Study Guide Physics C1402(001) Final Prof. H. Evans. Monday, May 7 1:00-4:00 pm Room 309, Havemeyer

Similar documents
Louisiana State University Physics 2102, Exam 3 April 2nd, 2009.

Describe the forces and torques exerted on an electric dipole in a field.

Welcome to PHY2054C. Office hours: MoTuWeTh 10:00-11:00am (and after class) at PS140

Physics 208, Spring 2016 Exam #3

Where k = 1. The electric field produced by a point charge is given by

Physics GRE: Electromagnetism. G. J. Loges 1. University of Rochester Dept. of Physics & Astronomy. xkcd.com/567/

LC circuit: Energy stored. This lecture reviews some but not all of the material that will be on the final exam that covers in Chapters

2426 Required Topics (May 4, 2012 draft) Halliday, FUNDAMENTALS OF PHYSICS, 9e Required topics are in bold text. Optional topics are in normal text.

Final on December Physics 106 R. Schad. 3e 4e 5c 6d 7c 8d 9b 10e 11d 12e 13d 14d 15b 16d 17b 18b 19c 20a

SUMMARY Phys 2523 (University Physics II) Compiled by Prof. Erickson. F e (r )=q E(r ) dq r 2 ˆr = k e E = V. V (r )=k e r = k q i. r i r.

Physics 2102 Gabriela González. Marathon review of the course: 15 weeks in ~60 minutes!

Louisiana State University Physics 2102, Exam 2, March 5th, 2009.

AP Physics C. Magnetism - Term 4

Yell if you have any questions

Yell if you have any questions

Name (Last, First): You may use only scientific or graphing calculators. In particular you may not use the calculator app on your phone or tablet!

Exam 3 Topics. Displacement Current Poynting Vector. Faraday s Law Self Inductance. Circuits. Energy Stored in Inductor/Magnetic Field

Exam 4 Solutions. a. 1,2,and 3 b. 1 and 2, not 3 c. 1 and 3, not 2 d. 2 and 3, not 1 e. only 2

Electrical polarization. Figure 19-5 [1]

Outline of College Physics OpenStax Book

On my honor, I have neither given nor received unauthorized aid on this examination.

Chapter 31: Electromagnetic Induction and Faraday s Law All sections covered.

SUGGESTED LESSON PLANS FOR PHY 097 SEMESTER NOV10 Text Book : PHYSICS FOR SCIENTISTS & ENGINEERS WITH MODERN PHYSICS BY GIANCOLI, FOURTH EDITION

Chapter 1: Electrostatics

AP Physics C Mechanics Objectives

AP Physics C. Electricity - Term 3

Yell if you have any questions

Exam 2 Solutions. Note that there are several variations of some problems, indicated by choices in parentheses.

we can said that matter can be regarded as composed of three kinds of elementary particles; proton, neutron (no charge), and electron.

AP Physics C Electricity and Magnetism

Name (Print): 4 Digit ID: Section:

Principles of Physics II

Part 4: Electromagnetism. 4.1: Induction. A. Faraday's Law. The magnetic flux through a loop of wire is

Physics Lecture 40: FRI3 DEC

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Spring 2014 Final Exam Equation Sheet. B( r) = µ o 4π

CHAPTER 7 ELECTRODYNAMICS

Mansfield Independent School District AP Physics C: Electricity and Magnetism Year at a Glance

Physics 208 Final Exam

Solutions to PHY2049 Exam 2 (Nov. 3, 2017)

PHYS 272 (Spring 2018): Introductory Physics: Fields Homeworks

PHYSICS PHYSICS FOR SCIENTISTS AND ENGINEERS. Course Outline - Spring 2009

n Higher Physics 1B (Special) (PHYS1241) (6UOC) n Advanced Science n Double Degree (Science/Engineering) n Credit or higher in Physics 1A

On my honor, I have neither given nor received unauthorized aid on this examination.

CBSE 12th Physics 2016 Unsolved Paper Delhi Board ARYAN INSTITUTE

On my honor, I have neither given nor received unauthorized aid on this examination.

AP Physics C. Electricity and Magne4sm Review

Physics Jonathan Dowling. Final Exam Review

Electromagnetic Induction Faraday s Law Lenz s Law Self-Inductance RL Circuits Energy in a Magnetic Field Mutual Inductance

cancel each other out. Thus, we only need to consider magnetic field produced by wire carrying current 2.

PHYS 1444 Section 004 Lecture #22

fiziks Institute for NET/JRF, GATE, IIT-JAM, JEST, TIFR and GRE in PHYSICAL SCIENCES

Physics Will Farmer. May 5, Physics 1120 Contents 2

University of the Philippines College of Science PHYSICS 72. Summer Second Long Problem Set

Profs. P. Avery, A. Rinzler, S. Hershfield. Final Exam Solution

Physics Lecture 01: MON 25 AUG

Physics Final. Last Name First Name Student Number Signature

Physics 112. Study Notes for Exam II

PHY2049 Fall11. Final Exam Solutions (1) 700 N (2) 350 N (3) 810 N (4) 405 N (5) 0 N

b) (4) How large is the current through the 2.00 Ω resistor, and in which direction?

Chapter wise Theoretical Important Questions in Physics for Class-XII

Exam 4 (Final) Solutions

Final Exam: Physics Spring, 2017 May 8, 2017 Version 01

r r 1 r r 1 2 = q 1 p = qd and it points from the negative charge to the positive charge.

Final Exam Concept Map

Chapter wise Theoretical Important Questions in Physics for. Class-XII. Electrostatics

Exam 2 Solutions. ε 3. ε 1. Problem 1

Impedance/Reactance Problems

University of Colorado at Boulder Summer 2017, Session B Tuesday, July 11 - Friday, August 11. Prof. Mik Sawicki PHYS 1120 COURSE CALENDAR WEEK 1

/20 /20 /20 /60. Dr. Galeazzi PHY207 Test #3 November 20, I.D. number:

Physics 420 Fall 2004 Quiz 1 Wednesday This quiz is worth 6 points. Be sure to show your work and label your final answers.

Physics / Higher Physics 1A. Electricity and Magnetism Revision

Waves. Decibels. Chapter 21: Dimension

PHYSICS Course Structure Units Topics Marks Electrostatics Current Electricity III Magnetic Effect of Current & Magnetism

Calculus Relationships in AP Physics C: Electricity and Magnetism

Review. Spring Semester /21/14. Physics for Scientists & Engineers 2 1

PHY 112 GENERAL PHYSICS II WITH LAB

Maxwell s equations and EM waves. From previous Lecture Time dependent fields and Faraday s Law

Physics for Scientists and Engineers 4th Edition 2017

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics: Final Exam Review Session Problems Solutions

EXAM 3: SOLUTIONS. B = B. A 2 = BA 2 cos 0 o = BA 2. =Φ(2) B A 2 = A 1 cos 60 o = A 1 2 =0.5m2

Exam 3 November 19, 2012 Instructor: Timothy Martin

CBSE PHYSICS QUESTION PAPER (2005)

Physics 2020 Exam 2 Constants and Formulae

UNIT I ELECTROSTATIC FIELDS

Exam 2 Fall 2014

DEHRADUN PUBLIC SCHOOL I TERM ASSIGNMENT SUBJECT- PHYSICS (042) CLASS -XII

Gen. Phys. II Exam 2 - Chs. 21,22,23 - Circuits, Magnetism, EM Induction Mar. 5, 2018

10/11/2018 1:48 PM Approved (Changed Course) PHYS 42 Course Outline as of Fall 2017

Exam 2, Phy 2049, Spring Solutions:

5) Ohm s Law gives the relationship between potential difference and current for a.

Profs. Y. Takano, P. Avery, S. Hershfield. Final Exam Solution

Circuits Capacitance of a parallel-plate capacitor : C = κ ε o A / d. (ρ = resistivity, L = length, A = cross-sectional area) Resistance : R = ρ L / A

Physics For Scientists and Engineers A Strategic Approach 3 rd Edition, AP Edition, 2013 Knight

Name Final Exam May 1, 2017

COWLEY COLLEGE & Area Vocational Technical School

A) n 1 > n 2 > n 3 B) n 1 > n 3 > n 2 C) n 2 > n 1 > n 3 D) n 2 > n 3 > n 1 E) n 3 > n 1 > n 2

PHY102 Electricity Course Summary

Physics 227 Final Exam Wednesday, May 9, Code: 000

NEW HORIZON PRE UNIVERSITY COLLEGE LESSON PLAN FOR THE ACADEMIC YEAR Department of PHYSICS (II PUC)

Physics 240 Fall 2005: Exam #3 Solutions. Please print your name: Please list your discussion section number: Please list your discussion instructor:

Transcription:

Study Guide Physics C1402(001) Final Prof. H. Evans Monday, May 7 1:00-4:00 pm Room 309, Havemeyer (ver.1) http://www.nevis.columbia.edu/~evans/c1402/pdf/f_guide.pdf MATERIAL COVERED Concepts in Halliday, Resnick and Walker, Chapters 22-37! There will be 6 questions on the exam! The approximate breakdown of the questions will be: Half covering Chapters 22-33 (midterms 1 & 2) Half covering Chapters 34-37 (after midterm 2) Questions will be based on material covered in:! Lectures! Problems in the Homework! Sections of the Text not touched on in Lectures or Homework will not be included in the exam. Question Format:! Questions will be very similar to the homework WHAT TO BRING The exam will be closed book, but You will be allowed to use one 8½ x 11 note sheet! You may use both sides of the note sheet! The notes must be in your handwriting No photocopies! You may include anything you want on the note sheet (formulas, example problems, graphs, inspirational poetry )! You will be asked to hand in your note sheet with your exam, so put your name on it The note sheet will not be graded, but Failure to hand in your note sheet will cost you points Remember to bring a calculator I will provide all necessary:! constants! unit conversions and prefixes (nano, pico, etc.) 1

GENERAL ADVICE Studying for the Exam! Do all the homework problems and understand the solutions.! Review your lecture notes.! Have a look at the Questions at the end of each chapter. If you find that you have problems with groups of them you should concentrate on understanding those areas. Exam-Taking Strategies! Before beginning the exam read over all the problems.! Before doing a problem read it carefully so you don t miss anything.! Start with the easiest problem.! If you get stuck don t waste time. Go on to another problem.! Write legibly. If the grader can t read your solution he/she can t grade it.! Show your work. No work = no partial credit.! Draw detailed pictures - this can indicate to the grader that you understand the concept of the problem even if you don't do the math correctly.! Solve problems algebraically before plugging in numbers.! Check your answers for correct units and reasonable values.! Don t worry if you can t do everything. Grading will be on a curve. Time Budgeting! Do not allow yourself to miss out on points by wasting all your time on one problem.! Make a time budget at the beginning of the exam and stick carefully to it!! For a 3-hour exam with 6 questions a sample budget could be: 10 min Read over all problems and decide the order to do them. 25 min Spend this amount of time on each problem. When a problem's time is up, stop, and go to the next one. 20 min Check over your work and revisit any parts you couldn't do. Partial Credit. How to make sure you get it.! Show your work. You will not get credit if you simply write down the correct answer.! Draw a diagram of the problem with forces and a coordinate system. A well drawn diagram will be worth points. No diagram will make it difficult for the grader to give partial credit.! Show clearly the steps you have taken in attempting to solve the problem. If the grader can t follow your reasoning you won t get much credit.! Include units in your answers. Points will be taken off for answers without units.! Use appropriate significant digits Points will be taken off for answers that have many (3-4) more significant digits than the information given. 2

Key Concepts UNITS Always include units in answers! Know common units! V = J/C, A = C/s, etc. Be able to convert back and forth between different units VECTORS Difference between Vectors and Scalars! Vector = magnitude and direction (at least two numbers)! Scalar = number with sign Vector Representation! Cartesian: v = v x i + v y j + v z k Unit vectors! Polar: v = magnitude(v) and angle(θ)! Calculating components of vectors along coordinate axes Adding and Subtracting Vectors Multiplying Vectors! Dot Product: c = a b = ab cosθ! Cross Product: c = a b c = ab sinθ Direction of c from Right-Hand-Rule ELECTRIC FORCES & FIELDS Charge is quantized:! e = 1.60 10 19 C Electrostatic Force and Coulomb s Law: r kq1q 2! F = rˆ r 2 Electric Fields: E = F/q o! Be able to calculate Forces from Fields and vice versa Draw Field Lines for Simple Configurations of Charge! small numbers of discrete charges! simple continuous charge distributions: lines, planes, spheres, cylinders Simple applications of Coulomb s Law for E-Fields! no complicated integrals Electric Dipoles! field configuration! dipole moment: p = qd! torque in an external field: τ = p E! energy in an external field: U = p E 3

On exam calculate Electric Fields using two methods:! 1) Superposition of E-Fields apply this to find total fields for systems where you know the fields separately for each of the components! 2) Gauss Law only appropriate when there is strong symmetry Electric Flux: dφ = E da! understand meaning of flux (field lines per area)! direction of area element da Gauss Law: surf E da = q enc /ε o! find E for simple shapes: 1) points, spheres 2) lines, cylinders 3) planes! use superposition to find field for combinations! understand consequences of special cases: q enc = 0 E = 0 on surface! General Steps for Solving Gauss Law Problems 1) Use symmetry to get: > a) direction of E-Field vectors > b) surfaces where E is constant 2) Choosing your Gaussian surface: > a) break up a simple surface so that E-Field is constant (or zero) on all elements of it non-constant E-Fields make the integral very difficult > b) it s also helpful if the da s of your surface are parallel to the field non-constant angles # difficult integration > Note: in this class we ve only considered three surfaces (spheres, cylinders and boxes). Your surface should be one of these! 3) Φ = Σ E surface A surface 4) Evaluate Enclosed Charge ELECTRIC POTENTIAL Definition of Electric Potential: V = U / q! Potential differences are path independent (Electric Force is conservative) Understand concept of reference potential Use conservation of Energy to describe how particles move in a potential! Kinetic vs. Potential energy Calculate Potentials for simple situations: V = i f E ds! point charges! simple distributions: spheres, lines, cylinders, planes Superposition of Potentials! calculate potential of groups of objects 4

Potential Energy required to build a charge distribution PROPERTIES OF CONDUCTORS Note: applies only to electrostatics Always keep these in mind when confronted with a problem involving conductors! 1) All free charge on a conductor resides on the surface! Free Charge is: a) charge that you put on the conductor b) accumulations of negative or positive charge from the atoms in the conductor that are induced by external fields 2) E = 0 at all points inside a conductor! Gaussian surfaces which lie completely inside a conductor enclose zero net charge 3) At the surface of the conductor: E points perpendicular to the surface at each point 4) All points on a conductor (or a set of connected conductors) are at the same potential. Be able to solve Gauss Law problems involving conductors CAPACITANCE Definition: Q = CV Calculate C for simple configurations! C from calculation of potential difference (V) between two conductors when charge (Q) is put on them! plates, cylinders, spheres Energy Stored in Capacitor: U = ½ CV 2 = ½ Q 2 /C Energy Density: u = ½ ε o E 2 Equivalent Capacitances:! Series: 1/C = Σ 1/C i! Parallel: C = Σ C i! Remember how these were derived Effect of Introducing a Dielectric: C = κc vacuum CURRENT Definition: I = dq/dt! remember defined as motion of positive charges Getting current from drift velocity of electrons! I = nev d A RESISTANCE Definition: R = ρ (L/A) (for most materials)! Resistivity depends on Temperature: ρ = ρ(t) Ohm s Law: V = IR 5

! understand concept of potential drop across resistor! sign of potential drop Equivalent Resistance! Series: R = Σ R i! Parallel: 1/R = Σ 1/R i! Remember how these were derived DC CIRCUITS Circuit Solving Techniques 1. Draw Equivalent Circuits when possible Conductors in contact are at the same potential Change shape of circuit to suit your taste, but: Conserve number of Junctions Only change shape of Loops! don t cut them! don t add extra loops Replace groups of Resistors and Capacitors with Equivalent R or C using rules for combining in parallel and series 2. Label the sides of each EMF to indicate high (+) or low ( ) potential 3. Find the Branches (Loops) in the circuit 4. Choose a direction for the Current in each Element and draw an arrow indicating that direction 5. Apply the Junction Rule (currents) to the Currents going into and out of each Branch Point Σ I in = Σ I out 6. Apply the Loop Rule (voltages) to all the Loops in the circuit Σ V = 0 around loop for EMF s: V > 0 - + V < 0 + - for Resistors: V > 0 traversing element opposite to direction of I V < 0 traversing element in same direction as I for Capacitors: V > 0 -plate +plate V < 0 +plate -plate 7. Solve the Simultaneous Equations Power! Supplied (or absorbed) by EMF: P = IV! Dissipated in Resistor: P = I 2 R = V 2 /R! Understand the how to tell whether power is supplied or absorbed I through battery from to + : power is supplied I through batter from + to : power is absorbed 6

MAGNETIC FIELDS AND FORCES Magnetic Force:! Charges: F = qv B (point particle)! Currents: F = IL B (straight wire)! Use right-hand rule to find direction! Force between current carrying wires: Two straight wires Straight wire and Loop! Circular Path of Charged Particle in a Uniform Magnetic Field: For v perpendicular to B > mv = qbr Crossed Magnetic and Electric Fields! Understand examples of systems using both Electric and Magnetic Fields Mass Spectrometer Electron Discovery (cathode ray tube)! Generally: E-Field used to accelerate particle > K = q V B-Field used to make particle move in a circle > mv = qbr Undeviated motion through region of crossed E and B > F E = F B Magnetic Dipoles: Torque & Energy! τ = µ B! U = µ B! µ = Magnetic Dipole Moment µ = N I A (for current loop of N turns) Biot Savart Law (fundamental calculation of magnetic fields) v v µ o ds rˆ! db = i currents 2 4π r v v µ o rˆ! B = q charges 2 4π r! Simple Applications no complicated integrals! Use with symmetry of problem to get direction of B On exam calculate Magnetic Fields using two methods:! 1) Superposition of B-Fields apply this to find total fields for systems where you know the fields separately for each of the components! 2) Ampere s Law only appropriate when there is strong symmetry Ampere's Law: v! B ds = µ oienc loop v 7

! Steps for using Ampere's Law (similar to Gauss' Law) Determine direction of Magnetic Field using symmetry of problem Choose Amperean Loop either parallel or perpendicular to Field Do the integral Calculate how much current is enclosed by loop > sign of current from (yet another) right-hand rule! Understand derivation of fields for: 1) Straight Wires 2) Planes of Current 3) Solenoids 4) Toroids Right-Hand Rules for Direction of Fields from Wires:! Straight Wires! Circular Loops! Solenoids TIME VARYING MAGNETIC FIELDS Magnetic Flux: Φ = B da! Understand calculation for: B = constant (in space) B varies with position > only very simple calculations here Faraday's Law / Lenz's Law! EMF Induced Around Loop = dφ B / dt induced EMF opposes change in flux! Induced Current from Induced EMF Direction of induced current > sets up induced B-field to oppose change in flux from external B-field Magnitude of induced current from: > I ind = V ind / R! Understand Ways to get dφ B / dt Time Varying B Area of Loop Changes Loop Rotates in Constant Field Loop moves through region of non-uniform field! Simple Calculations of induced EMFs and Currents INDUCTANCE Mutual Inductance:! Know what this is and how it arises Self Inductance! Definition: L = N Φ / I Calculate for simple configurations (especially solenoids)! Voltage Drop across an inductor: 8

V L = L di/dt! Adding Inductances Series: L eq = Σ L i Parallel: (1/ L eq ) = Σ (1/L i )! Energy in Inductor: U = ½ L i 2! Energy Density in Magnetic Field u B = B 2 / 2µ o RC & RL CIRCUITS Know general forms of current and voltage in series RC and RL circuits when connecting or disconnecting from a battery of voltage V. Connect Disconnect RC Q(t) Q f [1 exp( t/τ C )] Q o exp( t/τ C ) τ C = RC I(t) I o exp( t/τ C ) I o exp( t/τ C ) I o = V / R V C (t) V [1 exp( t/τ C )] V exp( t/τ C ) RL I(t) I f [1 exp( t/τ L )] I o exp( t/τ L ) τ L = L/R V L (t) V exp( t/τ L ) V exp( t/τ L ) I o = I f = V / R Understand t=0 and t= values of current through parts of a circuit containing capacitors or inductors after connecting a voltage source! t = 0 Capacitor acts like a wire Inductor acts like a block! t = Capacitor acts like a block Inductor acts like a wire ALTERNATING CURRENT CIRCUITS Form for Voltage Supplied and Current:! v(t) = V m sin(ωt)! i(t) = I m sin(ωt φ) Single Element Circuits! Phase Difference between v and i! Reactances: X R, X C, X L RMS quantities! Definition: A rms = (<A 2 >) 1/2! A = A m sinωt # A rms = A m / 2 Series RLC Circuits! Total Impedance Z = [R 2 + (X L X C ) 2 ] 1/2! Phase Angle & Current Amplitude tan φ = (X L X C ) / R I m = V m / Z! Resonance Condition: Driving Frequency = Natural Frequency 9

ω o = 1 / (LC) understand how I m, etc. changes as circuit moves off resonance! RMS and Average Current and Voltages across elements! Energy Stored in Capacitor and Inductor and how it changes! Average Power and where it is dissipated <P> = I rms 2 R = I rms V rms cosφ understand how to calculate power usage in circuit only resistors dissipate power understand how power dissipation changes as the circuit moves off resonance Transformers! Relationships between V and I in Primary and Secondary Circuits V s = V p (N s /N p ) I s = I p (N p /N s )! Equivalent Resistance R eq = R (N p /N s ) 2 understand what is meant by impedance matching MAXWELL'S EQUATIONS Know what these are EM WAVES Form of EM Waves:! E perpendicular to B! E,B perpendicular to Direction of Propagation! E/B = E m /B m = c = w/k = fλ = 1/(µ o ε o ) 1/2! For Plane Waves (the only kind we studied): E(x,t) = E m sin(kx wt) B(x,t) = B m sin(kx wt) Energy Flow Poynting Vector! S = (E B)/µ o Direction of S = Direction of Propagation S = E 2 /cµ o Intensity = Power / Area! Understand Variation of Intensity with distance from source calculate for isotropic source of known power: I(r) = I o / r 2! Average Intensity: 2 I = <S> = E rms /cµ o Radiation Pressure and Momentum! total reflection: P rad = 2I/c! total absorption P rad = I/c! Calculate Force from Radiation Pressure Polarization! Understand the difference between polarized and unpolarized light Polarization Direction = Direction of oscillation of E-field 10

! Transmission of Light through Polarizing Filters Unpolarized Light: I trans = ½ I o Polarized Light: I trans = I o cos 2 θ Be able to solve problems with multiple polarizing filters Reflection and Refraction:! Law of Reflection: θ r = θ i! Snell s Law: n 1 sinθ 1 = n 2 sinθ 2 θ measured with respect to the normal to the surface Definition of Index of Refraction: > n = c/v (v = speed of light in medium < c)! Special Cases: Total Internal Reflection > sin θ crit = n 2 / n 1 Polarization by Reflection > Reflected Light is Polarized parallel to interface between media > Total Polarization at Brewster s Angle: tan θ B = n 2 / n 1 GEOMETRICAL OPTICS Optical Devices Studied:! Plane Mirrors! Spherical Mirrors! Spherical Refracting Surfaces! Thin Lenses Understand Conventions (see Optics Handout available on the Web)! What is convex and concave! Signs for radii of curvature and focii! Image Positions with respect to device and object! Magnification! Definitions of Virtual/Real Upright/Inverted Images Ray Tracing to understand general characteristics of Images Solve Problems involving:! Single optical devices! Two optical devices: the image of the 1 st forms the object of the 2 nd INTERFERENCE Understand relationships between frequency, wavelength, speed! w = 2π/T = 2πf k = 2π/λ! In Vacuum: w/k = fλ = c! In Material (index of refraction n): v = c/n f n = f w n = w λ n = λ/n k n = nk Amplitude and Intensity of Waves: 11

! Amplitude: E(x,t) = E m sin φ(x,t)! Intensity: I = <E(x,t) 2 > / cµ o ( Amplitude 2 )! Adding waves together: Add Amplitudes then square to get intensity Understand concept of phase of wave: φ(x,t)! For Plane wave in a particular medium: φ(x,t) = k n x wt! Calculate change in phase between two points on a single wave Count number of oscillations between points A and B > φ = 2πN N = x / λ Be able to do this for: > waves travelling in one medium between A and B > waves moving through several media between A and B Understand concept of Coherence between waves:! Waves must oscillate at same frequency! Waves must have same phase at some point in space Sources of Phase Difference between initially coherent waves! 1) Travel over different distances! 2) Travel through different media! 3) Reflect off different surfaces! 4) All of the above Know how to calculate phase differences in terms of:! wavelengths: N(x) = N A N B! radians: φ(x) = 2π N! Be able to do this for all 3 possible ways initially coherent waves can get out of phase Conditions for Constructive and Destructive Interference! Constructive: φ = 2mπ (even multiple of π)! Destructive: φ = (2m+1)π (odd multiple of π)! Apply these conditions to general situations involving two sources Some specific examples to understand:! Note: problems will generally be slight twists on these! 2-Slit (or 2 Source) Interference: Conditions for Maxima and Minima of intensity > Max: d sinθ = mλ > Min: d sinθ = (m+1/2)λ > know how these were obtained from constructive and destructive interference Formula for Intensity vs. Angle > I = 4I o cos 2 ( φ/2) φ = 2πd sinθ / λ Understand plot of Intensity vs. Angle! Interference of light passing through different thicknesses of transparent material! Thin Film Interference Understand how to set up the conditions for interference in thin films for arbitrary indices of refraction 12

> (don t just memorize the formula for thin films in air and apply it to everything) Sources of phase difference between rays reflected from top and bottom surfaces of thin film: > 1) Phase shift on reflection: low n to high n: φ = π high n to low n: φ = 0 > 2) Difference in paths of two rays (including index of refraction) DIFFRACTION Single-Slit Diffraction! Understand the concepts of how the equations are derived. No need to be able to reproduce the math. questions here will ask you to apply the formulas we have derived! Position of Minima Min: a sinθ = mλ! Maxima approximately halfway between minima: Max: a sinθ ~ (m+1/2)λ! Intensity: I = I o ( sinα / α) 2 α = πa sinθ / λ Understand plot of Intensity width of central maximum Diffraction by a Circular Aperture! Position of first minimum: sinθ = 1.22 λ/d! Width of diffracted beams! Resolvability understand Rayleigh s criterion and how to apply it to find the minimum resolvable distance/angle between distant objects Double-Slit Diffraction! only need to know the general forms of the intensities from this! No detailed calculations 13