Shedding Light on Lenses
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Object-Image Real Image Virtual Image
Object-Image • A physical object is usually observed by reflected light that diverges from the object. • An optical system (mirrors or lenses) can 3.1 Images formed by Mirrors and Lenses produce an image of the object by redirecting the light. • Images – Real Image • Image formation by mirrors – Virtual Image • Images formed by lenses Real Image Virtual Image Optical System ing diverging erg converging diverging diverging div Object Object real Image Optical System virtual Image Light appears to come from the virtual image but does not Light passes through the real image pass through the virtual image Film at the position of the real image is exposed. Film at the position of the virtual image is not exposed. Each point on the image can be determined Image formed by a plane mirror. by tracing 2 rays from the object. B p q B’ Object Image The virtual image is formed directly behind the object image mirror. Light does not A pass through A’ the image mirror A virtual image is formed by a plane mirror at a distance q behind the mirror. q = -p 1 Parabolic Mirrors Parabolic Reflector Optic Axis Parallel rays reflected by a parabolic mirror are focused at a point, called the Parabolic mirrors can be used to focus incoming parallel rays to a small area Focal Point located on the optic axis. or to direct rays diverging from a small area into parallel rays. Spherical mirrors Parallel beams focus at the focal point of a Concave Mirror. •Spherical mirrors are much easier to fabricate than parabolic mirrors • A spherical mirror is an approximation of a parabolic Focal point mirror for small curvatures. -
Lab 11: the Compound Microscope
OPTI 202L - Geometrical and Instrumental Optics Lab 9-1 LAB 9: THE COMPOUND MICROSCOPE The microscope is a widely used optical instrument. In its simplest form, it consists of two lenses Fig. 9.1. An objective forms a real inverted image of an object, which is a finite distance in front of the lens. This image in turn becomes the object for the ocular, or eyepiece. The eyepiece forms the final image which is virtual, and magnified. The overall magnification is the product of the individual magnifications of the objective and the eyepiece. Figure 9.1. Images in a compound microscope. To illustrate the concept, use a 38 mm focal length lens (KPX079) as the objective, and a 50 mm focal length lens (KBX052) as the eyepiece. Set them up on the optical rail and adjust them until you see an inverted and magnified image of an illuminated object. Note the intermediate real image by inserting a piece of paper between the lenses. Q1 ● Can you demonstrate the final image by holding a piece of paper behind the eyepiece? Why or why not? The eyepiece functions as a magnifying glass, or simple magnifier. In effect, your eye looks into the eyepiece, and in turn the eyepiece looks into the optical system--be it a compound microscope, a spotting scope, telescope, or binocular. In all cases, the eyepiece doesn't view an actual object, but rather some intermediate image formed by the "front" part of the optical system. With telescopes, this intermediate image may be real or virtual. With the compound microscope, this intermediate image is real, formed by the objective lens. -
How Do the Lenses in a Microscope Work?
Student Name: _____________________________ Date: _________________ How do the lenses in a microscope work? Compound Light Microscope: A compound light microscope uses light to transmit an image to your eye. Compound deals with the microscope having more than one lens. Microscope is the combination of two words; "micro" meaning small and "scope" meaning view. Early microscopes, like Leeuwenhoek's, were called simple because they only had one lens. Simple scopes work like magnifying glasses that you have seen and/or used. These early microscopes had limitations to the amount of magnification no matter how they were constructed. The creation of the compound microscope by the Janssens helped to advance the field of microbiology light years ahead of where it had been only just a few years earlier. The Janssens added a second lens to magnify the image of the primary (or first) lens. Simple light microscopes of the past could magnify an object to 266X as in the case of Leeuwenhoek's microscope. Modern compound light microscopes, under optimal conditions, can magnify an object from 1000X to 2000X (times) the specimens original diameter. "The Compound Light Microscope." The Compound Light Microscope. Web. 16 Feb. 2017. http://www.cas.miamioh.edu/mbi-ws/microscopes/compoundscope.html Text is available under the Creative Commons Attribution-NonCommercial 4.0 International (CC BY-NC 4.0) license. - 1 – Student Name: _____________________________ Date: _________________ Now we will describe how a microscope works in somewhat more detail. The first lens of a microscope is the one closest to the object being examined and, for this reason, is called the objective. -
Lecture 37: Lenses and Mirrors
Lecture 37: Lenses and mirrors • Spherical lenses: converging, diverging • Plane mirrors • Spherical mirrors: concave, convex The animated ray diagrams were created by Dr. Alan Pringle. Terms and sign conventions for lenses and mirrors • object distance s, positive • image distance s’ , • positive if image is on side of outgoing light, i.e. same side of mirror, opposite side of lens: real image • s’ negative if image is on same side of lens/behind mirror: virtual image • focal length f positive for concave mirror and converging lens negative for convex mirror and diverging lens • object height h, positive • image height h’ positive if the image is upright negative if image is inverted • magnification m= h’/h , positive if upright, negative if inverted Lens equation 1 1 1 푠′ ℎ′ + = 푚 = − = magnification 푠 푠′ 푓 푠 ℎ 푓푠 푠′ = 푠 − 푓 Converging and diverging lenses f f F F Rays refract towards optical axis Rays refract away from optical axis thicker in the thinner in the center center • there are focal points on both sides of each lens • focal length f on both sides is the same Ray diagram for converging lens Ray 1 is parallel to the axis and refracts through F. Ray 2 passes through F’ before refracting parallel to the axis. Ray 3 passes straight through the center of the lens. F I O F’ object between f and 2f: image is real, inverted, enlarged object outside of 2f: image is real, inverted, reduced object inside of f: image is virtual, upright, enlarged Ray diagram for diverging lens Ray 1 is parallel to the axis and refracts as if from F. -
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 lens, paraxial rays that are parallel to the principal axis converge to the focal point, F. The focal length, f, is the distance between F and the lens. Two prisms can bend light toward the principal axis acting like a crude converging lens but cannot create a sharp focus. Lenses With a diverging lens, paraxial rays that are parallel to the principal axis appear to originate from the focal point, F. The focal length, f, is the distance between F and the lens. Two prisms can bend light away from the principal axis acting like a crude diverging lens, but the apparent focus is not sharp. Lenses Converging and diverging lens come in a variety of shapes depending on their application. We will assume that the thickness of a lens is small compared with its focal length è Thin Lens Approximation The Formation of Images by Lenses RAY DIAGRAMS. Here are some useful rays in determining the nature of the images formed by converging and diverging lens. Since lenses pass light through them (unlike mirrors) it is useful to draw a focal point on each side of the lens for ray tracing. The Formation of Images by Lenses IMAGE FORMATION BY A CONVERGING LENS do > 2f When the object is placed further than twice the focal length from the lens, the real image is inverted and smaller than the object. -
11.4 the Optics of Other Devices
11.4 The Optics of Other Devices projection head Activity 11.4.1 Optics of an Overhead Projector focus knob Overhead projectors (Figure 1), like many optical systems, consist of three sys- tems that work together: a mechanical system, an electronic system, and an optical system. Their function is to project an enlarged image from a transparent film onto a distant screen. In this activity, you will see how the different optical optical components of the projector work together. stage Materials overhead projector appropriate screwdrivers projector case Procedure Figure 1 1. Before turning on the overhead projector, open the optical stage to see An overhead projector inside the projector case. Sketch the arrangement of optical components by considering what a cross-section of the projector would look like. Note the arrangement of any bulbs, mirrors, or lenses that you find in the projector case. Add the optics of the projection head to your sketch. 2. Turn on the projector to project an image of a letter onto a screen nearby. Make adjustments to focus the image. 3. Use the focus knob to move the projection head upward. How does this affect the image? Refocus the image. 4. Use the focus knob to move the projection head downward. How does this affect the image? Refocus the image. 5. Move the projector farther from the screen. How does this affect the image? Analysis (a) Draw a ray diagram, with at least three different rays, showing how light travels from the bulb to the screen. (b) In table form, describe the structure and function of each optical compo- nent of the overhead projector. -
Geometric Optics
GEOMETRIC OPTICS I. What is GEOMTERIC OPTICS In geometric optics, LIGHT is treated as imaginary rays. How these rays interact with at the interface of different media, including lenses and mirrors, is analyzed. LENSES refract light, so we need to know how light bends when entering and exiting a lens and how that interaction forms an image. MIRRORS reflect light, so we need to know how light bounces off of surfaces and how that interaction forms an image. II. Refraction We already learned that waves passing from one media to another cause light to do two things: Change path Change wavelength which means…Change velocity (speed of light) The velocity DECREASES and the wavelength SHORTENS when light passes from a “faster” to a “slower” media. The velocity INCREASES and the wavelength LENGTHENS when light passes from a “slower” to a “faster” media. In either case, the FREQUENCY remains the same. 1 refraction, continued When light hits the interface of two media at an angle, the lower part of the ray interacts first, thus slowing it down before the rest of the ray meets the interface. This rotates the ray toward the normal. The NORMAL LINE is an imaginary line PERPENDICULAR to the interface of two media. The REFRACTIVE INDEX of a substance tells you how much light will change speed (or bend) when it passes through the substance. It is the ratio of the speed of light in the medium to the speed of light in a vacuum. The medium will commonly n is the refractive index be air, water, glass, plastic c is the speed of light in a vacuum 2 refraction, continued substance refractive index, n vacuum 1 air 1.000277 water 1.333 glass 1.50 The table of refractive index values shows you that light slows down only a little in air, but its speed is reduced about 33% in glass. -
Image Formation Types of Images
Image formation A. Karle Physics 202 Nov. 27, 2007 Chapter 36 • Mirrors • Images • Ray diagrams • Lenses As usual, these notes are only a complement to the notes on the whiteboard. Types of Images • A real image is formed when light rays pass through and diverge from the image point – Real images can be displayed on screens • A virtual image is formed when light rays do not pass through the image point but only appear to diverge from that point – Virtual images cannot be displayed on screens 1 Images Formed by Flat Mirrors • Simplest possible mirror • Light rays leave the source and are reflected from the mirror • Point I is called the image of the object at point O • The image is virtual Images Formed by Flat Mirrors Definitions: • The object distance Flat mirror: – Denoted by p • -|p|=|q| • The image distance – Denoted by q • M = 1 • The lateral magnification •The image is virtual – Denoted by M=h’/h •The image is upright 2 Application – Day and Night Settings on Auto Mirrors • With the daytime setting, the bright beam of reflected light is directed into the driver’s eyes • With the nighttime setting, the dim beam of reflected light is directed into the driver’s eyes, while the bright beam goes elsewhere Spherical mirrors: Concave Mirror Notation • Radius of curvature: R • Center of curvature: C • A line drawn from C to V: principal axis of the mirror 3 Spherical Aberration • Rays that are far from the principal axis converge to other points on the principal axis • This produces a blurred image • The effect is called spherical aberration Image Formed by a Concave Mirror Geometrical analysis shows: 1. -
Reflection Angle of Incidence = Angle of Reflection
Physics 212 Lecture 27: Mirrors Physics 212 Lecture 27, Slide 1 Music Who is the Artist? A) Soul Rebels Brass Band B) John Boutte C) New Orleans Nightcrawlers D) Paul Sanchez & Shammar Allen E) Alex McMurray and Matt Perrine Why? Threadhead Records Beats Shazam !! Fan-funded and volunteer run record company Wonderful music from New Orleans Hint: Thursday’s artists also did a great set at Lagniappe stage last Jazzfest Physics 212 Lecture 27 Your Comments “Since the extended rays intersect behind the convex mirror, where there is no light, is the image How can you have a real image with a mirror? It always looks like we're looking at something behind the mirror. I don't understand how a mirror can produce a real image. produced virtual or real? wouldn't the image just be magnified? I'm so confused.” We will Do Examples “When are images real and when are they inverted in Clarify Sign Conventions mirrors?” Orientation of images “Not too bad. Just a recap of all the sign conventions Note How Similar This including lenses would be nice” Lecture is to the Lenses Lecture !! “How can you have a real image with a mirror? It always Does a virtual image also show that the image is upright? And vice versa, does a real image also show that the image is inverted? looks like we're looking at something behind the mirror. I don't understand how a mirror can produce a real image.” Go over drawing the lines for convex mirrors again “Go over drawing the lines for convex mirrors again” Even better – the calculation Is there an easy way to memorize what is a concave lens/mirror and what is a convex lens/mirror? “When you look at a shiny spoon, you can see yourself upside down on the concave part, and right side up on the convex part. -
Day Laboratory Exercise #3: Optics and Telescopes Page 1
AS102 - Day Laboratory Exercise #3: Optics and Telescopes Page 1 DAY LABORATORY EXERCISE #3: OPTICS AND TELESCOPES Goals: To explore the functions of simple lenses To construct and use a refracting telescope To understand the concepts of focal length, focal ratio, and magnification. To study aberrations in simple telescope systems. To explore the concept of angular resolution. Equipment: Lens kits, optical benches, light sources, rulers, calculators Methods: Measure lens focal lengths by forming images of distant objects Focus refracting telescope on distant object - measure lens separations Compare optical aberrations of refracting and reflecting telescopes Explore optical systems using a multiple lens optics kit and light source Measure angular resolution of the eye using distant eye chart Introduction - Telescopes are the primary instruments for the acquisition of data by astronomers. This exercise investigates the basic principles of geometric optics as applied to telescopes. You will primarily use refracting telescopes for the examples, but what you learn can be applied to any telescope (i.e., reflecting or radio). Lenses and Mirrors - A positive lens has at least one convex surface and is capable of focusing light from a distant object into a real image, that is, an image which can be seen projected onto a screen (see Figure 1). However, the same lens, when placed close to an object, produces a magnified virtual image which can be seen through the lens with the eye, but cannot be projected onto a screen (see Figure 2). A negative lens has at least one concave surface and always produces a virtual image. All of the lenses in this exercise have convex surfaces (the glass surface bulges outward from the lens center). -
US03CPHY21 Optics Unit1
SARDAR PATEL UNIVERSITY Vallabh Vidyanagar-388120 B.Sc. (semester -3) Subject; Physics Course; US03CPHY21 Optics (Four credit Course-4 hours per week) (Effective from –June 2019) UNIT- I GEOMETRICAL OPTICS [Lens systems (Chapter-4)]: Introduction: A lens is an image-forming device. It forms an image by refraction of light at its two bounding surfaces. In general, a lens is made of glass and is bounded by two regular curved surfaces; or by one spherical surface and a plane surface. Spherical surfaces are easy to make. Therefore, most lenses are made of spherical surfaces and have a wide range of curvatures. Other transparent materials such as quartz, fused silica and plastics are also used in making lenses. A single lens with two refracting surfaces is a simple lens. We study here the behaviour of a simple lens, with a view to gain familiarity with lens systems. We use the ray concept to understand the behaviour of light passing through lenses and derive the relationship between focal length of the lens, object distance and image distance. Different types of lenses LENSES: Lenses are mainly of two types- convex lens and concave lens. A convex lens is thicker at the center than at the edges while a concave lens is thinner at the center than at the edges. A convex lens is a converging lens since a parallel beam of light, after refraction, converges to a point, F. A concave lens is called a diverging lens since rays coming parallel to the principal axis, after refraction, diverge out and seem to come from a point, F. -
Inside the Camera Obscura – Optics and Art Under the Spell of the Projected Image
MAX-PLANCK-INSTITUT FÜR WISSENSCHAFTSGESCHICHTE Max Planck Institute for the History of Science 2007 PREPRINT 333 Wolfgang Lefèvre (ed.) Inside the Camera Obscura – Optics and Art under the Spell of the Projected Image TABLE OF CONTENTS PART I – INTRODUCING AN INSTRUMENT The Optical Camera Obscura I A Short Exposition Wolfgang Lefèvre 5 The Optical Camera Obscura II Images and Texts Collected and presented by Norma Wenczel 13 Projecting Nature in Early-Modern Europe Michael John Gorman 31 PART II – OPTICS Alhazen’s Optics in Europe: Some Notes on What It Said and What It Did Not Say Abdelhamid I. Sabra 53 Playing with Images in a Dark Room Kepler’s Ludi inside the Camera Obscura Sven Dupré 59 Images: Real and Virtual, Projected and Perceived, from Kepler to Dechales Alan E. Shapiro 75 “Res Aspectabilis Cujus Forma Luminis Beneficio per Foramen Transparet” – Simulachrum, Species, Forma, Imago: What was Transported by Light through the Pinhole? Isabelle Pantin 95 Clair & Distinct. Seventeenth-Century Conceptualizations of the Quality of Images Fokko Jan Dijksterhuis 105 PART III – LENSES AND MIRRORS The Optical Quality of Seventeenth-Century Lenses Giuseppe Molesini 117 The Camera Obscura and the Availibility of Seventeenth Century Optics – Some Notes and an Account of a Test Tiemen Cocquyt 129 Comments on 17th-Century Lenses and Projection Klaus Staubermann 141 PART IV – PAINTING The Camera Obscura as a Model of a New Concept of Mimesis in Seventeenth-Century Painting Carsten Wirth 149 Painting Technique in the Seventeenth Century in Holland and the Possible Use of the Camera Obscura by Vermeer Karin Groen 195 Neutron-Autoradiography of two Paintings by Jan Vermeer in the Gemäldegalerie Berlin Claudia Laurenze-Landsberg 211 Gerrit Dou and the Concave Mirror Philip Steadman 227 Imitation, Optics and Photography Some Gross Hypotheses Martin Kemp 243 List of Contributors 265 PART I INTRODUCING AN INSTRUMENT Figure 1: ‘Woman with a pearl necklace’ by Vermeer van Delft (c.1664).