Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 24: Optical Instruments Combinations.

Slides:



Advertisements
Similar presentations
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 23: Reflection and Refraction.
Advertisements

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 25: Interference and Diffraction.
5) Magnifying glass (Simple magnifier)
Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 15: Thermodynamics The First.
Week 3.
(c) McGraw Hill Ryerson Using Lenses to Form Images A lens is a piece of transparent material that can bend, or refract, light rays in useful.
Physics 1C Lecture 26C. Recap from last lecture Optical characteristics of lens are defined by focal length f: For a given f, imaging properties are given.
and Optical Instruments
Image Formation 2 Thin Lens Multi lens/mirror system
Ch. 18 Mirrors and Lenses Milbank High School. Sec Mirrors Objectives –Explain how concave, convex, and plane mirrors form images. –Locate images.
26.6 Lenses. Converging Lens Focal length of a converging lens is real and considered positive.
Homework Set 4: From “Seeing the Light” Chapter 3: (starting page 101) P9, P10, P11, PM3 From “Seeing the Light” Chapter 4: P2, P5, P7, P13 Due: Monday,
Lenses Physics 202 Professor Lee Carkner Lecture 21.
Copyright © 2009 Pearson Education, Inc. Lecture 2 – Geometrical Optics b) Thin Lenses.
PH 103 Dr. Cecilia Vogel Lecture 9. Review Outline  Multiple Lenses  application to microscope  and telescope  Lenses  more corrective lenses  application.
Photgraphic camera. How it works? Take a simple converging lens: Object – usually at a distance much, much larger from the lens than its focal length Lens.
Lecture 17 Ray Optics-3 Chapter 23 PHYSICS 270 Dennis Papadopoulos March 22, 2010.
LENSES.
Lenses Physics 202 Professor Lee Carkner Lecture 23.
Refraction (bending light) Refraction is when light bends as it passes from one medium into another. When light traveling through air passes into the glass.
Converging lenses Diverging Lenses The Lens Equation We can make use of the fact that changing the focal length and position of the object we can change.
Application of Lenses Lenses in Eyes
Thin Lenses.
Chapter 25 Optical Instruments 1. The eye 2. The magnifying glass.
Lecture 14 Images Chp. 35 Opening Demo Topics –Plane mirror, Two parallel mirrors, Two plane mirrors at right angles –Spherical mirror/Plane mirror comparison.
A. can be focused on a screen. B. can be projected on a wall.
Chapter 18 Mirrors and Lenses Lenses A. Types of Lenses A. Types of Lenses B. Convex Lenses B. Convex Lenses C. Concave Lenses C. Concave Lenses.
(c) McGraw Hill Ryerson Extending Human Vision Microscopes A compound light microscope uses two convex lenses to magnify small, close objects.
Chapter 14 Section 2 Thin lenses.
Chapter 34 Lecture Eight: Images: II. Image Formed by a Thin Lens A thin lens is one whose thickness is small compared to the radii of curvature For a.
Extending Human Vision. Microscopes (c) McGraw Hill Ryerson 2007  A compound light microscope uses two convex lenses to magnify small, close objects.
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.
Lesson 25 Lenses Eleanor Roosevelt High School Chin-Sung Lin.
OPTICAL INSTRUMENTS PRESENTED BY P.R. PARTHIBAN J. KRISHNA MOORTHY R. RAJA SEKHAR D.SATHISH KUMAR P. RAJESH GUIDED BY B. RAVINDRANATH.
Lesson 6 – Microscope and telescope
SEEING THROUGH A LENS.  We see the world through lenses.  Eye glasses = lenses. Contact lenses = lenses.  Magnifying glasses = lenses. Microscopes.
Thin Lens Optics Physics 11. Thin Lens Optics If we have a lens that has a small diameter when compared to the focal length, we can use geometrical optics.
Lecture 18 Optical Instruments
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.
Physics 203/204 4: Geometric Optics Images formed by refraction Lens Makers Equation Thin lenses Combination of thin lenses Aberration Optical Instruments.
Converging Lenses & Their Application Dan Li SUNY-Stony Brook 11/07/2002.
Lens Application Camera Movie Projector Magnifying Glass
Chapter 18 Mirrors and Lenses. Objectives 18.1 Explain how concave, convex, and plane mirrors form images 18.1 Locate images using ray diagrams, and calculate.
2/15/16Oregon State University PH 212, Class #191 The Compound Microscope Of course, we can use more than one external lens to create the en- larged image.
2/8/16Oregon State University PH 212, Class #161 The Thin-Lens Equation The thin lens approximation holds for a lens whose thick- ness is small compared.
SEEING THROUGH A LENS.  We see the world through lenses.  Eye glasses = lenses. Contact lenses = lenses.  Magnifying glasses = lenses. Microscopes.
OPTICAL INSTRUMENTS PRESENTED BY: 1. ANA ALINA 2. FIRDIANA SANJAYA.
Mirrors. Types of mirror There are two types of mirror Plane (flat) Curved Concave (curves in) Convex (curves out)
Chapter 33 Lenses and Optical Instruments The Thin Lens Equation; Magnification Example 33-2: Image formed by converging lens. What are (a) the.
Refraction. Refraction of Light When light waves pass from one medium to the next, its speed changes, causing it to bend. Going from lower to higher index.
Chapter 33 Lenses and Optical Instruments
Ch. 30 Lenses.
Lenses & Optical Instruments
Ch.13 Applications (應用) of Convex Lenses
Chapter 24: Optical Instruments
Refraction at Spherical Surfaces.
15/11/2018 Lenses.
13.4 The Lens Equation.
Chapter 3 Image Slides Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Refraction at Spherical Surfaces.
14-2 Thin lenses.
5.3 Using Lenses to Form Images
5.3 Using Lenses to Form Images
Convex and Concave Lenses
Lenses 2: Thin Lens Equation
5.3 Using Lenses to Form Images
Lens Equations.
Thin Lens Equation 1
(c) McGraw Hill Ryerson 2007
5.3 Using Lenses to Form Images
Presentation transcript:

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 1 Chapter 24: Optical Instruments Combinations of Lenses The Camera The Eye The Magnifier The Compound Microscope The Telescope

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 2 §24.1 Combinations of Lenses With lenses in combination, the image formed by one lens is the object for the next lens.

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 3 The thin lens equation still applies. p is the object distance, q is the image distance, f is the focal length and s is the distance between the lenses. It is possible to have the object for the second lens be virtual (p 2 <0); here the image formed by the first lens is beyond the second lens.

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 4 The magnification of a combination of lenses is just the product of the magnifications for the individual lenses.

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 5 Example (text problem 24.2): A converging and diverging lens, separated by a distance of 30.0 cm, are used in combination. The converging lens has f 1 = 15.0 cm and the diverging lens has an unknown focal length. An object is placed at 20.0 cm in front of the converging lens; the final image is virtual and is formed 12.0 cm before the diverging lens. What is the focal length of the diverging lens? Given: p 1 = 20 cm; f 1 = 15 cm. Find that q 1 = 60 cm Given: s = 30.0 cm. Find that p 2 = -30 cm. Given: q 2 = -12 cm and p 2 = -30 cm. Find that f 2 = -8.6 cm.

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 6 §24.2 The Camera A camera forms a real, inverted image. For far away objects, the film must be placed one focal length from the lens.

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 7 Example (text problem 24.17): A person on safari wants to take a photograph of a hippopotamus from a distance of 75.0 m. The animal is 4.00 m long and its image is to be 1.20 cm long on the film. (a) What focal length lens should be used? Now use the thin lens equation

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 8 (b) What would be the size of the image if a lens of 50.0 mm focal length were used? The object is 2.67 mm long (inverted). Example continued:

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 9 §24.3 The Eye The lens is at a fixed distance from the retina (unlike in some cameras where this is adjustable). The lens has a variable focal length, which is adjusted to keep the image distance (q) constant as the object distance (p) varies.

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 10 The near point is the closest distance from your eye that an object can be seen clearly. For a normal eye this distance is 25 cm. Refractive power of a lens is defined as: The far point is farthest distance from your eye that an object can be seen clearly. For a normal eye this distance is . where f is the focal length of the lens; typical units of P are diopters (1D = 1 m -1 ).

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 11 For a near sighted (myopic) person, light rays converge before they strike the retina. A diverging lens is placed in the light path. This creates a virtual image closer to your eye than the actual object is.

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 12 For a far sighted (hyperopic) person, light rays converge after they strike the retina. A converging lens is placed in the light path. This creates a virtual image farther from your eye than the actual object is.

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 13 Example (text problem 24.63): If Harry has a near point of 1.5 m, what focal length contact lenses does he require? The near point refers to the closest distance an object can be to see it clearly, in this case 1.5 m. A normal eye has a near point of 25 cm. These corrective lenses must take an object at 25 cm and form a virtual image at a distance of 1.5 m. Given p = 25 cm; q = -1.5m. Here f = cm The refractive power of these lenses is (Diopter) Harry is farsighted.

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 14 §24.4 The Magnifier For an object to look bigger the image of it formed on the retina must be made bigger. The farther an object is from your eye, the smaller it will look.

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 15 Using the triangles in the figure, the angular size  of an object is:

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 16 The angular magnification is The largest angular size an object can have and still be seen clearly is when it is placed at your near point. Now the object is placed at the focal point of a converging lens

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 17 N is the near point for a person (typically 25 cm) and f is the focal length of the lens used in the magnifier.

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 18 Example (text problem 24.34): An insect that is 5.00 mm long is placed 10.0 cm from a converging lens with a focal length of 12.0 cm. (a) What is the position of the image? Given: p = 10.0 cm and f = 12.0 cm. Find that q = cm; on the same side of the lens as the insect.

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 19 (b) What is the size of the image? (c) Is the image upright or inverted? Since h’>0, the image is upright. Example continued:

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 20 (d) Is the image real or virtual? Since q<0 (the image forms on the same side of the lens as the object), the image is virtual. (e) What is the angular magnification if the lens is close to the eye? Object is at a distance of p, not f from the lens. Example continued:

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 21 §24.5 The Compound Microscope The objective lens forms an enlarged real image here. Two converging lenses are used to produce a highly magnified image. The eyepiece is used to view this image.

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 22 The eyepiece is used as a magnifier; the image formed by the objective is placed at the focal point of the eyepiece. The total magnification is the product of the individual magnifications: where L = “tube length” = q 0 - f 0 ; N = near point distance; and f obj & f eye are focal lengths of the objective and eyepiece respectively.

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 23 Example (text problem 24.42): A microscope has an objective lens of focal length 5.00 mm. The objective forms an image 16.5 cm from the lens. The focal length of the eyepiece is 2.80 cm. (a) What is the distance between the lenses? Using figure 24.16, the distance between the lenses is d = f eye + q o = 2.80 cm cm = 19.3 cm.

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 24 (b) What is the angular magnification? The near point is 25.0 cm. (c) How far from the objective should the object be placed? Given: q = 16.5 cm and f = 0.5 cm. Find that p = 0.52 cm. Example continued:

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 25 §24.6 The Telescope A telescope is a combination of lenses and/or mirrors used to collect a large amount of light and bring it to a focus.

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 26 A refracting telescope (or refractor) uses lens. The barrel (or tube) length is The angular magnification is

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 27 Light path of a Cassegrain telescope: A reflecting telescope uses mirrors (and lenses).

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 28 Example (text problem 24.49): A refracting telescope is used to view the moon (diameter of 3474 km & distance from Earth 384,500 km). The focal lengths of the objective and eyepiece are m and cm, respectively. (a) What should be the distance between the lenses?

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 29 (b) What is the diameter of the image produced by the objective? (c) What is the angular magnification? Example continued:

Fisica Generale - Alan Giambattista, Betty McCarty Richardson Copyright © 2008 – The McGraw-Hill Companies s.r.l. 30 Summary Combinations of Lens The Camera The Eye The Magnifier The Compound Microscope The Telescope