) = nct n 1 Ct n dt = 1
|
|
- Coral Gallagher
- 6 years ago
- Views:
Transcription
1 Constnts: g 9.8 m/s G N m / kg c m / s M E kg E m v sound n r 343 m/s t 0 C k B J/K N A k 4π Nm C C N m q e C m e kg T m m p kg ev J 4π 0 7 A h J s h π Spheres: A 4πr V 4 3 πr 3 Cylnders: A πr + πrh V πr h c m/s Crcles: A πr C πr Qudrtc Formul: z + bz + c 0 solutons re Bnoml Approxmton: for ε the followng pproxmton holds ( + ε n + nε Clculus: d ( Ct n nct n Ct n n + Ct n+ + D Knemtcs: Δx x f x Δv v f v Δ f Δt t f t v Δx Δt Δ ( t lm Δx v( t lm Δt d t Δt dx t d v t Δv Δt d 3 x( t 3 Δx v t Δv ( t lm t Δt dv t d x( t Δ Δt t t t Δv t Δ t x f x + v t + t v f v + t v f v + ( x f x x f x ( v + v f t crculr moton: c v r Forces & Newton s Second Lw: t lm Δv F net Δt dv F m t unform crculr moton: work, constnt force: W F Δr FΔr cosθ work, vrble force: W F dr work-energy theorem: W net ΔKE KE f KE Potentl Energy: ΔPE PE f PE F conservtve dr t v πr T πrf Knetc Energy: KE trnslton mv KE rotton Iω Power: P F v Δr lm F Δt dw Energy Conservton, conservtve forces: PE + KE PE f + KE f Energy Conservton, nonconservtve forces: Lner Momentum: p m v P net momentum conservton: f F net externl d P net m v MV CM PE + KE + W nonconservtve PE f + KE f F F net externl d P net z b ± b 4c 0 then P net ntl P net fnl or m v ntl m v fnl
2 ottonl Knemtcs: θ f θ + ω t + αt ω f ω + αt ω f ω + α ( θ f θ rottonl-to-lner connectons: v rω c rω t rα ottonl Dynmcs: τ net τ Iα d L net momentum conservton: f τ net externl d L net where τ r F rf snβ ˆn nd I m r r dm 0 then L net ntl L net fnl or L ntl L fnl energy: KE rot Iω nd for generl moton KE net KE trns + KE rot MV CM Electrc Force nd Electrc Feld: Coulomb s Lw F kq q r pont chrge E kq r ˆr pont chrges E ˆr E F q o kq ˆr contnuous chrge r + I CMω k E r dqˆr chrge denstes λ q l or dq λdl σ q A or dq σda ρ q or dq ρdτ (τ s volume τ Guss s Lw: Φ E Electrc Dpole Moment: E d A q enclosed p q L nd nfnte lne E τ p E λ π r ˆr nfnte sheet E σ ˆn Electrc Potentl Energy nd Electrc Potentl: ΔPE PE B PE A q o E dl r A ΔV V B V A ΔPE r B E dl q o pont chrge V kq r pont chrges V kq contnuous chrge V k r dq Cpctors nd esstors: r A ΔV I prllel C eq C + C r B r A d + eq + C eq C C C Q ΔV C κc o where ε κ prllel plte C κ eq + seres energy stored U Q C QΔV C( ΔV power dsspted P IΔV I ΔV energy densty u E E Electrc Current: I dq conductors I nqv d A where v d qe m τ current densty J I A nqv d resstvty ρ ρ o + α ( T T o nd ρ m nq τ nd ρ L A
3 C Crcuts: chrgng q(t Cε e t C nd I(t ε e t C dschrgng q(t Qe t C nd I(t Q C e t C Mgnetc Force: Mgnetc Dpole Moment: F q v B F I l B d F Id s B prllel wres µ I A nd τ µ B Mgnetc Flux: Φ B B da Ampere s Lw: Frdy s Lw: ε E dl dφ B Mgnetc Felds: solenod B NI l motonl emf ε Blv B d l I enclosed F l I I π Bot-Svrt db Ids ˆr wre B µ I o 4π r πr torod B µ NI o πr ni loop on symmetry xs perpendculr to plne B x I! x + fnte wre s shown t rght B µ I o ( 4πr snθ + snθ energy densty u B B Inductors: self-nduced emf ε L L di nductnce L NΦ B I L Crcuts: chrgng I(t ε ( e t / L LC Crcuts: Q( t Q o cos( ωt + δ I ( t ωq o sn( ωt + δ LC Crcuts: Q Q o e t L cos( ω d t where ω d dschrgng I(t ε t / L e LC L AC Crcuts: rms vlues x rms x mx rectnces X C ωc I energy U LI nd X L ω L 3 gven genertor v V mx snωt then V mx snωt V mx C sn ωt + π X C L V mx sn ωt π X L generl mpednce Z + ( X L X C phse ngle tnφ X X L C Ohm s Lw equvlent V mx I mx Z or V rms I rms Z AC LC Crcut I rms V rms Z V rms + X L X C resonnce ω o LC P ve I rms qulty fctor Q ω o Δω FWHM!! r V rms + X L X C power P ve I rms V rms cosφ V rms ω + L ω ω o
4 Mxwell s Eqns: B d A 0 where Φ E E A or Φ E wve equtons E x Electromgnetc dton: E d A q enc B d l I enc + dφ E E da nd Φ B B A or Φ B B da µ E B o t x E E mx cos kx ωt B t where v c nd c f λ ω πf k π λ ĵ nd B B mx cos( kx ωt ˆk B mx E mx c E d l dφ B energy densty u E u B ε E o B so u u E + u B E B ndu v ( E µ v o ε E o mx ntensty I S A E B where power Iv S v E mx c cb mx cu v momentum p U c (complete bsorpton pressure P F A A Δp Δt ΔU ca Δt ca S c emf B mx Optcs: lw of reflecton θ θ I Snell s Lw n snθ n snθ where n c v n crtcl ngle θ c sn lens/mrror eqn f p + q mgnfer NP f M NP f n + telescope M f o f e norml eye NP 5 cm nd FP nfnty mgnfcton M q p mcroscope M NP l f e f o ylegh crteron for slt θ mn λ for crcle θ mn. λ D polrzton I I o cos θ Two Slt: constructve δ d snθ m mλ or δ d y m L mλ where m 0,±,±... destructve δ d snθ m m + λ or δ d y m L m + λ where m 0,±,±... Sngle Slt: destructve snθ m m λ or y m m λl where m ±,±,±3... Dffrcton Grtng: constructve d snθ m mλ where m 0,,... Trgonometrc Identtes: sn A cos A ( cos ( A + tn A sec A cos( A cos A sn A ( + cos ( A + cot A csc A sn( A ± B sn Acos B ± cos Asn B sn A + cos A sn( A sn Acos A cos( A ± B cos Asn B sn Acos B
5 sn Asn B cos( A B cos( A + B cos Acos B cos( A B + cos( A + B eltvty: L L p v c Δt Δt p v c p mu u c Lorentz Trnsformtons: S to S S to S ΔE (Δmc coordntes: x γ (x vt x γ (x+ vt where γ v y y nd z z y y nd z z t γ t v c x t γ t + v c x u veloctes: u x x v u x v c u u x + v x + u x v c c u y u z u y u u y y γ ( + u x v c γ u x v c u z γ u x v c u u z z γ ( + u x v c Photon: E hf p h λ DeBrogle: λ h p h mv Hesenberg: ΔxΔp ΔEΔt Photoelectrc Effect: KE mx eδv s hf φ Schrödnger Eqn: d ψ + Vψ Eψ m dx λ c c f c hc φ Compton: Δλ λ λ h cosθ m e c normlzton ψ dx probblty P b ψ dx expectton x x ψ dx Prtcle n Infnte Well: ψ n nπx sn L L E n h 8mL n where n,, 3... Blmer-ydberg: λ f c H n f n where.097 H 07 m Bohr: E n π m( ke h n ke o n n 3.6eV r h n n 4π mke n o Blckbody: Stefn-Boltzmnn P AeσT 4 Plnck ( λ πhc λ 5 e hc λkt b Wen λ mx T mk ylegh-jens λ πk B Tc λ 4 o m
Louisiana State University Physics 2102, Exam 3 April 2nd, 2009.
PRINT Your Name: Instructor: Louisiana State University Physics 2102, Exam 3 April 2nd, 2009. Please be sure to PRINT your name and class instructor above. The test consists of 4 questions (multiple choice),
More informationSUMMARY 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.
SUMMARY Phys 53 (University Physics II) Compiled by Prof. Erickson q 1 q Coulomb s Law: F 1 = k e r ˆr where k e = 1 4π =8.9875 10 9 N m /C, and =8.85 10 1 C /(N m )isthepermittivity of free space. Generally,
More informationQ1. In a stretched string the frequency of the wave DOES NOT depends on:
Coordinator: Al-Shukri Wednesday, June 08, 011 Page: 1 Q1. In a stretched string the frequency of the wave DOES NOT depends on: A) Amplitude of the wave B) Wavelength of the wave C) Velocity of the wave
More informationQuiz 4 (Discussion Session) Phys 1302W.400 Spring 2018
Quiz 4 (Discussion ession) Phys 1302W.400 pring 2018 This group quiz consists of one problem that, together with the individual problems on Friday, will determine your grade for quiz 4. For the group problem,
More informationPhys102 Final-132 Zero Version Coordinator: A.A.Naqvi Wednesday, May 21, 2014 Page: 1
Coordinator: A.A.Naqvi Wednesday, May 1, 014 Page: 1 Q1. What is the potential difference V B -V A in the circuit shown in Figure 1 if R 1 =70.0 Ω, R =105 Ω, R 3 =140 Ω, ε 1 =.0 V and ε =7.0 V? A).3 V
More informationHarold s AP Physics Cheat Sheet 23 February Electricity / Magnetism
Harold s AP Physics Cheat Sheet 23 February 206 Kinematics Position (m) (rad) Translation Horizontal: x = x 0 + v x0 t + 2 at2 Vertical: y = y 0 + v y0 t 2 gt2 x = x 0 + vt s = rθ x = v / Rotational Motion
More informationFOUNDATION STUDIES EXAMINATIONS June PHYSICS Semester One February Main
1 FOUNDATION STUDIES EXAMINATIONS June 2015 PHYSICS Semester One February Main Time allowed 2 hours for writing 10 minutes for reading This paper consists of 6 questions printed on 10 pages. PLEASE CHECK
More informationLouisiana State University Physics 2102, Exam 2, March 5th, 2009.
PRINT Your Name: Instructor: Louisiana State University Physics 2102, Exam 2, March 5th, 2009. Please be sure to PRINT your name and class instructor above. The test consists of 4 questions (multiple choice),
More informationPHY2049 Exam 2 solutions Fall 2016 Solution:
PHY2049 Exam 2 solutons Fall 2016 General strategy: Fnd two resstors, one par at a tme, that are connected ether n SERIES or n PARALLEL; replace these two resstors wth one of an equvalent resstance. Now
More informationPhysics 114 Exam 3 Spring Name:
Physcs 114 Exam 3 Sprng 015 Name: For gradng purposes (do not wrte here): Queston 1. 1... 3. 3. Problem 4. Answer each of the followng questons. Ponts for each queston are ndcated n red. Unless otherwse
More informationFundamental Constants
Fundamental Constants Atomic Mass Unit u 1.660 540 2 10 10 27 kg 931.434 32 28 MeV c 2 Avogadro s number N A 6.022 136 7 36 10 23 (g mol) 1 Bohr magneton μ B 9.274 015 4(31) 10-24 J/T Bohr radius a 0 0.529
More informationPhysics Equations Course Comparison
Physics Equatios Couse Compaiso Ietify you couse. You may use ay of the equatios beeath a to the left of you couse. Math A A PeCalculus Calculus AB o BC A to B is OR A:B is (Cocuet) (Cocuet) B B Algeba
More informationFOUNDATION STUDIES EXAMINATIONS June PHYSICS Semester One February Main
1 FOUNDATION STUDIES EXAMINATIONS June 2013 PHYSICS Semester One February Main Time allowed 2 hours for writing 10 minutes for reading This paper consists of 4 questions printed on 10 pages. PLEASE CHECK
More informationPhysics 208, Spring 2016 Exam #3
Physics 208, Spring 206 Exam #3 A Name (Last, First): ID #: Section #: You have 75 minutes to complete the exam. Formulae are provided on an attached sheet. You may NOT use any other formula sheet. You
More informationName (Last, First): You may use only scientific or graphing calculators. In particular you may not use the calculator app on your phone or tablet!
Final Exam : Physics 2113 Fall 2014 5:30PM MON 8 DEC 2014 Name (Last, First): Section # Instructor s name: Answer all 6 problems & all 8 questions. Be sure to write your name. Please read the questions
More informationPhysics Lecture 40: FRI3 DEC
Physics 3 Physics 3 Lecture 4: FRI3 DEC Review of concepts for the final exam Electric Fields Electric field E at some point in space is defined as the force divided by the electric charge. Force on charge
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Spring 2014 Final Exam Equation Sheet. B( r) = µ o 4π
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.02 Spring 2014 Final Exam Equation Sheet Force Law: F q = q( E ext + v q B ext ) Poynting Vector: S = ( E B) / µ 0 Force on Current Carrying
More informationragsdale (zdr82) HW6 ditmire (58335) 1 the direction of the current in the figure. Using the lower circuit in the figure, we get
rgsdle (zdr8) HW6 dtmre (58335) Ths prnt-out should hve 5 questons Multple-choce questons my contnue on the next column or pge fnd ll choces efore nswerng 00 (prt of ) 00 ponts The currents re flowng n
More informationω = 0 a = 0 = α P = constant L = constant dt = 0 = d Equilibrium when: τ i = 0 τ net τ i Static Equilibrium when: F z = 0 F net = F i = ma = d P
Equilibrium when: F net = F i τ net = τ i a = 0 = α dp = 0 = d L = ma = d P = 0 = I α = d L = 0 P = constant L = constant F x = 0 τ i = 0 F y = 0 F z = 0 Static Equilibrium when: P = 0 L = 0 v com = 0
More informationPhysics Will Farmer. May 5, Physics 1120 Contents 2
Physics 1120 Will Farmer May 5, 2013 Contents Physics 1120 Contents 2 1 Charges 3 1.1 Terms................................................... 3 1.2 Electric Charge..............................................
More informationPhysics GRE: Electromagnetism. G. J. Loges 1. University of Rochester Dept. of Physics & Astronomy. xkcd.com/567/
Physics GRE: Electromagnetism G. J. Loges University of Rochester Dept. of Physics & stronomy xkcd.com/567/ c Gregory Loges, 206 Contents Electrostatics 2 Magnetostatics 2 3 Method of Images 3 4 Lorentz
More informationFOUNDATION STUDIES EXAMINATIONS September 2009
1 FOUNDATION STUDIES EXAINATIONS September 2009 PHYSICS First Paper July Fast Track Time allowed 1.5 hour for writing 10 minutes for reading This paper consists of 4 questions printed on 7 pages. PLEASE
More informationPhysics 111. Exam #1. February 14, 2014
Physics 111 Exam #1 February 14, 2014 Name Please read and follow these instructions carefully: Read all problems carefully before attempting to solve them. Your work must be legible, and the organization
More informationFinal on December Physics 106 R. Schad. 3e 4e 5c 6d 7c 8d 9b 10e 11d 12e 13d 14d 15b 16d 17b 18b 19c 20a
Final on December11. 2007 - Physics 106 R. Schad YOUR NAME STUDENT NUMBER 3e 4e 5c 6d 7c 8d 9b 10e 11d 12e 13d 14d 15b 16d 17b 18b 19c 20a 1. 2. 3. 4. This is to identify the exam version you have IMPORTANT
More informationFOUNDATION STUDIES EXAMINATIONS November PHYSICS Semester Two February Main
FOUNDATION STUDIES EXAMINATIONS November 203 PHYSICS Semester Two February Main Time allowed 2 hours for writing 0 minutes for reading This paper consists of 5 questions printed on 0 pages. PLEASE CHECK
More informationFOUNDATION STUDIES EXAMINATIONS January 2016
1 FOUNDATION STUDIES EXAMINATIONS January 2016 PHYSICS Seester 2 Exa July Fast Track Tie allowed 2 hours for writing 10 inutes for reading This paper consists of 4 questions printed on 11 pages. PLEASE
More informationPhysics 1B Spring 2010: Final Version A 1 COMMENTS AND REMINDERS:
Physics 1B Spring 2010: Final Version A 1 COMMENTS AND REMINDERS: Closed book. No work needs to be shown for multiple-choice questions. 1. Four charges are at the corners of a square, with B and C on opposite
More informationn Higher Physics 1B (Special) (PHYS1241) (6UOC) n Advanced Science n Double Degree (Science/Engineering) n Credit or higher in Physics 1A
Physics in Session 2: I n Physics / Higher Physics 1B (PHYS1221/1231) n Science, dvanced Science n Engineering: Electrical, Photovoltaic,Telecom n Double Degree: Science/Engineering n 6 UOC n Waves n Physical
More informationCHAPTER 31. Answer to Checkpoint Questions
CHAPTE 31 INDUCTION AND INDUCTANCE 89 CHAPTE 31 Answer to Checkpont Questons 1. b, then d nd e te, nd then nd c te (zero). () nd (b) te, then (c) (zero) 3. c nd d te, then nd b te 4. b, out; c, out; d,
More informationExam 2 Solutions. Note that there are several variations of some problems, indicated by choices in parentheses.
Exam 2 Solutions Note that there are several variations of some problems, indicated by choices in parentheses. Problem 1 Part of a long, straight insulated wire carrying current i is bent into a circular
More informationExam 2 Solutions. ε 3. ε 1. Problem 1
Exam 2 Solutions Problem 1 In the circuit shown, R1=100 Ω, R2=25 Ω, and the ideal batteries have EMFs of ε1 = 6.0 V, ε2 = 3.0 V, and ε3 = 1.5 V. What is the magnitude of the current flowing through resistor
More informationPoynting Vector and Energy Flow W14D1
Poynting Vector and Energy Flow W14D1 1 Announcements Week 14 Prepset due online Friday 8:30 am PS 11 due Week 14 Friday at 9 pm in boxes outside 26-152 Sunday Tutoring 1-5 pm in 26-152 2 Outline Poynting
More information3. Quasi-Stationary Electrodynamics
3. Qus-ttonry Electrodynmcs J B 1 Condtons for the Qus- ttonry Electrodynmcs The Qus-ttonry Electrodynmcs s chrcterzed y 1 st order tme ntercton etween electrc nd mgnetc felds. In qus-sttonry EM, n the
More informationPart 4: Electromagnetism. 4.1: Induction. A. Faraday's Law. The magnetic flux through a loop of wire is
1 Part 4: Electromagnetism 4.1: Induction A. Faraday's Law The magnetic flux through a loop of wire is Φ = BA cos θ B A B = magnetic field penetrating loop [T] A = area of loop [m 2 ] = angle between field
More information3.4 Black-Body Radiation Nuclear reactions Radioactivity Nuclear Fission Nuclear Fusion Quark Model...
Contents 1 Classical Mechanics 4 1.1 Kinematics: 1-D, Constant Acceleration......................... 4 1.2 Kinematics: 2-D, Constant Acceleration......................... 4 1.3 Uniform Circular Motion.................................
More informationPrinciples of Physics II
Principles of Physics II J. M. Veal, Ph. D. version 18.05.4 Contents 1 Fluid Mechanics 3 1.1 Fluid pressure............................ 3 1. Buoyancy.............................. 3 1.3 Fluid flow..............................
More informationComplement to Physics 259
Complement to Physics 259 P. Marzlin 1 1 Institute for Quantum Information Science, University of Calgary, 2500 University Drive NW, Calgary, Alberta T2N 1N4, Canada I. INTRODUCTORY REMARKS The purpose
More informationEMF induced in a coil by moving a bar magnet. Induced EMF: Faraday s Law. Induction and Oscillations. Electromagnetic Induction.
Inducton and Oscllatons Ch. 3: Faraday s Law Ch. 3: AC Crcuts Induced EMF: Faraday s Law Tme-dependent B creates nduced E In partcular: A changng magnetc flux creates an emf n a crcut: Ammeter or voltmeter.
More informationChapter 31. Faraday s Law
Chapter 31 Faraday s Law 1 Ampere s law Magnetic field is produced by time variation of electric field dφ B ( I I ) E d s = µ o + d = µ o I+ µ oεo ds E B 2 Induction A loop of wire is connected to a sensitive
More informationAngular Displacement. θ i. 1rev = 360 = 2π rads. = "angular displacement" Δθ = θ f. π = circumference. diameter
Rotational Motion Angular Displacement π = circumference diameter π = circumference 2 radius circumference = 2πr Arc length s = rθ, (where θ in radians) θ 1rev = 360 = 2π rads Δθ = θ f θ i = "angular displacement"
More information[variable] = units (or dimension) of variable.
Dimensional Analysis Zoe Wyatt wyatt.zoe@gmail.com with help from Emanuel Malek Understanding units usually makes physics much easier to understand. It also gives a good method of checking if an answer
More information2nd Year Electromagnetism 2012:.Exam Practice
2nd Year Electromagnetism 2012:.Exam Practice These are sample questions of the type of question that will be set in the exam. They haven t been checked the way exam questions are checked so there may
More information10/23/2003 PHY Lecture 14R 1
Announcements. Remember -- Tuesday, Oct. 8 th, 9:30 AM Second exam (coverng Chapters 9-4 of HRW) Brng the followng: a) equaton sheet b) Calculator c) Pencl d) Clear head e) Note: If you have kept up wth
More informationFields, Charges, and Field Lines
Felds, Charges, and Feld Lnes Electrc charges create electrc felds. (Gauss Law) Electrc feld lnes begn on + charges and end on - charges. Lke charges repel, oppostes attract. Start wth same dea for magnetc
More informationWhere k = 1. The electric field produced by a point charge is given by
Ch 21 review: 1. Electric charge: Electric charge is a property of a matter. There are two kinds of charges, positive and negative. Charges of the same sign repel each other. Charges of opposite sign attract.
More information3 Chapter. Gauss s Law
3 Chapter Gauss s Law 3.1 Electric Flux... 3-2 3.2 Gauss s Law (see also Gauss s Law Simulation in Section 3.10)... 3-4 Example 3.1: Infinitely Long Rod of Uniform Charge Density... 3-9 Example 3.2: Infinite
More informationPhysics 2020 Exam 2 Constants and Formulae
Physics 2020 Exam 2 Constants and Formulae Useful Constants k e = 8.99 10 9 N m 2 /C 2 c = 3.00 10 8 m/s ɛ = 8.85 10 12 C 2 /(N m 2 ) µ = 4π 10 7 T m/a e = 1.602 10 19 C h = 6.626 10 34 J s m p = 1.67
More informationWorked Examples Set 2
Worked Examples Set 2 Q.1. Application of Maxwell s eqns. [Griffiths Problem 7.42] In a perfect conductor the conductivity σ is infinite, so from Ohm s law J = σe, E = 0. Any net charge must be on the
More informationPhysics 102 Exam 1 Fall Last Name: First Name Network-ID
Physics 0 Exam Fall 03 Last Name: First Name Network-ID Discussion Section: Discussion TA Name: Turn off your cell phone and put it out of sight. Keep your calculator on your own desk. Calculators cannot
More informationLECTURE 17. Reminder Magnetic Flux
LECTURE 17 Motional EMF Eddy Currents Self Inductance Reminder Magnetic Flux Faraday s Law ε = dφ B Flux through one loop Φ B = BAcosθ da Flux through N loops Φ B = NBAcosθ 1 Reminder How to Change Magnetic
More informationYell if you have any questions
Class 36: Outline Hour 1: Concept Review / Overview PRS Questions Possible Exam Questions Hour : Sample Exam Yell if you have any questions P36-1 Before Starting All of your grades should now be posted
More informationQueen s University at Kingston. Faculty of Arts and Science. Department of Physics PHYSICS 106. Final Examination.
Page 1 of 5 Queen s University at Kingston Faculty of Arts and Science Department of Physics PHYSICS 106 Final Examination April 16th, 2009 Professor: A. B. McLean Time allowed: 3 HOURS Instructions This
More informationPhysics 4B. Question and 3 tie (clockwise), then 2 and 5 tie (zero), then 4 and 6 tie (counterclockwise) B i. ( T / s) = 1.74 V.
Physcs 4 Solutons to Chapter 3 HW Chapter 3: Questons:, 4, 1 Problems:, 15, 19, 7, 33, 41, 45, 54, 65 Queston 3-1 and 3 te (clockwse), then and 5 te (zero), then 4 and 6 te (counterclockwse) Queston 3-4
More informationElectricity. Revision Notes. R.D.Pilkington
Electricity Revision Notes R.D.Pilkington DIRECT CURRENTS Introduction Current: Rate of charge flow, I = dq/dt Units: amps Potential and potential difference: work done to move unit +ve charge from point
More informationUNIT # 10. JEE-Physics ELECTROMAGNETIC INDUCTION & ALTERNATING CURRENT EXERCISE I N B A
J-Physcs UN # OMAGN NDUON & ANANG UN XS. otl chnge n flu otl chrge flown through the col resstnce. esstnce. Webers. N A t W.mJ v t r r... d N S d N e N 5volt d e.8 volt volt d 6 NA ()( ). > mg < mg 5.
More informationMagnetic Materials. 1. Magnetization 2. Potential and field of a magnetized object
Magnetic Materials 1. Magnetization 2. Potential and field of a magnetized object 3. H-field 4. Susceptibility and permeability 5. Boundary conditions 6. Magnetic field energy and magnetic pressure 1 Magnetic
More informationPreliminary Examination - Day 1 Thursday, August 10, 2017
UNL - Department of Physics and Astronomy Preliminary Examination - Day Thursday, August, 7 This test covers the topics of Quantum Mechanics (Topic ) and Electrodynamics (Topic ). Each topic has 4 A questions
More informationPhysics 121 Sample Common Exam 2 Rev2 NOTE: ANSWERS ARE ON PAGE 7. Instructions:
Physcs 121 Smple Common Exm 2 Rev2 NOTE: ANSWERS ARE ON PAGE 7 Nme (Prnt): 4 Dgt ID: Secton: Instructons: Answer ll 27 multple choce questons. You my need to do some clculton. Answer ech queston on the
More informationYell if you have any questions
Class 36: Outline Hour 1: Concept Review / Overview PRS Questions Possible Exam Questions Hour : Sample Exam Yell if you have any questions P36-1 efore Starting All of your grades should now be posted
More informationName (Print): 4 Digit ID: Section:
Physics 11 Sample Common Exam 3: Sample 5 Name (Print): 4 Digit ID: Section: Honors Code Pledge: As an NJIT student I, pledge to comply with the provisions of the NJIT Academic Honor Code. I assert that
More informationPhysics Exam 1 Formulas
INSTRUCTIONS: Write your NAME on the front of the blue exam booklet. The exam is closed book, and you may have only pens/pencils and a calculator (no stored equations or programs and no graphing). Show
More informationChapter 31. Faraday s Law
Chapter 31 Faraday s Law 1 Ampere s law Magnetic field is produced by time variation of electric field B s II I d d μ o d μo με o o E ds E B Induction A loop of wire is connected to a sensitive ammeter
More informationReview. Spring Semester /21/14. Physics for Scientists & Engineers 2 1
Review Spring Semester 2014 Physics for Scientists & Engineers 2 1 Notes! Homework set 13 extended to Tuesday, 4/22! Remember to fill out SIRS form: https://sirsonline.msu.edu Physics for Scientists &
More informationElectricity and Magnetism - Physics 121 Lecture 10 - Sources of Magnetic Fields (Currents) Y&F Chapter 28, Sec. 1-7
Electrcty and Magnetsm - Physcs 11 Lecture 10 - Sources of Magnetc Felds (Currents) Y&F Chapter 8, Sec. 1-7 Magnetc felds are due to currents The Bot-Savart Law Calculatng feld at the centers of current
More informationTHE UNIVERSITY OF SYDNEY FACULTY OF SCIENCE INTERMEDIATE PHYSICS PHYS 2912 PHYSICS 2B (ADVANCED) ALL QUESTIONS HAVE THE VALUE SHOWN
CC0936 THE UNIVERSITY OF SYDNEY FACULTY OF SCIENCE INTERMEDIATE PHYSICS PHYS 91 PHYSICS B (ADVANCED) SEMESTER, 014 TIME ALLOWED: 3 HOURS ALL QUESTIONS HAVE THE VALUE SHOWN INSTRUCTIONS: This paper consists
More informationPhysics 231 Exam III Dec. 1, 2003
Physics 231 Exam III Dec. 1, 2003 1. One night while asleep you find you are having a nightmare. You find that you are in the middle of the French revolution. Unfortunately you are being led up to the
More informationPhysics 114 Exam 2 Fall 2014 Solutions. Name:
Physcs 114 Exam Fall 014 Name: For gradng purposes (do not wrte here): Queston 1. 1... 3. 3. Problem Answer each of the followng questons. Ponts for each queston are ndcated n red. Unless otherwse ndcated,
More informationFinal Exam: Physics Spring, 2017 May 8, 2017 Version 01
Final Exam: Physics2331 - Spring, 2017 May 8, 2017 Version 01 NAME (Please Print) Your exam should have 11 pages. This exam consists of 18 multiple-choice questions (2 points each, worth 36 points), and
More informationForces of Rolling. 1) Ifobjectisrollingwith a com =0 (i.e.no netforces), then v com =ωr = constant (smooth roll)
Physics 2101 Section 3 March 12 rd : Ch. 10 Announcements: Mid-grades posted in PAW Quiz today I will be at the March APS meeting the week of 15-19 th. Prof. Rich Kurtz will help me. Class Website: http://www.phys.lsu.edu/classes/spring2010/phys2101-3/
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Spring 2014 Practice Problem Set 11 Solutions
MASSACHUSES INSIUE OF ECHNOLOGY Department of Physics 8 Spring 4 Practice Problem Set Solutions Problem : Electromagnetic Waves and the Poynting Vector We have been studying one particular class of electric
More informationMaxwell s Equations & Electromagnetic Waves. The Equations So Far...
Maxwell s Equations & Electromagnetic Waves Maxwell s equations contain the wave equation Velocity of electromagnetic waves c = 2.99792458 x 1 8 m/s Relationship between E and B in an EM wave Energy in
More informationSolutions: Homework 5
Ex. 5.1: Capacitor Solutions: Homework 5 (a) Consider a parallel plate capacitor with large circular plates, radius a, a distance d apart, with a d. Choose cylindrical coordinates (r,φ,z) and let the z
More informationnrt V dv = nrt ln(3) = P AV A ln(3) P A dv = P A V 5/ / /3
Problem. a For an isothermal process: W iso = VA 3V A PdV = VA 3V A nrt V dv = nrt ln3 = P AV A ln3 For the adiabatic leg, PV γ =const. Thus, I get that P = P A VA V γ. Since the gas is monatomic, γ =
More informationPhysics 442. Electro-Magneto-Dynamics. M. Berrondo. Physics BYU
Physics 44 Electro-Magneto-Dynamics M. Berrondo Physics BYU 1 Paravectors Φ= V + cα Φ= V cα 1 = t c 1 = + t c J = c + ρ J J ρ = c J S = cu + em S S = cu em S Physics BYU EM Wave Equation Apply to Maxwell
More informationPhysics: Dr. F. Wilhelm E:\Excel files\230 lecture\230 tests\final 230 F07 Practice.doc page 1 of 9
Physics: Dr. F. Wilhelm E:\Excel files\3 lecture\3 tests\final 3 F7 Practice.doc page 1 of 9 NAME:... POINTS:... Dr. Fritz Wilhelm, Diablo Valley College, Physics Department Phone: (95) 671-739 Extension:
More informationMany-Body Calculations of the Isotope Shift
Mny-Body Clcultons of the Isotope Shft W. R. Johnson Mrch 11, 1 1 Introducton Atomc energy levels re commonly evluted ssumng tht the nucler mss s nfnte. In ths report, we consder correctons to tomc levels
More informationSolutions to PS 6 Physics 401a
Solutions to PS 6 Physics 401a 1. Let B point along the z axis. Then by circuar symmetry, we have B(r, t) =B(r, t)e z (1) Using Faraday s Law, we can find the electric field at radius r to be E(r, t) dl
More informationAP Physics C. Electricity and Magne4sm Review
AP Physics C Electricity and Magne4sm Review Electrosta4cs 30% Chap 22-25 Charge and Coulomb s Law Electric Field and Electric Poten4al (including point charges) Gauss Law Fields and poten4als of other
More informationPhysics 2102 Spring 2007 Lecture 10 Current and Resistance
esstance Is Futle! Physcs 0 Sprng 007 Jonathan Dowlng Physcs 0 Sprng 007 Lecture 0 Current and esstance Georg Smon Ohm (789-854) What are we gong to learn? A road map lectrc charge lectrc force on other
More informationFormularium Natuurkunde II Jarne Verhaeghe:
Formularium Natuurkunde II Jarne Verhaeghe: 016-017 7. Magnetic Field and Magnetic Forces Magnetic Field F = qv B magnitude of F = q vb sin φ = q v verticaal op B B Magnetic Field Lines and Magnetic Flux
More informationPhysics 342: Modern Physics
Physics 342: Modern Physics Final Exam (Practice) Relativity: 1) Two LEDs at each end of a meter stick oriented along the x -axis flash simultaneously in their rest frame A. The meter stick is traveling
More informationPhysics 208, Spring 2016 Exam #2
Physics 208, Spring 2016 Exam #2 A Name (Last, First): ID #: Section #: You have 75 minutes to complete the exam. Formulae are provided on an attached sheet. You may NOT use any other formula sheet. You
More informationPhysics 111. Exam #3. March 4, 2011
Phyic Exam #3 March 4, 20 Name Multiple Choice /6 Problem # /2 Problem #2 /2 Problem #3 /2 Problem #4 /2 Total /00 PartI:Multiple Choice:Circlethebetanwertoeachquetion.Anyothermark willnotbegivencredit.eachmultiple
More informationPhysics 2020 Exam 4 Constants and Formulae
Physics 2020 Exam 4 Constants and Formulae Useful Constants k e = 8.99 10 9 Nm 2 /C 2 ɛ = 8.85 10 12 C 2 /(N m 2 ) µ = 4π 10 7 T m/a e = 1.60219 10 19 C G = 6.673 10 11 Nm 2 /kg 2 h = 6.62620 10 34 Js
More informationPES 1120 Spring 2014, Spendier Lecture 6/Page 1
PES 110 Sprng 014, Spender Lecture 6/Page 1 Lecture today: Chapter 1) Electrc feld due to charge dstrbutons -> charged rod -> charged rng We ntroduced the electrc feld, E. I defned t as an nvsble aura
More informationQuantum Mechanics & Atomic Structure (Chapter 11)
Quantum Mechanics & Atomic Structure (Chapter 11) Quantum mechanics: Microscopic theory of light & matter at molecular scale and smaller. Atoms and radiation (light) have both wave-like and particlelike
More informationData Provided: A formula sheet and table of physical constants is attached to this paper. DEPARTMENT OF PHYSICS & Autumn Semester ASTRONOMY
PHY221 PHY472 Dt Provided: Formul sheet nd physicl constnts Dt Provided: A formul sheet nd tble of physicl constnts is ttched to this pper. DEPARTMENT OF PHYSICS & Autumn Semester 2009-2010 ASTRONOMY DEPARTMENT
More information10/9/2003 PHY Lecture 11 1
Announcements 1. Physc Colloquum today --The Physcs and Analyss of Non-nvasve Optcal Imagng. Today s lecture Bref revew of momentum & collsons Example HW problems Introducton to rotatons Defnton of angular
More informationECE 470 Electric Machines Review of Maxwell s Equations in Integral Form. 1. To discuss a classification of materials
EE 470 Electric Mchines Review of Mxwell s Equtions in Integrl Form Objectives: 1. To discuss clssifiction of mterils 2. To discuss properties of homogeneous, liner, isotropic, nd time-invrint mterils
More informationPHYSICS - CLUTCH CH 28: INDUCTION AND INDUCTANCE.
!! www.clutchprep.com CONCEPT: ELECTROMAGNETIC INDUCTION A col of wre wth a VOLTAGE across each end wll have a current n t - Wre doesn t HAVE to have voltage source, voltage can be INDUCED V Common ways
More informationE = K + U. p mv. p i = p f. F dt = p. J t 1. a r = v2. F c = m v2. s = rθ. a t = rα. r 2 dm i. m i r 2 i. I ring = MR 2.
v = v i + at x = x i + v i t + 1 2 at2 E = K + U p mv p i = p f L r p = Iω τ r F = rf sin θ v 2 = v 2 i + 2a x F = ma = dp dt = U v dx dt a dv dt = d2 x dt 2 A circle = πr 2 A sphere = 4πr 2 V sphere =
More informationb) (4) How large is the current through the 2.00 Ω resistor, and in which direction?
General Physics II Exam 2 - Chs. 19 21 - Circuits, Magnetism, EM Induction - Sep. 29, 2016 Name Rec. Instr. Rec. Time For full credit, make your work clear. Show formulas used, essential steps, and results
More informationP812 Midterm Examination February Solutions
P8 Midterm Exmintion Februry s. A one dimensionl chin of chrges consist of e nd e lterntively plced with neighbouring distnce. Show tht the potentil energy of ech chrge is given by U = ln. 4πε Explin qulittively
More informationPhysics 202, Exam 1 Review
Physics 202, Exam 1 Review Logistics Topics: Electrostatics (Chapters 21-24.6) Point charges: electric force, field, potential energy, and potential Distributions: electric field, electric potential. Interaction
More informationTranslational vs Rotational. m x. Connection Δ = = = = = = Δ = = = = = = Δ =Δ = = = = = 2 / 1/2. Work
Translational vs Rotational / / 1/ Δ m x v dx dt a dv dt F ma p mv KE mv Work Fd / / 1/ θ ω θ α ω τ α ω ω τθ Δ I d dt d dt I L I KE I Work / θ ω α τ Δ Δ c t s r v r a v r a r Fr L pr Connection Translational
More informationExam 3 Topics. Displacement Current Poynting Vector. Faraday s Law Self Inductance. Circuits. Energy Stored in Inductor/Magnetic Field
Exam 3 Topics Faraday s Law Self Inductance Energy Stored in Inductor/Magnetic Field Circuits LR Circuits Undriven (R)LC Circuits Driven RLC Circuits Displacement Current Poynting Vector NO: B Materials,
More informationPHY102 Electricity Course Summary
TOPIC 1 ELECTOSTTICS PHY1 Electricity Course Summary Coulomb s Law The magnitude of the force between two point charges is directly proportional to the product of the charges and inversely proportional
More informationChapter 7 Steady Magnetic Field. september 2016 Microwave Laboratory Sogang University
Chpter 7 Stedy Mgnetic Field september 2016 Microwve Lbortory Sogng University Teching point Wht is the mgnetic field? Biot-Svrt s lw: Coulomb s lw of Mgnetic field Stedy current: current flow is independent
More informationYell if you have any questions
Class 31: Outline Hour 1: Concept Review / Overview PRS Questions possible exam questions Hour : Sample Exam Yell if you have any questions P31 1 Exam 3 Topics Faraday s Law Self Inductance Energy Stored
More informationCh 7 Electric Potential
Ch 7 Electric Potential Electric Energy, Electric Potential Energy concepts are going to be extremely important to us as we consider the behavior of charges in electric fields. How do energy concepts help
More information