Optics for Residents Amy Nau O.D., F.A.A.O

Slides:



Advertisements
Similar presentations
Reflection at a Spherical Surface
Advertisements

Chapter 36 - Lenses A PowerPoint Presentation by
Option G2: Optical Instruments
Consider Refraction at Spherical Surfaces:
Option G: Electromagnetic Waves G2: Optical Instruments.
Cutnell/Johnson Physics 7th edition
Notation for Mirrors and Lenses
1© Manhattan Press (H.K.) Ltd. Final image at infinity Eye-ring Eye-ring 12.6 Refracting telescope.
Convex and Concave Lenses
With Lenses Created by Derek J. Wells. Under the expressed written consent of Derek J. Wells in accordance with the rules and by-laws of Derek J. Wells.
→ ℎ
Chapter 31 Images.
Chapter 23 Mirrors and Lenses.
Chapter 23 Mirrors and Lenses. Notation for Mirrors and Lenses The object distance is the distance from the object to the mirror or lens Denoted by p.
Chapter 23 Mirrors and Lenses.
and Optical Instruments
Lecture 23 Mirrors Lens.
2 nd & 3 th N.U.T.S. Workshops Gulu University Naples FEDERICO II University 3 – Imaging (thin lenses and spherical mirrors)
Example A 2.0 cm high object is placed 5 cm in front of a +10 cm focal length lens. Where is the object located? Is it real or virtual? Find the height.
Chapter 36 Image Formation. Summary: mirrors Sign conventions: + on the left - on the right Convex and plane mirrors: only virtual images (for real objects)
Magnification of lenses Images
Fundamental of Optical Engineering Lecture 2.  In order to locate the image, the 2 rays are needed as ◦ The parallel ray: parallel to the axis and then,
Reflection & Mirrors.
Physics 1502: Lecture 30 Today’s Agenda Announcements: –Midterm 2: Monday Nov. 16 … –Homework 08: due Friday Optics –Mirrors –Lenses –Eye.
Physics 1402: Lecture 31 Today’s Agenda Announcements: –Midterm 2: Monday Nov. 16 … –Homework 08: due Wednesday (after midterm 2) Optics –Lenses –Eye.
Thin Lenses 91 is the highest grade while 75 is the lowest grade. 91 is the highest grade while 75 is the lowest grade. Best Project ( Website and Reflection.
Chapter 23 Mirrors and Lenses.
Optics 1----by Dr.H.Huang, Department of Applied Physics
Textbook sections 27-1 – 27-3 Physics 1161: PreLecture 25 Lenses and your EYE Ciliary Muscles.
Physics 1161: Lecture 19 Lenses and your EYE
Refraction through a lens. we have seen people using spectacles for reading. The watchmakers use a small glass to see tiny parts. Pistol or rifle shooters.
Chapter 3: Mirrors and Lenses. Lenses –Refraction –Converging rays –Diverging rays Converging Lens –Ray tracing rules –Image formation Diverging Lens.
Thin Lenses Chapter 15.
1 Chapter 34 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.
Find image with a thin lens
Geometric Optics Conceptual Quiz 23.
Physics 1C Lecture 26A.
Geometric Optics September 14, Areas of Optics Geometric Optics Light as a ray. Physical Optics Light as a wave. Quantum Optics Light as a particle.
 Mirrors that are formed from a section of a sphere.  Convex: The reflection takes place on the outer surface of the spherical shape  Concave: The.
Unit 11: Part 2 Mirrors and Lenses. Outline Plane Mirrors Spherical Mirrors Lenses The Lens Maker’s Equation Lens Aberrations.
Geometric Optics This chapter covers how images form when light bounces off mirrors and refracts through lenses. There are two different kinds of images:
 When light strikes the surface of an object  Some light is reflected  The rest is absorbed (and transferred into thermal energy)  Shiny objects,
Refraction and Lenses.
Chapter 36 Image Formation.
AP Physics IV.C Geometric Optics. Wave Fronts and Rays.
You should be able to: Draw ray diagrams for converging and diverging lenses Use the equation 1/u+1/v =1/f for converging lenses Perform.
1 32 Optical Images image formation reflection & refraction mirror & lens equations Human eye Spherical aberration Chromatic aberration.
Today’s agenda: Death Rays. You must know when to run from Death Rays. Refraction at Spherical Surfaces. You must be able to calculate properties of images.
Its now time to see the light…..  A lens is a curved transparent material that is smooth and regularly shaped so that when light strikes it, the light.
Magnification Amy Nau, O.D.
Physics 203/204 4: Geometric Optics Images formed by refraction Lens Makers Equation Thin lenses Combination of thin lenses Aberration Optical Instruments.
Dispersion The spreading of light into its color components is called dispersion. When light enters a prism, the refracted ray is bent towards the normal,
Chapter 27 Lenses and Optical Instruments. Lenses Converging lens Diverging lens.
Reflection at Mirrors and Curved Surfaces Amy C Nau, OD.
 Mirrors that are formed from a section of a sphere.  Convex: The reflection takes place on the outer surface of the spherical shape  Concave: The.
Physics 1202: Lecture 22 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, etc.
Mirrors.
GEOMETRICAL OPTICS. Laws of Reflection Laws of Refraction.
Chapter Reflection and Mirrors. Millions of light rays reflect from objects and enter our eyes – that’s how we see them! When we study the formation of.
Textbook sections 27-1 – 27-3 Physics 1161: Lecture 19 Lenses and your EYE Ciliary Muscles.
How Does a Lens Work? Light travels slower in the lens material than in the air around it. This means a linear light wave will be bent by the lens due.
Refraction and Lenses. Refraction is the bending of light as it moves from one medium to a medium with a different optical density. This bending occurs.
Refraction and Lenses. The most common application of refraction in science and technology is lenses. The kind of lenses we typically think of are made.
Basics Reflection Mirrors Plane mirrors Spherical mirrors Concave mirrors Convex mirrors Refraction Lenses Concave lenses Convex lenses.
Lenses Converging Lens Diverging Lens F F f f.
Spherical Thin Lenses Optics for Residents Amy Nau O.D., F.A.A.O.
Chapter 34 Geometric Optics © 2016 Pearson Education Inc.
Physics 2102 Jonathan Dowling Lecture 37: MON 20 APR Optics: Images.
Refraction at Spherical Surfaces.
Mirrors, Plane and Spherical Spherical Refracting Surfaces
Presentation transcript:

Optics for Residents Amy Nau O.D., F.A.A.O Spherical Thin Lenses Optics for Residents Amy Nau O.D., F.A.A.O

Spherical Lenses Formulas Thin lens formula 1/do+1/di=1/f F=1/f2 Linear Mag Image size/Object size= di/do Prentice’s Rule P=F (diopters) xd (cm)

Thin Spherical Lenses The shape of the refracting surface determines the type of lens and power Object space Image space Image space Object space C2 C2 C1 C1 A1 A2 A1 A2 Lens is thin if the thickness is small enough not to influence the power All refraction is thus considered to occur in one plane between the two surfaces A1 front surface vertex; A2 back surface vertex

Thin Lens Power F1=nlens-nobject/r and F2=nimage-nlens/r The total dioptric power of the lens (F) is F1+F2 By substitution, another way to write this is : F=(n’-n)/(1/r1-1/r2) This is called the Lens Makers Formula, and it assumes that the surrounding media is air.

Thin Lens Problem A plastic biconcave lens (n=1.49) has a surface radii of 40cm and 20 cm. Calculate the surface and total lens powers. Solve for F1 F1=nlens-nobject/r Solve for F2 F2=nimage-nlens/r Solve for total power F=F1+F2

Image Object Relationships: Position Assumptions: surrounding media is air Imaging occurs through single plane Formulas The Gaussian Imaging formula is used to calculate image-object power relationship L’=L+F F=total power of the lens Incident vergence (L)=no/l=ns/l=1.0/l (in air) Emergent vergence (L’)=ni/l’=ns/l’=1.0/l’(in air) Where l=object distance and l’=image distance

Object Image Relationships The types of images and objects as well as sign convention are the same as for single refracting surfaces object space Image space VIRTUAL OBJECTS REAL IMAGES REAL OBJECTS VIRTUAL IMAGES negative positive

Problem Virtual image is formed 25cm from a thin lens. If the object is real and positioned 50 cm from the lens, what is the lens power? L’=L+F

Image-Object Relationships Focal Points The primary and secondary focal points are calculated the same was as that for single curved surfaces. Assume the surrounding media is air (n=1) F=-n/f=n’/f’ becomes F=-1.0/f=1.0/f’ The equation shows that for thin lenses f=f’, but they are opposite signs

Focal Points Recall that an infinite axial object forms an image at f’ Recall that an object placed at f, forms an image at infinity

Secondary focal point – convex surface Object at infinity F’ f’ secondary focal length (+) Rays converge towards secondary focal point

Secondary focal point –concave surface Rays diverge as if they came from secondary focal point n n’ Secondary focal point F’ Object at infinity f’ secondary focal length (-)

Primary focal point The object position that yields the image at infinity Emergent vergence (L’) is zero

Primary focal point- positive surface F’ (infinity) f (primary focal length) f’ secondary focal length

Primary focal point – negative surface Infinite image rays c F’ F f primary focal length f’’ secondary focal length

Problem What are the primary and secondary focal lengths for a lens (n=1.49) with a power of -12D in air? F=-n/f F=n’/f’

Image-Object Relationships Size and Orientation This is LATERAL MAGNIFICATION and the ratio is image size/object size - invereted/+erect These equations are the basis for the lensometer LM=h’/h=nl’/n’l=nsl’/nsl=l’/l LM=-f/x=-x’/f’ (x= extrafocal dist) Where x=dist from primary focal point to object and x’=dist from seconary focal point to image Just as for single refracting surfaces, set up similar triangles!!!!!!!!!!!!!!!!!!!!!!

Lateral Magnification xx’=ff’ xx’=-f’f’ xx’=-(f)2 h F c c h’ l l’ x’ x f f’

Problem LM A real image moves to 5cm away from a lens when an object is moved from infinity to a position 40cm in front of the lens. What is the power of the lens? xx’=-(f)2

Distant Object Size tanw=h’/f=-h’/f’ h’=-f’tanw When an object is at an infinite distance, the LM cannot be determined. To solve for the object size use the chief ray tanw=h’/f=-h’/f’ h’=-f’tanw F’ h’ h’ F f f’

Who cares? The angular subtense of an object as it falls on the retina is used in vision to describe the size of a distant object. A 20/60 letter on an eye chart subtends a 15 minute arc at 20 feet (1 degree= 60 minutes).

Prismatic Effect of Thin Lenses The amount of bending after refraction is a function of the distance from the axis Closer to the axis bends less This is considered the prismatic effect of a lens The change in direction is the deviation Unlike a prism which has ONE deviation for any incident ray, a lens has an infinite number of deviations

Prismatic Effect of Thin Lenses d1 d2

Prismatic Effect of Thin Lenses THERE IS NO PRISMATIC EFFECT AT THE OC OF A LENS However, if the visual axis is not aligjed with the OC there is prism

Prismatic Effect of Thin Lenses The image always shifts Towards the APEX. Positive lenses displace Images opposite the direction Of decentration                         

Prismatic Effect of Thin Lenses Lens decentered downward = base up. In general, negative lenses displace images In the SAME direction as decentration.

Prismatic Effects The magnitude of prismatic deviation in prism diopters is expressed in terms of displacement (cm) and the secondary focal length (m) d=ycm/f’m = ycmFD

Prism Problem Patient with PD of 60mm is given a frame with a 70mm PD. If the pt’s Rx is -3.00D OU, what is the direction and amount of induced prism?

Effective Power Vergence (power) required for a lens at a new position to have the same effect on the incident rays. Becomes important if the distance between a lens and an image plane (retina) is changed. MOVING A LENS AWAY FROM THE IMAGE PLANE INCREASES POSITIVE POWER (DECREASES NEG. POWER)

Effective Power Fx=1/f’x=1/f’-d f’x Fx=F/1-dF p1 p2 screen This is the situation when You move a lens closer (i.e. glasses going to contact Lenses) F’ F’d Fx=1/f’x=1/f’-d Fx=F/1-dF f’x d d f’

Effective Power p1 p2 When the lens is moved AWAY, then less power Is required to put the image In the same place CLS to glasses OR need more bifocal power F’ f’ If lens is moved to the right d is positive, if lens is Moved right to left, d is neg d d f’x

Which soldier is taller?                                                                                                              

Is it moving and shimmering. Buy a poster Is it moving and shimmering?                                                                                                    Buy a poster! Look at this illusion for a while and it will appear to be shimmering and moving. Also: Follow the outermost groove and watch it change from a groove to a hump as you go around the wheel.

Problem Sets When rays from the sun pass through a convex lens, it makes a bright point image 0.7m behind the lens on the ground. What is the focal length of the lens? What is the nature of the image? What is the magnification? What is the power of the lens?

Problem Sets A light bulb is placed 300 cm from a convex lens with a focal length of 50 cm. Where is the image located? What is the nature of the image? What is the magnification of the image?

Problem Sets A light bulb is placed 300 cm from a convex lens with a focal length of 500 cm. Where is the image? What is the nature of the image? What is the magnification of the image?

Problem Sets A slide is placed 50mm from a projector lens and no image is formed. Why? An object of height 7cm is placed 25 cm in front of a thin converging lens with a focal length of 35 cm. What is the height, location and nature of the image?

Problem Sets Now the object is moved to 90 cm. What is the new image distance, height, and nature of the image?

Problem Sets A patient comes in having trouble with their new glasses which you prescribed. Their acuity is 20/20 in each eye and you determine that the refraction (-5.50 OD and -2.50+1.00X090 OS) is accurate. However, the patient reports that they glasses make them uncomfortable. You determine that the lenses have not been centered properly. They are decentered 2mm out on the OD and 2mm up on the OS. (how would you do that??). What is the induced prismatic effect?

Problem Sets A patient has a 10D exophoria at near. The patient needs a +2.00D reading add. What amount of prism would you prescribe? How much decentration needs to be added? In what direction is the base of the prism?

Problem Sets A patient with ARMD is having trouble reading. You determine that she needs a +4.50 add on top of her distance Rx of +1.00 OU to see the newspaper. How far away does she need to hold the paper to see it clearly? What will be the magnification of an object 10 cm tall held 5 cm from the lens?

Problem Sets An object 0.08 m high is placed 0.2m from a (+) lens. If the distance of the image from the lens is .40m, what is the height of the image? Diverging lenses form what kind of images?

Problem Sets An object is placed 0.2m from a lens with a focal length of 1.0m. How far from the lens will the image be formed?