Chapter 35 - Refraction. A PowerPoint Presentation by Paul E. Tippens, Professor of Physics Southern Polytechnic State University

Similar documents
Chapter 35 - Refraction

INF-GEO Solutions, Geometrical Optics, Part 1

Ray Optics Theory and Mode Theory. Dr. Mohammad Faisal Dept. of EEE, BUET

REFLECTION AND REFRACTION

Lesson 8 Refraction of Light

Section 19. Dispersing Prisms

Section 19. Dispersing Prisms

Physics 30 Lesson 8 Refraction of Light

REFLECTION AND REFRACTION

(A sequence also can be thought of as the list of function values attained for a function f :ℵ X, where f (n) = x n for n 1.) x 1 x N +k x N +4 x 3

Section 1.1. Calculus: Areas And Tangents. Difference Equations to Differential Equations

Chapter 35 Solutons. = m/s = Mm/s. = 2( km)(1000 m/km) (22.0 min)(60.0 s/min)

EDEXCEL NATIONAL CERTIFICATE UNIT 4 MATHEMATICS FOR TECHNICIANS OUTCOME 4 - CALCULUS

CALCULUS BASIC SUMMER REVIEW

Ray-triangle intersection

SNAP Centre Workshop. Basic Algebraic Manipulation

Chapter 1. Complex Numbers. Dr. Pulak Sahoo

CALCULATION OF FIBONACCI VECTORS

PHYS 450 Spring semester Lecture 06: Dispersion and the Prism Spectrometer. Ron Reifenberger Birck Nanotechnology Center Purdue University

A sequence of numbers is a function whose domain is the positive integers. We can see that the sequence

Name Date PRECALCULUS SUMMER PACKET

Complex Numbers Solutions

Ma 530 Introduction to Power Series

Orthogonal transformations

Recurrence Relations

We will conclude the chapter with the study a few methods and techniques which are useful

Chapter 4. Fourier Series

The Scattering Matrix

Quadratic Functions. Before we start looking at polynomials, we should know some common terminology.

Optics. n n. sin. 1. law of rectilinear propagation 2. law of reflection = 3. law of refraction

Sequences A sequence of numbers is a function whose domain is the positive integers. We can see that the sequence

U8L1: Sec Equations of Lines in R 2

Lesson 10: Limits and Continuity

Question 1: The magnetic case

6.003 Homework #3 Solutions

Ma 530 Infinite Series I

10.2 Infinite Series Contemporary Calculus 1

R is a scalar defined as follows:

Lecture # 07: Flow Visualization techniques: Shadowgraph and Schlieren

Quiz No. 1. ln n n. 1. Define: an infinite sequence A function whose domain is N 2. Define: a convergent sequence A sequence that has a limit

September 2012 C1 Note. C1 Notes (Edexcel) Copyright - For AS, A2 notes and IGCSE / GCSE worksheets 1

U8L1: Sec Equations of Lines in R 2

Introduction to Signals and Systems, Part V: Lecture Summary

Math 312 Lecture Notes One Dimensional Maps

Apply change-of-basis formula to rewrite x as a linear combination of eigenvectors v j.

Statistics 511 Additional Materials

Infinite Sequences and Series

MTH Assignment 1 : Real Numbers, Sequences

Problem 4: Evaluate ( k ) by negating (actually un-negating) its upper index. Binomial coefficient

CHAPTER 10 INFINITE SEQUENCES AND SERIES

6 Integers Modulo n. integer k can be written as k = qn + r, with q,r, 0 r b. So any integer.

Section 11.8: Power Series

ENGI 4421 Probability and Statistics Faculty of Engineering and Applied Science Problem Set 1 Solutions Descriptive Statistics. None at all!

Section 7 Fundamentals of Sequences and Series

Expectation and Variance of a random variable

MATH301 Real Analysis (2008 Fall) Tutorial Note #7. k=1 f k (x) converges pointwise to S(x) on E if and

Curve Sketching Handout #5 Topic Interpretation Rational Functions

PROPERTIES OF SQUARES

The Michelson Interferometer

Machine Learning for Data Science (CS 4786)

Lecture #20. n ( x p i )1/p = max

Summary: CORRELATION & LINEAR REGRESSION. GC. Students are advised to refer to lecture notes for the GC operations to obtain scatter diagram.

SECTION 2 Electrostatics

CHAPTER 8 SYSTEMS OF PARTICLES

Lecture 6 Chi Square Distribution (χ 2 ) and Least Squares Fitting

A second look at separation of variables

ECE Spring Prof. David R. Jackson ECE Dept. Notes 20

UNIVERSITY OF NORTHERN COLORADO MATHEMATICS CONTEST. First Round For all Colorado Students Grades 7-12 November 3, 2007

Vector Quantization: a Limiting Case of EM

RADICAL EXPRESSION. If a and x are real numbers and n is a positive integer, then x is an. n th root theorems: Example 1 Simplify

arxiv:physics/ v1 [physics.pop-ph] 29 Mar 2005

If the escalator stayed stationary, Billy would be able to ascend or descend in = 30 seconds. Thus, Billy can climb = 8 steps in one second.

Types of Waves Transverse Shear. Waves. The Wave Equation

APPENDIX F Complex Numbers

mx bx kx F t. dt IR I LI V t, Q LQ RQ V t,

Goodness-of-Fit Tests and Categorical Data Analysis (Devore Chapter Fourteen)

Assignment 1 : Real Numbers, Sequences. for n 1. Show that (x n ) converges. Further, by observing that x n+2 + x n+1

Analysis Methods for Slab Waveguides

CALCULATING FIBONACCI VECTORS

Lecture 6 Chi Square Distribution (χ 2 ) and Least Squares Fitting

Scattering at an Interface:

3.2 Properties of Division 3.3 Zeros of Polynomials 3.4 Complex and Rational Zeros of Polynomials

Linearly Independent Sets, Bases. Review. Remarks. A set of vectors,,, in a vector space is said to be linearly independent if the vector equation

Salmon: Lectures on partial differential equations. 3. First-order linear equations as the limiting case of second-order equations

Math 21B-B - Homework Set 2

Math 10A final exam, December 16, 2016

TEACHER CERTIFICATION STUDY GUIDE

ANSWERS SOLUTIONS iiii i. and 1. Thus, we have. i i i. i, A.

The Growth of Functions. Theoretical Supplement

The Method of Least Squares. To understand least squares fitting of data.

Zeros of Polynomials

FLC Ch 8 & 9. Evaluate. Check work. a) b) c) d) e) f) g) h) i) j) k) l) m) n) o) 3. p) q) r) s) t) 3.

Math E-21b Spring 2018 Homework #2

Solutions. tan 2 θ(tan 2 θ + 1) = cot6 θ,

CEE 522 Autumn Uncertainty Concepts for Geotechnical Engineering

ARITHMETIC PROGRESSIONS

SECTION 1.5 : SUMMATION NOTATION + WORK WITH SEQUENCES

10.6 ALTERNATING SERIES

MID-YEAR EXAMINATION 2018 H2 MATHEMATICS 9758/01. Paper 1 JUNE 2018

Unit 6: Sequences and Series

Transcription:

Chapter 35 - Refractio A PowerPoit Presetatio by Paul E. Tippes, Professor of Physics Souther Polytechic State Uiersity 2007

Objecties: After completig this module, you should be able to: Defie ad apply the cocept of the idex of refractio ad discuss its effect o the elocity ad waelegth of light. Apply Sell s s law to the solutio of problems iolig the refractio of light. Determie the chages i elocity ad/or waelegth of light after refractio. Defie ad apply the cocepts of total iteral reflectio ad the critical agle of icidece.

Refractio Refractio is is the bedig of of light as it it passes from oe medium ito aother. Note: the agle of icidece A i air ad the agle of refractio A i water are each measured with the ormal N. A w N Water refractio The icidet ad refracted rays lie i i the same plae ad are reersible.

Refractio Distorts Visio Water Water The eye, belieig that light traels i i straight lies, sees objects closer to to the surface due to to refractio. Such distortios are commo.

The Idex of Refractio The idex of of refractio for a material is is the ratio of of the elocity of of light i i a acuum (3 x 10 8 m/s) to to the elocity through the material. Idex of refractio c c c Examples: = 1; 1; glass = 1.5; Water = 1.33

Example 1. Light traels from air ( ( = 1) ) ito glass, where its elocity reduces to oly 2 x 10 8 m/s. What is the idex of refractio for glass? air = c Glass G = 2 x 10 8 m/s c 8 3 x 10 m/s 8 2 x 10 m/s For glass: = 1.50 If the medium were water: W = 1.33.. The you should show that the elocity i water would be reduced from c to 2.26 x 10 8 m/s.

Aalogy for Refractio 3 x 10 8 m/s Paemet Glass 2 x 10 8 m/s Sad s < p 3 x 10 8 m/s Light beds ito glass the returs alog origial path much as a rollig axle would whe ecouterig a strip of of mud.

Deriig Sell s s Law Cosider two light rays. Velocities are 1 i medium 1 ad 2 i med. 2. Segmet R is commo hypoteuse to two rgt. triagles. Verify show agles from geometry. si t R ; si t R 1 2 1 2 1 Medium 2 2 t 1 2 R Medium 1 1 t t si R si t R 1 1 1 2 2 2

Sell s s Law Medium 1 1 2 1 Medium 2 2 The ratio of of the sie of of the agle of of icidece 1 to to the sie of of the agle of of refractio 2 is is equal to to the ratio of of the icidet elocity 11 to to the refracted elocity 22. Sell s Law: si si 1 1 2 2

Example 2: A laser beam i a darkeed room strikes the surface of water at a agle of 30 0. The elocity i water is 2.26 x 10 8 m/s. What is the agle of refractio? 30 0 A The icidet agle is: A = 90 0 30 0 = 60 0 H 2 O W si A si W A W 8 0 W si A (2 x 10 m/s)si 60 siw W = 35.3 0 A 8 3 x 10 m/s

Sell s s Law ad Refractie Idex Aother form of Sell s s law ca be deried from the defiitio of the idex of refractio: 1 Medium 1 2 Medium 2 c from which c ; c 1 1 1 2 2 2 1 2 c Sell s s law for elocities ad idices: si si 1 1 2 2 2 1

A Simplified Form of the Law Sice the idices of refractio for may commo substaces are usually aailable, Sell s s law is ofte writte i the followig maer: si si 1 1 2 2 2 1 si si 1 1 2 2 The product of of the idex of of refractio ad the sie of of the agle is is the same i i the refracted medium as for the icidet medium.

Example 3. Light traels through a block of glass, the remerges ito air. Fid agle of emergece for gie iformatio. First fid G iside glass: 50 0 Glass G G =1.5 si si A A G G Asi A (1.0)si 50 sig 1.50 G G = 30.7 0 0 From geometry, ote agle G same for ext iterface. Apply to e each iterface: = 50 0 Same Asi A GsiG Asi as etrace agle! A

Waelegth ad Refractio The eergy of light is determied by the frequecy of the EM waes, which remais costat as light passes ito ad out of a medium. (Recall = f.) f Glass =1 A =1.5 G f A = f G G A f ; f A A A G G G A fa A A ; ; f G G G G si si 1 1 1 2 2 2

The May Forms of Sell s s Law: Refractio is is affected by the idex of of refractio, the elocity, ad the waelegth. I geeral: Sell s Law: si si 1 2 1 1 2 1 2 2 All the ratios are equal. It It is is helpful to to recogize that oly the idex differs i i the ratio order.

Example 4: A helium eo laser emits a beam of waelegth 632 m i air (( A = 1). 1 What is the waelegth iside a slab of glass ( ( G = 1.5)? Glass G G =1.5 G = 1.5; A = 632 m A G AA ; G G A G G (1.0)(632 m) 1.5 421 m Note that the light, if see iside the glass, would be blue.. Of course it still appears red because it returs to air before strikig the eye.

Dispersio by a Prism Red Orage Yellow Gree Blue Idigo Violet Dispersio is is the separatio of of white light ito its arious spectral compoets. The colors are refracted at at differet agles due to to the differet idexes of of refractio.

Total Iteral Reflectio Whe light passes at a agle from a medium of higher idex to oe of lower idex, the emergig ray beds away from the ormal. light c 90 0 Critical agle i = r Water Whe the agle reaches a certai maximum, it will be reflected iterally. The critical agle c is is the limitig agle of of icidece i i a deser medium that results i i a agle of of refractio equal to to 90 0.

Example 5. Fid the critical agle of icidece from water to air. For critical agle, A = 90 0 A = 1.0; W = 1.33 si si W C A A A sic 0 si 90 (1)(1) w 1.33 Critical agle Critical agle: c = 48.8 0 Water c 90 0 I geeral, for media where 1 > 2 we fid that: si C 1 2

Summary Medium c = 3 x 10 8 m/s Idex of refractio c Refractio is is affected by the idex of of refractio, the elocity, ad the waelegth. I geeral: Sell s Law: si si 1 2 1 1 2 1 2 2

Summary (Cot.) The critical agle c is is the limitig agle of of icidece i i a deser medium that results i i a agle of of refractio equal to to 90 0. Critical agle 2 c 90 0 1 1 > 2 I geeral, for media where 1 > 2 we fid that: si C 1 2

CONCLUSION: Chapter 35 Refractio