instructions Workshop exercises are to be carried out in groups of three. One report per group is due by

Understanding Spherical Mirrors

[ Assignment View ] [ EΓ°lisfrΓ¦Γ°i 2, vor 2007 34. Geometric Optics and Optical Instruments Assignment is due at 2:00am on Wednesday, January 17, 2007 Credit for problems submitted late will decrease to

Solution Derivations for Capa #13

Solution Derivations for Capa #13 1) A super nova releases 1.3 10 45 J of energy. It is 1540 ly from earth. If you were facing the star in question, and your face was a circle 7 cm in radius, how much

1. Reflection, Refraction, and Geometric Optics (Chapters 33 and 34) [ Edit ]

1 of 17 2/8/2016 9:34 PM Signed in as Weida Wu, Instructor Help Sign Out My Courses Course Settings University Physics with Modern Physics, 14e Young/Freedman Instructor Resources etext Study Area ( RUPHY228S16

9/16 Optics 1 /11 GEOMETRIC OPTICS

9/6 Optics / GEOMETRIC OPTICS PURPOSE: To review the basics of geometric optics and to observe the function of some simple and compound optical devices. APPARATUS: Optical bench, lenses, mirror, target

It bends away from the normal, like this. So the angle of refraction, r is greater than the angle of incidence, i.

Physics 1403 Lenses It s party time, boys and girls, because today we wrap up our study of physics. We ll get this party started in a bit, but first, you have some more to learn about refracted light.

waves rays Consider rays of light from an object being reflected by a plane mirror (the rays are diverging): mirror object

PHYS1000 Optics 1 Optics Light and its interaction with lenses and mirrors. We assume that we can ignore the wave properties of light. waves rays We represent the light as rays, and ignore diffraction.

The diagram below shows the image formed on the film when Moana takes a picture.

WAVES: LENSES QUESTIONS LENSES AND REFRACTION (2015;2) Tom uses a convex lens as a magnifying glass. He puts a petal of a flower 2.0 cm in front of the lens to study it. The lens has a focal length of

Lenses. Types of Lenses (The word lens is derived from the Latin word lenticula, which means lentil. A lens is in the shape of a lentil.

Lenses Notes_10_ SNC2DE_09-10 Types of Lenses (The word lens is derived from the Latin word lenticula, which means lentil. A lens is in the shape of a lentil. ) Most lenses are made of transparent glass

1 of 9 2/9/2010 3:38 PM

1 of 9 2/9/2010 3:38 PM Chapter 23 Homework Due: 8:00am on Monday, February 8, 2010 Note: To understand how points are awarded, read your instructor's Grading Policy. [Return to Standard Assignment View]

April 29. Physics 272. Spring Prof. Philip von Doetinchem

Physics 272 April 29 Spring 2014 http://www.phys.hawaii.edu/~philipvd/pvd_14_spring_272_uhm.html Prof. Philip von Doetinchem philipvd@hawaii.edu Phys272 - Spring 14 - von Doetinchem - 411 Summary Object

O5: Lenses and the refractor telescope

O5. 1 O5: Lenses and the refractor telescope Introduction In this experiment, you will study converging lenses and the lens equation. You will make several measurements of the focal length of lenses and

Lesson 26: Reflection & Mirror Diagrams

Lesson 26: Reflection & Mirror Diagrams The Law of Reflection There is nothing really mysterious about reflection, but some people try to make it more difficult than it really is. All EMR will reflect

Chapter 17 Light and Image Formation

Chapter 7 Light and Image Formation Reflection and Refraction How is an image in a mirror produced? Reflection and Image Formation In chapter 6 we studied physical optics, which involve wave aspects of

Experiment 8. Thin Lenses. Measure the focal length of a converging lens. Investigate the relationship between power and focal length.

Experiment 8 Thin Lenses 8.1 Objectives Measure the focal length of a converging lens. Measure the focal length of a diverging lens. Investigate the relationship between power and focal length. 8.2 Introduction

Curved surfaces and lenses

Curved surfaces and lenses (Material taken from: Optics, by E. Hecht, 4th Ed., Ch: 5) One of the important challenges pertaining to the practical aspects of optics is wave shaping, i.e. controlling the

REFLECTION & REFRACTION

REFLECTION & REFRACTION OBJECTIVE: To study and verify the laws of reflection and refraction using a plane mirror and a glass block. To see the virtual images that can be formed by the reflection and refraction

Geometric Optics. Chapter 34. Goals for Chapter 34. Reflection at a plane surface. Introduction How do magnifying lenses work?

Goals for Chapter 34 Chapter 34 To see how plane and curved mirrors form images To learn how lenses form images Geometric Optics To understand how a camera works To analyze defects in vision and how to

Lecture Notes for Chapter 34: Images

Lecture Notes for hapter 4: Images Disclaimer: These notes are not meant to replace the textbook. Please report any inaccuracies to the professor.. Spherical Reflecting Surfaces Bad News: This subject

C) D) As object AB is moved from its present position toward the left, the size of the image produced A) decreases B) increases C) remains the same

1. For a plane mirror, compared to the object distance, the image distance is always A) less B) greater C) the same 2. Which graph best represents the relationship between image distance (di) and object

Page 1 Class 10 th Physics LIGHT REFLECTION AND REFRACTION

Page 1 LIGHT Light is a form of energy, which induces the sensation of vision in our eyes and makes us able to see various things present in our surrounding. UNITS OF LIGHT Any object which has an ability

Homework 13 chapter 36: 17, 21, 33, 74

http://iml.umkc.edu/physics/wrobel/phy50/homework.htm Homework chapter 6: 7,,, 74 Problem 6.7 A spherical mirror is to be used to form, on a screen located 5 m from the object, an image five times the

Multiple Element Optical Systems

O4 ultiple Element Optical Systems Introduction Optical elements and systems irrors Lenses Systems Instruments O4. Introduction In this section we will be presented with a series of examples to illustrate

AP Physics B Ch. 23 and Ch. 24 Geometric Optics and Wave Nature of Light

AP Physics B Ch. 23 and Ch. 24 Geometric Optics and Wave Nature of Light Name: Period: Date: MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) Reflection,

Lecture 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

Physics 6C. Cameras and the Human Eye

Physics 6C Cameras and the Human Eye CAMERAS A typical camera uses a converging lens to focus a real (inverted) image onto photographic film (or in a digital camera the image is on a CCD chip). (Picture

Chapter 17: Light and Image Formation

Chapter 17: Light and Image Formation 1. When light enters a medium with a higher index of refraction it is A. absorbed. B. bent away from the normal. C. bent towards from the normal. D. continues in the

Lab 9. Optics. 9.1 Introduction

Lab 9 Name: Optics 9.1 Introduction Unlike other scientists, astronomers are far away from the objects they want to examine. Therefore astronomers learn everything about an object by studying the light

Chapter 23. Ray Optics. Chapter 23. Ray Optics. What is specular reflection? Chapter 23. Reading Quizzes

Chapter 23. Ray Optics Chapter 23. Ray Optics Our everyday experience that light travels in straight lines is the basis of the ray model of light. Ray optics apply to a variety of situations, including

Basic Optics System OS-8515C

40 50 30 60 20 70 10 80 0 90 80 10 20 70 T 30 60 40 50 50 40 60 30 C 70 20 80 10 90 90 0 80 10 70 20 60 50 40 30 Instruction Manual with Experiment Guide and Teachers Notes 012-09900B Basic Optics System

Procedure: Geometrical Optics. Theory Refer to your Lab Manual, pages 291 294. Equipment Needed

Theory Refer to your Lab Manual, pages 291 294. Geometrical Optics Equipment Needed Light Source Ray Table and Base Three-surface Mirror Convex Lens Ruler Optics Bench Cylindrical Lens Concave Lens Rhombus

Reflection and Refraction

Equipment Reflection and Refraction Acrylic block set, plane-concave-convex universal mirror, cork board, cork board stand, pins, flashlight, protractor, ruler, mirror worksheet, rectangular block worksheet,

Question 2: The radius of curvature of a spherical mirror is 20 cm. What is its focal length?

Question 1: Define the principal focus of a concave mirror. ANS: Light rays that are parallel to the principal axis of a concave mirror converge at a specific point on its principal axis after reflecting

1. You stand two feet away from a plane mirror. How far is it from you to your image? a. 2.0 ft c. 4.0 ft b. 3.0 ft d. 5.0 ft

Lenses and Mirrors 1. You stand two feet away from a plane mirror. How far is it from you to your image? a. 2.0 ft c. 4.0 ft b. 3.0 ft d. 5.0 ft 2. Which of the following best describes the image from

Ray Optics 11/96. Physical Science 101 Name Section. Partner s Name

Physical Science 101 Name Section Partner s Name Purpose: The purpose of this lab is to study the laws of reflection and refraction for flat surfaces and to find out how converging lenses and converging

Objectives 426 CHAPTER 10 LIGHT AND OPTICAL SYSTEMS

Objectives Explain what is meant by the curvature and focal length of mirrors and lenses. Explain how curvature and focal length are related. Use light rays to trace light from an object to a mirror to

MIRRORS AND REFLECTION

MIRRORS AND REFLECTION PART 1 ANGLE OF INCIDENCE, ANGLE OF REFLECTION In this exploration we will compare ΞΈ i (angle of incidence) and ΞΈ r (angle of reflection). We will also investigate if rays are reversed

Rutgers Analytical Physics 750:228, Spring 2016 ( RUPHY228S16 )

1 of 13 2/17/2016 5:28 PM Signed in as Weida Wu, Instructor Help Sign Out Rutgers Analytical Physics 750:228, Spring 2016 ( RUPHY228S16 ) My Courses Course Settings University Physics with Modern Physics,

How can I predict how big my reflection will appear in a mirror? Think about it and we might try your solution.

How can I predict how big my reflection will appear in a mirror? Think about it and we might try your solution. Introduction to Optics Lecture 12 (See Giancoli Chapter 23) Refraction Phenomena Silas Laycock,

Chapter 34B - Reflection and Mirrors II (Analytical)

Chapter 34B - Reflection and Mirrors II (Analytical) A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University 2007 Objectives: After completing this module,

PHY 171. Homework 5 solutions. (Due by beginning of class on Wednesday, February 8, 2012)

PHY 171 (Due by beginning of class on Wednesday, February 8, 2012) 1. Consider the figure below which shows four stacked transparent materials. In this figure, light is incident at an angle ΞΈ 1 40.1 on

RAY OPTICS II 7.1 INTRODUCTION

7 RAY OPTICS II 7.1 INTRODUCTION This chapter presents a discussion of more complicated issues in ray optics that builds on and extends the ideas presented in the last chapter (which you must read first!)

Optics and Image formation

Optics and Image formation Pascal Chartrand chercheur-agrΓ©gΓ© DΓ©partement de Biochimie email: p.chartrand@umontreal.ca The Light Microscope Four centuries of history Vibrant current development One of the

Turnbull High School Physics Department. CfE. National 4 /National. Physics. Unit 1: Waves and Radiation. Section 3: Light

Turnbull High School Physics Department CfE National 4 /National 5 Physics Unit 1: Waves and Radiation Section 3: Light Name: Class: 1 National 5 Unit 1: Section 3 I can state the law of reflection and

PHY208FALL2008. Week3HW. Is Light Reflected or Refracted? Due at 11:59pm on Sunday, September 21, [ Print ] View Grading Details

Assignment Display Mode: View Printable Answers PHY208FALL2008 Week3HW [ Print ] Due at 11:59pm on Sunday, September 21, 2008 View Grading Details The next exercise is about reflection and refraction of

Analytical Technologies in Biotechnology Dr. Ashwani K. Sharma Department of Biotechnology Indian Institute of Technology, Roorkee

Analytical Technologies in Biotechnology Dr. Ashwani K. Sharma Department of Biotechnology Indian Institute of Technology, Roorkee Module 1 Microscopy Lecture - 2 Basic concepts in microscopy 2 In this

Lecture 14 Images Chapter 34

Lecture 4 Images Chapter 34 Preliminary topics before mirrors and lenses Law of Reflection Dispersion Snell s Law Brewsters Angle Law of Reflection Dispersion Snell s Law Brewsters Angle Geometrical Optics:Study

Physics I Honors: Chapter 14 Practice Test - Refraction of Light

Physics I Honors: Chapter 14 Practice Test - Refraction of Light Multiple Choice Identify the letter of the choice that best completes the statement or answers the question. 1. Refraction is the bending

P222. Optics Supplementary Note # 3: Mirrors Alex R. Dzierba Indiana University. ΞΈ ΞΈ. Plane Mirrors

P222 Optics Supplementary Note # 3: Mirrors Alex R. Dzierba Indiana University Plane Mirrors Let s talk about mirrors. We start with the relatively simple case of plane mirrors. Suppose we have a source

HOMEWORK 4 with Solutions

Winter 996 HOMEWORK 4 with Solutions. ind the image of the object for the single concave mirror system shown in ig. (see next pages for worksheets) by: (a) measuring the radius R and calculating the focal

2) A convex lens is known as a diverging lens and a concave lens is known as a converging lens. Answer: FALSE Diff: 1 Var: 1 Page Ref: Sec.

Physics for Scientists and Engineers, 4e (Giancoli) Chapter 33 Lenses and Optical Instruments 33.1 Conceptual Questions 1) State how to draw the three rays for finding the image position due to a thin

EXPERIMENT 8. To Determine the Wavelength of Sodium Light using Newton s Rings. Introduction. Background

EXPERIMENT 8 To Determine the Wavelength of Sodium Light using Newton s Rings Introduction Please read additional instructions on the bench for setting up the PC and camera for this experiment Newton s

Lenses and Telescopes

A. Using single lenses to form images Lenses and Telescopes The simplest variety of telescope uses a single lens. The image is formed at the focus of the telescope, which is simply the focal plane of the

and that for the minima is min ( m 1 2). Divide the second equation by the first and solve for the order of the maximum, m.

USEFUL FORMULAE AND DATA 1. Wien s Law: pt = 2.90 10-3 m K 2. v=c/n, is the speed of light in a material with an index of refraction n 3. Snell s Law: n1 sin 1 = n2 sin 2, where subscripts 1 stands for

Refractive Index and Dispersion: Prism Spectrometer

Refractive Index and Dispersion: Prism Spectrometer OBJECTIVES: The purpose of this experiment is to study the phenomenon of dispersion i.e. to determine the variation of refractive index of the glass

Solution Derivations for Capa #14

Solution Derivations for Capa #4 ) An image of the moon is focused onto a screen using a converging lens of focal length (f = 34.8 cm). The diameter of the moon is 3.48 0 6 m, and its mean distance from

Physics 9 th Standard Chapter 10 LENS Fill in the blanks 1. A transparent material which is thicker in the middle and thinner at the edges is called

Physics 9 th Standard Chapter 10 LENS Fill in the blanks 1. A transparent material which is thicker in the middle and thinner at the edges is called convex lens 2. An object should be placed at twice the

PRACTICAL APPLICATIONS

PRACTICAL APPLICATIONS OF OPTICAL LENSES: TELESCOPES & PROJECTORS By Diane Kasparie & Mary Young PRACTICAL APPLICATION OF OPTICAL LENSES: TELESCOPES & PROJECTORS Light & Sound workshop SUMMER INSTITUTE:

OPTICAL IMAGES DUE TO LENSES AND MIRRORS *

1 OPTICAL IMAGES DUE TO LENSES AND MIRRORS * Carl E. Mungan U.S. Naval Academy, Annapolis, MD ABSTRACT The properties of real and virtual images formed by lenses and mirrors are reviewed. Key ideas are

Chapter 22: Mirrors and Lenses

Chapter 22: Mirrors and Lenses How do you see sunspots? When you look in a mirror, where is the face you see? What is a burning glass? Make sure you know how to:. Apply the properties of similar triangles;

Refraction and Lenses. Snell s Law Total internal reflection Dispersion Absorption Scattering

Refraction and Lenses Snell s Law Total internal reflection Dispersion Absorption Scattering Refraction Two things happen when a light ray is incident on a smooth boundary between two transparent materials:

Law of Reflection. The angle of incidence (i) is equal to the angle of reflection (r)

Light GCSE Physics Reflection Law of Reflection The angle of incidence (i) is equal to the angle of reflection (r) Note: Both angles are measured with respect to the normal. This is a construction line

All the Sun through the eye of a pinhole

All the Sun through the eye of a pinhole Solar-B Education and Public Outreach (EPO) Solar-B is a multinational solar observatory satellite project headed by the Japanese Space Agency (ISAS), in partnership

1051-232 Imaging Systems Laboratory II. Laboratory 4: Basic Lens Design in OSLO April 2 & 4, 2002

05-232 Imaging Systems Laboratory II Laboratory 4: Basic Lens Design in OSLO April 2 & 4, 2002 Abstract: For designing the optics of an imaging system, one of the main types of tools used today is optical

Which type of electromagnetic radiation would be used to take the photograph? ... (1)

Q. After a person is injured a doctor will sometimes ask for a photograph to be taken of the patient s bone structure, e.g. in the case of a suspected broken arm. (i) Which type of electromagnetic radiation

Revision problem. Chapter 18 problem 37 page 612. Suppose you point a pinhole camera at a 15m tall tree that is 75m away.

Revision problem Chapter 18 problem 37 page 612 Suppose you point a pinhole camera at a 15m tall tree that is 75m away. 1 Optical Instruments Thin lens equation Refractive power Cameras The human eye Combining

Sensor Size & Field of View

Sensor Size & Field of View CONTENTS BASIC LENS CONCEPTS Sensor Dimensions Focal Length Angle of View Field of View Depth of Field FIELD OF VIEW CHANGES WITH SENSOR SIZE HOW TO CALCULATE & USE THE CROP

Light and its effects

Light and its effects Light and the speed of light Shadows Shadow films Pinhole camera (1) Pinhole camera (2) Reflection of light Image in a plane mirror An image in a plane mirror is: (i) the same size

Waves and Modern Physics PHY Spring 2012

Waves and Modern Physics PHY 123 - Spring 2012 1st Midterm Exam Wednesday, February 22 Chapter 32 Light: Reflec2on and Refrac2on Units of Chapter 32 Today we will cover: The Ray Model of Light Reflection;

Equations, Lenses and Fractions

46 Equations, Lenses and Fractions The study of lenses offers a good real world example of a relation with fractions we just can t avoid! Different uses of a simple lens that you may be familiar with are

Geometric Optics Physics Leaving Cert Quick Notes

Geometric Optics Physics Leaving Cert Quick Notes Geometric Optics Properties of light Light is a form of energy. As such it can be converted into other forms of energy. We can demonstrate this using a

Chapter 23. The Reflection of Light: Mirrors

Chapter 23 The Reflection of Light: Mirrors Wave Fronts and Rays Defining wave fronts and rays. Consider a sound wave since it is easier to visualize. Shown is a hemispherical view of a sound wave emitted

LASER OPTICAL DISK SET

LASER OPTICAL DISK SET LODS01 5 6 7 4 8 3 9 2 10 1 11 1. Description The laser Optical Disk Set includes a Laser Ray Box powered by a low voltage wall-mount power supply, a set of eight ray optics elements