Phys122A-Lecture 2 Electric Field
|
|
- Dale Arnold
- 5 years ago
- Views:
Transcription
1 Phys122A-Lecture 2 Electric Field
2 Physics 122 Labs Sections begin on next week Before your section meets Get a copy of the lab manual at the UW Bookstore! Read the information on page iii as it has a lot of information related to the course, the course website, WebAssign, etc. Get a WebAssign account (Pay by credit card only) There are 3 components to the labs: Pre-Labs: Needs to be completed before each of your lab sessions begin. Pre-labs will be completed in WebAssign In-class Experiment: This is your lab section in which you will need your lab manual. Post-Labs: Completed after your lab session also on WebAssign (Lab) Course website: Please check the Frequently Asked Questions (FAQs) link before you the Instructor!
3 Reading
4 From FlipIt Physics For the collection of charges shown in the above problem, which of the following statements best describes FY, the y component of the net force on the charge at the origin FY > 0 FY = 0 FY < 0 In Force from Four Charges it is unclear whether the angle matters.
5 From FlipIt Physics What is charge? Electric charge is the physical property of matter that causes it to experience a force when placed in an electromagnetic field. Conserved Units: [Q] = Coulomb (C) e p n Q -e +e 0 e = C
6 From FlipIt Physics Where are you from? Born in UK but lived here since I was 0.5 years old. Don t assign two units! Sorry. Explain why force on electrons and nucleus is equal magnitude. (Newton 3rd Law.) Line integral wasn t explained.
7 Coulomb Law: Introduction to the Electric Field ~F 1,2 = kq 1q 2 r 2 1,2 ˆr 1,2 Superposition for an collection of discrete charges: ~F Net,i = X j6=i kq i q j r 2 j,i ˆr j,i q 1 q 1 q 1 q 1 q 1 q 1 q 1
8 Introduction to the Electric Field Superposition for an collection of discrete charges: ~F Net,0 = X j6=0 q 1 q 2 kq 0 q j r 2 j,0 ˆr j,0 = q 0 X j6=0 kq j r 2 j,0 ˆr j,i q 3 q 4 q 5 q 6 q 0 Define the Electric Field (q0 is a test charge): ~E ~ F Net,0 q 0
9 Electric field from a point charge Electric Field from a point charge (at the origin): F ~E ~ 1,0 = kq 1 q 0 r 2 ˆr Electric Field from a collection of charges: ~E(~r 0 )= X j6=0 kq j r 2 j,0 ˆr j,0
10 What is a field? Scalar, vector (or tensor ) valued function of space (and time). Electric Field (vector) ~E(~r, t) Magnetic Field (vector) ~B(~r, t) Electric Potential (scalar) (~r, t)
11 Fields of all kinds These isolated Temperatures make up a Scalar Field (you learn only the temperature at a place you choose)
12 Fields of all kinds... It may be more interesting to know which way the wind is blowing That would require a VECTOR field. (you learn how fast the wind is blowing, AND in what direction)
13 Does the E field really exist? Computation tool or physical entity? Two unattractive alternatives: Assume E field exists at all locations in space Assume action at a distance Useful heuristic for understanding physics: There is no instantaneous action at a distance.
14 Visualizing the E field Direction: Radial ~E(~r )= kq 1 r 2 ˆr Direction of the force on a positive charge Amplitude: Decreases with distance
15 Visualizing the E field 6 ~E(~r )= kq 1 r 2 ˆr 4 quiver or Velocity Plot Y (m) Q You almost never see the E field drawn this way! X (m) General tool for visualizing a vector field.
16 Visualizing the E field Field lines next time.
17 Visualizing the E field 6 4 quiver or Velocity Plot Y (m) 2 0 +Q You almost never see the E field drawn this way! -2-4 General tool for visualizing a vector field X (m)
18 Visualizing the E field ~E(x, y) y=0 = kq 1 xî x 3 E x (AU) x (m)
19 Two equal mass balls are suspended from the ceiling with equal length nonconducting threads as shown. Ball 1 has charge Q 1 = +3q and Ball 2 has charge Q 2 = +q. Which of the following pictures best represents the equilibrium position? Q 1 Q 2 +3q +q (a) Q 1 +3q (b) Q 2 +q Q 1 Q 2 +3q +q (c) Clicker 2-1
20 What happens to the Force on q 1 if its sign is changed? A) F 1 increases B) F 1 remains the same C) F 1 decreases D) Need more information to determine Clicker 2-2 q 2 q 1 q 4 q 3
21 Two charges, Q 1 and Q 2, fixed along the x-axis as shown, produce an electric field E at a point (x,y) = (0,d) which is directed along the negative y-axis. Which is true? d y E (a) Both charges Q 1 and Q 2 must be positive. (b) Both charges Q 1 and Q 2 must be negative. Q 1 Q 2 x (c) The charges Q 1 and Q 2 must have opposite signs. Clicker 2-3
22 Q 1 has charge +Q Q 2 has charge +2Q They are separated by d. a d Charge q is a distance a away from Q 1 Is there a place the value for a -- between Q 1 and Q 2 where the force on ANY charge (positive or negative) is zero? (a) (b) (c) NO Yes, but I can t find it with all this time pressure. Yes and my answer is from Q 1. I will volunteer to specify if you ask me Clicker 2-4
23 Electric field from a point charge Electric Field from a point charge (at the origin): F ~E ~ 1,0 = kq 1 q 0 r 2 ˆr Electric Field from a collection of charges: ~E(~r 0 )= X j6=0 kq j r 2 j,0 ˆr j,0
24 E field from a line charge Electric Field from a collection of charges: ~E(~r 0 )= X j6=0 kq j r 2 j,0 ˆr j,0 Electric Field from a continuous charge distribution: observer E( r ) ~E(~r )=k Z dq ~r 0 ~r ~r 0 ~r ~r 0 3 r r r dq r origin r
25 E field from a charge distribution ~E(~r )=k Z dq ~r 0 ~r ~r 0 ~r ~r 0 3 observer E( r ) r r r dq r Electric Field from a 1D source: [λ] = C/m 1 origin r dq ~r 0! d` (~r 0 ) Electric Field from a 2D source: [σ] = C/m 2 dq ~r 0! d 2 x (~r 0 ) Electric Field from a 3D source: [ρ] = C/m 3 dq ~r 0! d 3 x (~r 0 )
26 E field from a line charge [a] =m [ ]=C/m a
27 Clicker
28 Work the integral
The World According to Physics 121
The World According to Physics Objects Forces Specified by geometry and mass Gravity: F = G m m r m Others: Tension, Normal, Friction Space and Time uclidean with Galilean Invariance ordinary 3D space;;
More informationWelcome to Physics 122
Welcome to Physics 122 122A: Paul A. Wiggins 122B: Miguel Morales 122C: Arka Majumdar Content: Electricity & Magnetism Here Format: Active Learning (Learn from Participation)» PreLectures & Checkpoints
More informationPhys 122 Lecture 3 G. Rybka
Phys 122 Lecture 3 G. Rybka A few more Demos Electric Field Lines Example Calculations: Discrete: Electric Dipole Overview Continuous: Infinite Line of Charge Next week Labs and Tutorials begin Electric
More informationWelcome. to Physics 2135.
Welcome to Physics 2135. PHYSICS 2135 Engineering Physics II Dr. S. Thomas Vojta Instructor in charge Office: 204 Physics, Phone: 341-4793 vojtat@mst.edu www.mst.edu/~vojtat Office hours: Mon+ Wed 11am-12pm
More informationGeneral Physics II. Electric Charge, Forces & Fields
General Physics II Electric Charge, Forces & Fields Electric Charge Recall that fundamental particles carry something called electric charge protons have exactly one unit of positive charge +1.602 x 10-19
More informationAnnouncements. I clickers. Expected to come prepared to participate in I clickers
Announcements Required pre-survey: Take TODAY and save confirmation page. Deadline Jan 26 midnight. https://rutgers.qualtrics.com/se/?sid=sv_2gj6vkee2lbv0fv&q_jfe=0 Makeup for required pre-test: Tuesday,
More informationWeek 4. Outline Review electric Forces Review electric Potential
Week 4 Outline Review electric Forces Review electric Potential Electric Charge - A property of matter Matter is made up of two kinds of electric charges (positive and negative). Like charges repel, unlike
More informationWelcome to Physics 161 Elements of Physics Fall 2018, Sept 4. Wim Kloet
Welcome to Physics 161 Elements of Physics Fall 2018, Sept 4 Wim Kloet 1 Lecture 1 TOPICS Administration - course web page - contact details Course materials - text book - iclicker - syllabus Course Components
More informationPHYSICS 272 Electric & Magnetic Interactions
PHYSICS 272 Electric & Magnetic Interactions Professor in Charge: Prof. Wei Xie WebAsssign Administrator: Dr. V.K. Saxena Office: PHYS 246 Office: PHYS 76 Email: wxie@purdue.edu E-Mail: saxena@purdue.edu
More informationThe Electric Field EM-L2-1
The EM-L2-1 Review of Lecture 1 Electric charge is quantised and conserved in interactions The force between two charges is given by Coulomb s law Force F 1,2 exerted by a charge q 1 on another charge
More informationAnnouncements Monday, September 18
Announcements Monday, September 18 WeBWorK 1.4, 1.5 are due on Wednesday at 11:59pm. The first midterm is on this Friday, September 22. Midterms happen during recitation. The exam covers through 1.5. About
More informationPhysics 9 Spring 2011 Homework 1 - Solutions Wednesday January 19, 2011
Physics 9 Spring 011 Homework 1 - s Wednesday January 19, 011 Make sure your name is on your homework, and please box your final answer. Because we will be giving partial credit, be sure to attempt all
More informationConcepTest PowerPoints
ConcepTest PowerPoints Chapter 16 Physics: Principles with Applications, 6 th edition Giancoli 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for
More informationPhysics Fall Semester. Sections 1 5. Please find a seat. Keep all walkways free for safety reasons and to comply with the fire code.
Physics 222 2018 Fall Semester Sections 1 5 Please find a seat. Keep all walkways free for safety reasons and to comply with the fire code. Electronic Devices Please separate your professional from your
More informationPHYS 241 Electricity, Magnetism & Optics Syllabus
PHYS 241 Electricity, Magnetism & Optics Syllabus Questions about grades, grade checks, absences, course withdrawal, etc please see Prof. Laura Pyrak-Nolte 1 PHYS 241 Electricity & Optics Physics & Astronomy
More informationPHYS 241 Electricity & Optics
PHYS 41 Electricity & Optics Physics & Astronomy Department Home page: http://www.physics.purdue.edu/ Course Home page: http://www.physics.purdue.edu/phys41/ CHIP Home page: http://chip.physics.purdue.edu/public/41/fall016/
More informationSemester 2 Physics (SF 026) Lecture: BP 3 by Yew Sze Fiona Website:
Semester 2 Physics (SF 026) Lecture: BP 3 by Yew Sze Ling @ Fiona Website: http://yslphysics.weebly.com/ Chapter 1: Electrostatics The study of electric charges at rest, the forces between them and the
More informationWelcome to PHY212!! General Physics II:! Electricity, Magnetism, and Light!
Welcome to PHY212!! General Physics II:! Electricity, Magnetism, and Light! Prof. Mitch Soderberg! msoderbe@syr.edu Lecture 1.1! Jan. 13, 2015 1 Announcements Register for PHY222 (labs) if you haven t
More informationWelcome to Physics 212
Welcome to Physics 212 http://online.physics.uiuc.edu/courses/phys212 This lecture is VERY full. Please sit next to someone nice. Find out the best thing that happened to them during the winter break!
More informationPhysics 101 covers. Forces Kinematics Energy/Momentum Rotations Fluids Waves/Sound Thermodynamics. Physics 101: Lecture 1, Pg 1
Physics 101 covers Forces Kinematics Energy/Momentum Rotations Fluids Waves/Sound Thermodynamics Physics 101: Lecture 1, Pg 1 Meet the Lecturer Professor Tom Kuhlman tkuhlman@illinois.edu Office Hours
More informationPhysics 1A, Lecture 3: One Dimensional Kinema:cs Summer Session 1, 2011
Your textbook should be closed, though you may use any handwrieen notes that you have taken. You will use your clicker to answer these ques:ons. If you do not yet have a clicker, please turn in your answers
More informationPHY 114 A General Physics II 11 AM-12:15 PM TR Olin 101. Plan for Lecture 1:
PHY 4 A General Physics II AM-:5 PM TR Olin Plan for Lecture :. Welcome & overview. Class structure & announcements 3. Electrical charges and forces /8/0 PHY 4 A Spring 0 -- Lecture PHY 4 A General Physics
More informationLecture 1.2 :! Electric Force and Electric Field
Lecture 1.2 :! Electric Force and Electric Field Lecture Outline:! Charging Objects! Coulomb s Law! Electric Field! Textbook Reading:! Ch. 25.3-25.5 Jan. 15, 2015 1 Announcements Quiz in class next Thu.
More informationWelcome Back to Physics Electric Fields. Micheal Faraday Physics 1308: General Physics II - Professor Jodi Cooley
Welcome Back to Physics 1308 Electric Fields Micheal Faraday 1791-1867 Announcements Assignments for Thursday, August 30th: - Reading: Chapter 22.3-22.5 - Watch Video: https://youtu.be/wc79wv5klx4 Lecture
More informationWelcome to Physics 212
Welcome to Physics 212 http://online.physics.uiuc.edu/courses/phys212 01 Physics 212 Lecture 1, Slide 1 Physics 212 Lecture 1 Today's Concepts: a) Coulomb s Law b) Superposition 03 Physics 212 Lecture
More information01. Introduction and Electric Field I
University of Rhode Island DigitalCommons@URI PHY 204: lementary Physics II Physics Course Materials 2015 01. Introduction and lectric Field I Gerhard Müller University of Rhode Island, gmuller@uri.edu
More informationPhysics 1A. Lecture 1B
Physics 1A Lecture 1B Angles: a Tricky Unit θ Angles are formally defined as a ratio of lengths; e.g. θ = Arclength/Radius [θ] = L/L = 1 This makes the angle unitless! The fundamental unit of angle is
More informationWelcome. to Electrostatics
Welcome to Electrostatics Outline 1. Coulomb s Law 2. The Electric Field - Examples 3. Gauss Law - Examples 4. Conductors in Electric Field Coulomb s Law Coulomb s law quantifies the magnitude of the electrostatic
More informationExperiment 3 Forces are Vectors
Name Partner(s): Experiment 3 Forces are Vectors Objectives Preparation Pre-Lab Understand that some quantities in physics are vectors, others are scalars. Be able to perform vector addition graphically
More informationPlease turn cell phones off
Welcome to Physics 102! Electricity Magnetism (at the heart of most processes around us: in atoms & molecules; living cells) Optics Atomic Physics Nuclear Physics Relativity http://www.communicationcurrents.com
More informationPHYS 241D Electricity & Optics
PHYS 241D Electricity & Optics Physics Department Home page: http://www.physics.purdue.edu/ Course Home page: http://www.physics.purdue.edu/phys241d/ CHIP Home page: http://chip.physics.purdue.edu/public/241d/fall2014/
More informationHistory. The word electricity comes from the Greek elektron which means amber. The amber effect is what we call static electricity.
Electrostatics 1 History The word electricity comes from the Greek elektron which means amber. The amber effect is what we call static electricity. 2 ELECTROSTATICS the study of electric charges, forces
More informationElectromagnetism Physics 15b
Electromagnetism Physics 15b Lecture #2 Guass s Law Electric Field and Flux Purcell 1.7 1.15 Administravia Online sectioning due Wednesday (tudy Card Day) Go to http://www.section.fas.harvard.edu/ Do both
More informationPHYS 2135 Engineering Physics II Fall Course Information: Canvas and Course Website Begin with Course Handbook and Syllabus
Instructor: Dr. Jim Musser musserj@mst.edu Physics 122 PHYS 2135 Engineering Physics II Fall 2018 Course Information: Canvas and Course Website Begin with Course Handbook and Syllabus PHYS 2135 Engineering
More informationPhysics 100. Reminder: All lecture notes posted, after lecture, follow link at:
Physics 100 Please pick up a clicker! Reminder: All lecture notes posted, after lecture, follow link at: http://www.hunter.cuny.edu/physics/courses/physics100/spring-2016 Note: Before the actual lecture,
More informationWelcome to PHYS2002!
Welcome to PHYS00! Physics I Done! We are now all experts in mechanics. Mechanics Mass M Interaction: mm F = G r 1 G = 6.67 10 Nm/ kg r M 11 1 We never said what mass is, only how it behaves. New Semester
More informationPHYS 1444 Section 02. Lecture #3
PHYS 1444 Section 0 Chapter 1 Electric Fields Electric Dipoles Lecture #3 Tuesday Jan 5, 011 Dr. Andrew Brandt Homework on Ch 1 is due 9pm Thursday, Jan. 7 1 Angle: After calculating magnitudes, take x+y
More informationELECTROSTATICS. the study of electric charges, forces and fields Static Electricity is Stationary Electricity or Accumulation of charge
Electrostatics 1 ELECTROSTATICS the study of electric charges, forces and fields Static Electricity is Stationary Electricity or Accumulation of charge Fundamental Rule Opposites attract, Likes Repel Things
More informationLecture 2.1 :! Electric Field
Lecture 2.1 :! Electric Field Lecture Outline:! Electric Field! Electric Field of Point Charges! Electric Field of Continuous Distribution of Charge! Textbook Reading:! Ch. 26.1-26.3 Jan. 20, 2015 1 Announcements
More informationComputer Model of Spring-Mass System. Q1: Can a computer model of a mass-spring system, based on the finite-time form of the momentum principle
QUESTIONS: Parts I, II (this week s activity): Computer Model of Spring-Mass System Q1: Can a computer model of a mass-spring system, based on the finite-time form of the momentum principle and using your
More informationElectrostatic Interactions (This lab is adapted from Chapter 1of Electric and Magnetic Interactions, Chabay and Sherwood, 1995.)
Name: Partner(s): 1118 section: Desk # Date: Electrostatic Interactions (This lab is adapted from Chapter 1of Electric and Magnetic Interactions, Chabay and Sherwood, 1995.) Purpose To investigate the
More informationThe Electric Field + + q 1 q 2. Coulomb s Law of Electro-static Force: How does q 1 know of the presence of q 2?
The Electric ield 1 Coulomb s Law of Electro-static orce: k How does 1 know of the presence of? 1 r rˆ sets up an electric field in the space surrounding it. At any point the field has both a magnitude
More informationPhysics Lab 202P-3. Electric Fields and Superposition: A Virtual Lab NAME: LAB PARTNERS:
Physics Lab 202P-3 Electric Fields and Superposition: A Virtual Lab NAME: LAB PARTNERS: LAB SECTION: LAB INSTRUCTOR: DATE: EMAIL ADDRESS: Penn State University Created by nitin samarth Physics Lab 202P-3
More informationPhysics Electrostatics Problems. Science and Mathematics Education Research Group
F FA ACULTY C U L T Y OF O F EDUCATION E D U C A T I O N Department of Curriculum and Pedagogy Physics Electrostatics Problems Science and Mathematics Education Research Group Supported by UBC Teaching
More informationPhysics 9 Spring 2012 Midterm 1 Solutions
Physics 9 Spring 22 NAME: TA: Physics 9 Spring 22 Midterm s For the midterm, you may use one sheet of notes with whatever you want to put on it, front and back. Please sit every other seat, and please
More informationSummary for last week: Newton s 2 nd Law + 1 st Law
! F resultant = Summary for last week: Newton s 2 nd Law + 1 st Law F! " i = F! 1 + F! 2 +...+ F! N = m! all forces acting on object due to other objects a Object if we measure acceleration in an inertial
More informationPHYS 221 General Physics: Electricity, Light and Modern Physics. Lecture 1 Electric Charges & Coulomb s Law. Electric Charge.
PHYS 1 General Phsics: Electricit, Light and Modern Phsics Lecture 1 Electric Charges & Coulomb s Law Phsics Department Home page: http://www.phsics.purdue.edu/ Course Home page: http://www.phsics.purdue.edu/phs1/
More informationEECS 117 Lecture 7: Electrostatics Review
EECS 117 Lecture 7: Electrostatics Review Prof. Niknejad University of California, Berkeley University of California, Berkeley EECS 117 Lecture 7 p. 1/19 Existence of Charge Charge, like mass, is an intrinsic
More informationElectric flux. You must be able to calculate the electric flux through a surface.
Today s agenda: Announcements. lectric field lines. You must be able to draw electric field lines, and interpret diagrams that show electric field lines. A dipole in an external electric field. You must
More information( E ) = Lecture 1 Electric Charges & Coulomb s Law. Electric & Magnetic Fields. Electric Charge. Electric Charge
Electric & Magnetic Fields Lecture 1 Electric Charges & Coulomb s Law Electric and magnetic fields manifest their existence through interactions with matter. Differential Form div E E = ( ) = div( B )
More informationEssential University Physics
Essential University Physics Richard Wolfson 22 Electric Potential PowerPoint Lecture prepared by Richard Wolfson Slide 22-1 In this lecture you ll learn The concept of electric potential difference Including
More informationPHYS 122 Introductory Physics II Dr. Eric C. Anderson UMBC Fall 2016 Syllabus. Getting ready
PHYS 122 Introductory Physics II Dr. Eric C. Anderson UMBC Fall 2016 Syllabus Getting ready Prerequisites You must have completed Phys 121, and Math 152 (or be enrolled in it this semester.) Workload Experience
More informationThe stars and the Earth
The stars and the Earth Astronomy 101 Syracuse University, Fall 2018 Walter Freeman August 30, 2018 Astronomy 101 The celestial sphere August 30, 2018 1 / 26 The celestial sphere of the stars I know that
More informationCharge. Electrostatics Notes (614) Review: Atomic Structure 3/10/14! Charge!! 3 Basic Particles make up Atoms:
Electrostatics Notes (614) Charge!! Review: Atomic Structure Sketch of Atomic Structure:! 3 Basic Particles make up Atoms: 1. 2. 3. Charge! Protons & Electrons have a property called Protons: electric
More informationToday in Physics 217: begin electrostatics
Today in Physics 217: begin electrostatics Fields and potentials, and the Helmholtz theorem The empirical basis of electrostatics Coulomb s Law At right: the classic hand-to-thevan-de-graaf experiment.
More informationPHYS 208, sections , Spring 2017
COLLEGE OF SCIENCE DEPARTMENT OF PHYSICS AND ASTRONOMY PHYS 208, sections 538-542, Spring 2017 Instructor Information Instructor Dr. Mioduszewski Telephone 979.845.1411 Email mio@comp.tamu.edu (please
More informationWelcome back to PHY101: Major Concepts in Physics I. Photo: J. M. Schwarz
Welcome back to PHY101: Major Concepts in Physics I Photo: J. M. Schwarz Announcements Course Website: http://jmschwarztheorygroup.org/phy101/ HW 7 on Chapters 9 and 16 is due on Friday at 5PM in your
More informationFebruary 20, Week 6. Homework #4, Due tonight. Mastering Physics: 9 problems from chapters 1 and 3 Written Question: 3.56
February 20, Week 6 Today: Chapter 5, Applying Newton s Laws Homework #4, Due tonight. Mastering Physics: 9 problems from chapters 1 and 3 Written Question: 3.56 Exam #2, Next Friday, February 24 Review
More informationPHYS 208, sections , Spring 2018
COLLEGE OF SCIENCE DEPARTMENT OF PHYSICS AND ASTRONOMY PHYS 208, sections 507-511, Spring 2018 Instructor Information Instructor Dr. R. Webb Telephone 979.845.4012 Email webb@physics.tamu.edu (please start
More informationLecture 2 [Chapter 21] Tuesday, Jan 17th
Lecture 2 [Chapter 21] Tuesday, Jan 17th Administrative Items Assignments this week: read Ch 21 and Ch 22 in the textbook complete Pre-Lecture Ch22 HW assignment complete Ch 21 HW assignment [Pre-Lecture
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 2B Electricity and Magnetism. Instructor: Prof Benjamin Grinstein UCSD
Physics 2B Electricity and Magnetism Instructor: Prof Benjamin Grinstein UCSD week 1 Rank in order, from most positive to most negative, the charges q a to q e of these five systems. 1. q a = q b >
More informationMass & Weight. weight a force acting on a body due to the gravitational attraction pulling that body to another. NOT constant.
Mass & Weight mass how much stuff a body has. Doesn t change. Is responsible for the inertial properties of a body. The greater the mass, the greater the force required to achieve some acceleration: Fnet
More informationMATH1014. Semester 1 Administrative Overview. Neil Montgomery calculus
MATH1014 Semester 1 Administrative Overview Lecturers: Scott Morrison linear algebra scott.morrison@anu.edu.au Neil Montgomery calculus neil.montgomery@anu.edu.au Dr Scott Morrison (ANU) MATH1014 Notes
More informationIntroductory Physics PHYS101
Introductory Physics PHYS101 Dr Richard H. Cyburt Office Hours Assistant Professor of Physics My office: 402c in the Science Building My phone: (304) 384-6006 My email: rcyburt@concord.edu TRF 9:30-11:00am
More informationDr. Todd Satogata (ODU/Jefferson Lab) Wednesday, March
Vector pointing OUT of page Vector pointing IN to page University Physics 227N/232N Ch: 26-27: Magnetism and Magnetic Induction Lab this Friday, Mar 21: Ohms Law and DC RC Circuits So NO QUIZ this Friday!
More informationElectrostatics Notes (614) Charge!
Electrostatics Notes (614) Charge! n Have you ever walked across the carpet and gotten shocked when you touched the doorknob? n What about static cling? Have you ever gotten to school only to be embarrassed
More information2 4πε ( ) ( r θ. , symmetric about the x-axis, as shown in Figure What is the electric field E at the origin O?
p E( r, θ) = cosθ 3 ( sinθ ˆi + cosθ ˆj ) + sinθ cosθ ˆi + ( cos θ 1) ˆj r ( ) ( p = cosθ sinθ ˆi + cosθ ˆj + sinθ cosθ ˆi sinθ ˆj 3 r where the trigonometric identit ( θ ) vectors ˆr and cos 1 = sin θ
More informationWelcome to Physics 202
Welcome to Physics 202 Todays Topics The Physics 202 Team Course Formality and Course Overview Q&A Ch 21: Electric Charges Physics 202 Homepage http://www.physics.wisc.edu/undergrads/courses/fall2011/202/index.html
More informationPhysics 8 Monday, September 9, 2013
Physics 8 Monday, September 9, 2013 HW2 (due Friday) printed copies. Read Chapter 4 (momentum) for Wednesday. I m reading through the book with you. It s my 3rd time now. One purpose of the reading responses
More informationPhysics 272: Electricity and Magnetism. Mark Palenik Thursday June 14 th
Physics 272: Electricity and Magnetism Mark Palenik Thursday June 14 th Topics Finish up dipoles Polarization of materials Conductors Charging/discharging iclicker (not credit) An atom is placed in a UNIFORM
More informationChapter 3, Problem 28. Agenda. Forces. Contact and Field Forces. Fundamental Forces. External and Internal Forces 2/6/14
Agenda Today: Homework Quiz, Chapter 4 (Newton s Laws) Thursday: Applying Newton s Laws Start reading Chapter 5 Chapter 3, Problem 28 A ball with a horizontal speed of 1.25 m/s rolls off a bench 1.00 m
More informationAgenda & Announcements
CHEM 115 Review for Exam 3 Lecture 24 Prof. Sevian 1 Agenda & Announcements Reminder to take post-test next week during first hour of any lab period (next slide) Assignment 13 is to study for Exam 3. Attending
More informationr 2 and the charge on a proton is +e. We never see objects that have a charge which is not a whole number multiple of this number.
Name: Physics Chapter 16 Study Guide ----------------------------------------------------------------------------------------------------- Useful Information: e = 1.6"10 #19 C mass electron = 9.11"10 #31
More informationPH 222-3A Spring 2007
PH -3A Spring 7 ELECTRIC FIELDS Lectures,3 Chapter (Halliday/Resnick/Walker, Fundamentals of Physics 8 th edition) 1 Chapter Electric Fields In this chapter we will introduce the concept of an electric
More informationPhysics 161 Lecture 5 Greek: π ρ σ Newton s Laws
Physics 161 Lecture 5 Greek: π ρ σ Newton s Laws September 18, 2018 1 Announcement 1: exam From the course webpage: Exams are multiple choice and machine graded. There are about fifteen questions in the
More informationUNIT 2 COULOMB S LAW. Objectives. to understand Coulomb s Law qualitatively and quantitatively
UNIT 2 COULOMB S LAW Objectives to understand Coulomb s Law qualitatively and quantitatively to understand the principle of superposition 1 Electric Field Hockey program 1.1 Open the program Electric Field
More informationPHYSICS 272 Electric & Magnetic Interactions
PHYS 272: Matter and Interactions II Electric And Magnetic Interactions PHYSICS 272 Electric & Magnetic Interactions Lecture 5 Charging/Discharging; Efield of distributed charges: charged rod and ring
More informationPHYS 172: Modern Mechanics
PHYS 172: Modern Mechanics Spring 2012 Lecture 1: Matter & Interactions Read: Ch 1.1-1.5 To do AS SOON AS POSSIBLE: 1. Obtain the textbook (campus bookstores, used is OK, but you are responsible for material
More informationPhysics 9 Spring 2011 Midterm 1 Solutions
Physics 9 Spring 2011 Midterm 1 s For the midterm, you may use one sheet of notes with whatever you want to put on it, front and back. Please sit every other seat, and please don t cheat! If something
More informationLecture5- Newton s Laws Chapter 5
1 / 45 Lecture5- Newton s Laws Chapter 5 Instructor: Prof. Noronha-Hostler Course Administrator: Prof. Roy Montalvo PHY-123 ANALYTICAL PHYSICS IA Phys- 123 Oct. 6 th, 2018 2 / 45 Nobel Prize in Physics
More informationElectric Fields and Potentials
Electric Fields and Potentials Please do not write on the conducting sheet, and do not use more than 5 volts from the power supply. Introduction The force between electric charges is intriguing. Why are
More informationElectric Fields of Charge Distributions
Welcome to Physics 308 Electric Fields of Charge Distributions Charles-Augustin de Coulomb 736-806 Physics 308: General Physics II - Professor Jodi Cooley Announcements Assignments for Tuesday, September
More informationLECTURE 17. Prof. Paul
LECTURE 17 Prof. Paul Announcements Exam II, two weeks away Cumulative (you must know concepts from first exam) On your hw I just handed back, (#38) I may have INCORRECTLY stated that it s wrong to use
More informationNORTHERN ILLINOIS UNIVERSITY PHYSICS DEPARTMENT. Physics 211 E&M and Quantum Physics Spring Lab #2: Electrostatics. qq k r
NORTHRN ILLINOIS UNIVRSITY PHYSICS DPARTMNT Physics 11 &M and Quantum Physics Spring 018 Lab #: lectrostatics Lab Writeup Due: Mon/Wed/Thu/Fri, Jan. 9/31/Jan. 1/, 018 Background You ve learned a lot about
More informationPHYSICS 231 INTRODUCTORY PHYSICS I
PHYSICS 231 INTRODUCTORY PHYSICS I Lecture 4 Main points of last lecture Scalars vs. Vectors Vectors A: (A x, A y ) or A & θ Addition/Subtraction Projectile Motion X-direction: a x = 0 (v x = constant)
More informationIntermediate Physics PHYS102
Intermediate Physics PHYS102 Dr Richard H. Cyburt Assistant Professor of Physics My office: 402c in the Science Building My phone: (304) 384-6006 My email: rcyburt@concord.edu My webpage: www.concord.edu/rcyburt
More informationElectricity & Magnetism Lecture 5: Electric Potential Energy
Electricity & Magnetism Lecture 5: Electric Potential Energy Today... Ø Ø Electric Poten1al Energy Unit 21 session Gravita1onal and Electrical PE Electricity & Magne/sm Lecture 5, Slide 1 Stuff you asked
More information- Like charges repel Induced Charge. or by induction. Electric charge is conserved
Course website: http://course.physastro.iastate.edu/phys112/ Here you will find the syllabus, lecture notes and other course information Links to the website are also on Blackboard: Phys 112 (Spring 2017)
More informationPhysics 201, Lecture 2. The Big Picture. Kinematics: Position and Displacement. Today s Topics
Physics 01, Lecture Today s Topics n Kinematics (Chap..1-.) n Position, Displacement (, and distance) n Time and Time Interval n Velocity (, and speed) n Acceleration *1-Dimension for today,,3-d later.
More informationConcepTest PowerPoints
ConcepTest PowerPoints Chapter 16 Physics: Principles with Applications, 7 th edition Giancoli 2014 Pearson Education, Inc. This work is protected by United States copyright laws and is provided solely
More informationAnnouncements September 19
Announcements September 19 Please complete the mid-semester CIOS survey this week The first midterm will take place during recitation a week from Friday, September 3 It covers Chapter 1, sections 1 5 and
More informationChmy 361 Elements of Physical Chemistry,
Chmy 361 Elements of Physical Chemistry, website: http://www.chemistry.montana.edu/callis/courses/chmy361 Instructor: Pat Callis office 55 Chem/Biochem Bldg (CBB) email: pcallis@montana. edu phone: 994-5414
More informationPhysics 1140 Fall 2013 Introduction to Experimental Physics
Physics 1140 Fall 2013 Introduction to Experimental Physics Joanna Atkin Lecture 1: Introduction to Course Significant Figures Standard Notation General information Lecture instructor: Joanna Atkin email:
More informationLecture-9 Date:
Lecture-9 Date: 27.01.2014 Coulomb s Law Electric Field Electric Field due to a Point Charge Electric Field due to a Line Charge Electric Charge Review Charge is measured in Coulombs (C). A Coulomb is
More informationPhysics 121. Instructor: Dr. Chris McCarthy. If you are enrolled, please mark the signup sheet
Physics 121 Instructor: Dr. Chris McCarthy If you are enrolled, please mark the signup sheet If you wish to add this class, add your name and ID# to the sheet. Pre-requisite: Physics 111. If you are not
More informationElectricity & Magnetism Lecture 4: Gauss Law
Electricity & Magnetism Lecture 4: Gauss Law Today s Concepts: A) Conductors B) Using Gauss Law Electricity & Magne/sm Lecture 4, Slide 1 Another question... whats the applica=on to real life? Stuff you
More informationSupplemental Instruction
For students enrolled in an introductory physics lab, PHYS 2108 and PHYS 2109 lab classes begin this week (Jan. 14-18). You must attend the first week class or send an email to lab@phys.lsu.edu PRIOR TO
More informationPhysics 202, Lecture 3. The Electric Field
Physics 202, Lecture 3 Today s Topics Electric Field (Review) Motion of charged particles in external E field Conductors in Electrostatic Equilibrium (Ch. 21.9) Gauss s Law (Ch. 22) Reminder: HW #1 due
More informationChapter 8: E & M (Electricity & Magnetism or Electromagnetism)
Chapter 8: E & M (Electricity & Magnetism or Electromagnetism) Electric charge & electric force Coulomb s Law Electrons & basic facts about atoms (mainly review) Charge conservation Electric current &
More information