Lecture 4.1 : Electric Potential
|
|
- Griffin Bond
- 5 years ago
- Views:
Transcription
1 Lecture 4.1 : Electric Potential Lecture Outline: Electric Potential Energy Potential Energy of Point Charges Electric Potential Textbook Reading: Ch Feb. 4,
2 Announcements Exam #1 in class Thu. (Feb. 6) covers Ch material. You are responsible for bringing your own calculator and writing utensils. 1 sheet of notes (front and back) allowed. Seating assignment will be posted by entrance doors to Stolkin. You must sit in your assigned seat. Optional review session TONIGHT from 7-8pm in Stolkin. If you attend, please bring your clickers! (Note: I know a few of you have an overlapping PHY222 lab. My apologies...i will try to schedule around this in the future. You can join us late. I actually have the room booked until 9pm and can stay late to cover anything you miss before you join.) HW4 due next Tue. (2/11) at 9am on Mastering Physics. During recitation on Friday you will go over exam solutions. 2
3 From HW3... 3
4 Last Lecture... Electric field must be zero at all points within a conductor in electrostatic equilibrium. Any excess charge has to reside on the outside surface. 4
5 From HW3... 5
6 Last Lecture... 6
7 From Recitation 3.2 Infinite Slab of Charge (27.48) 7
8 Electric Potential Energy So far in this course we have described electric charge in terms of fields and forces. We now need to consider Energy. Reminders from Mechanics: E mech = K + U =0 Conservation of Energy U = U f U i = W Work/Potential Energy Relation W = i j F ds Work done by a Force. 8
9 Electric Potential Energy Potential Energy in a Uniform Gravitational Field. U grav = mgy f mgy i U grav = U 0 + mgy = mgy 9
10 Clicker Question #1 Two rocks have equal mass. Which has more gravitational potential energy? A. Rock A. B. Rock B. C. They have the same potential energy. D. Both have zero potential energy. 10
11 Electric Potential Energy Consider a positive charge inside a parallel-plate capacitor: W elec = F elec rcos 0 = qe s f s i = qes i qes f U elec = U f U i = W elec = qes f qes i Define s=0 at negative plate, and U 0 is potential at s=0. 11
12 Electric Potential Energy Signs can be confusing here, so remember these pictures: 12
13 Clicker Question #2 Two positive charges are equal. Which has more electric potential energy? A. Charge A. B. Charge B. C. They have the same potential energy. D. Both have zero potential energy. 13
14 Electric Potential Energy Example problem: Proton/Electron in a 2.0 cm x 2.0 cm parallel plate capacitor 14
15 Clicker Question #3 A positive charge moves as shown. Its kinetic energy A. Increases. B. Remains constant. C. Decreases. 15
16 Potential Energy of Point Charges 16
17 Potential Energy of Point Charges Two like-sign point charges launched at each other: 17
18 Potential Energy of Point Charges Two opposite-sign point charges launched away from each other: E mech <0 implies a bound system. Can you think of any other bound systems in nature? 18
19 Clicker Question #4 A positive and a negative charge are released from rest in vacuum. They move toward each other. As they do: A. A positive potential energy becomes more positive. B. A positive potential energy becomes less positive. C. A negative potential energy becomes more negative. D. A negative potential energy becomes less negative. E. A positive potential energy becomes a negative potential energy. 19
20 Potential Energy of a Dipole 20
21 Electric Potential We introducted Electric Field to indicate an electric charge s alteration of space. Now we need a concept of potential energy at all points in space due to a source charge. Electric Potential: V U q+sources q 1 volt = 1 V 1 J/C Alessandro Volta 1.5 V Battery 21
22 Electric Potential V = Potential Difference, or Voltage. U = q V 22
23 Electric Potential What is the speed of a proton that has been accelerated from rest through a potential difference of -1000V? 23
24 Reminders Exam #1 on Thursday! Bring note sheet and calculator! Review session tonight from 7-8pm. 24
Lecture 11.2 : Magnetic Force
Lecture 11.2 : Magnetic Force Lecture Outline: The Hall Effect Forces on Current-Carrying Wires Forces on Current Loops Magnetic Properties of Matter Textbook Reading: Ch. 32.7-32.10 March 28, 2013 1 Announcements
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 informationLecture 3.1 :! Electric Flux
Lecture 3.1 :! Electric Flux Lecture Outline:! Motion in a Uniform Electric Field! Symmetry and Electric Fields! Electric Flux! Gauss s Law!! Textbook Reading:! Ch. 26.6-27.3 Jan. 27, 2015 1 Announcements
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 informationPHY294H. l Professor: Joey Huston l l office: BPS3230
l Professor: Joey Huston l email:huston@msu.edu l office: BPS3230 PHY294H l Homework will be with Mastering Physics (and an average of 1 handwritten problem per week) 2nd MP assignment due Wed Jan. 27;
More informationLecture 7.1 : Current and Resistance
Lecture 7.1 : Current and Resistance Lecture Outline: Current and Current Density Conductivity and Resistivity Resistance and Ohm s Law Textbook Reading: Ch. 30.3-30.5 Feb. 26, 2013 1 Announcements By
More informationA Uniform Gravitational Field
A Uniform Gravitational Field We could define a gravitational field in much the same way we have defined the electric field: E = F on q q, g = F on m m (note that m/s 2 = N/kg) The gravitational field
More informationLecture 15.2 :! Final Exam Review, Part 1
Lecture 15.2 :! Final Exam Review, Part 1 April 23, 2015 1 Announcements Online Evaluation e-mails should have been sent to you.! Please fill out the evaluation form...it is completely confidential. May
More informationChapter 16 Electrical Energy Capacitance. HW: 1, 2, 3, 5, 7, 12, 13, 17, 21, 25, 27 33, 35, 37a, 43, 45, 49, 51
Chapter 16 Electrical Energy Capacitance HW: 1, 2, 3, 5, 7, 12, 13, 17, 21, 25, 27 33, 35, 37a, 43, 45, 49, 51 Electrical Potential Reminder from physics 1: Work done by a conservative force, depends only
More informationPhysics 1202: Lecture 3 Today s Agenda
Physics 1202: Lecture 3 Today s Agenda Announcements: Lectures posted on: www.phys.uconn.edu/~rcote/ HW assignments, solutions etc. Homework #1: On Masterphysics: due this coming Friday Go to the syllabus
More informationHITT RF Remote Login Procedure:
HITT RF Remote Login Procedure: The radio channel number for this room is 07 (zero, seven). It is STRONGLY recommended to login your remote for every class just to be sure it is on the correct radio channel
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 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 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 informationPHY101: Major Concepts in Physics I. Photo: J. M. Schwarz
Welcome back to PHY101: Major Concepts in Physics I Photo: J. M. Schwarz Announcements In class today we will finish Chapter 17 on electric potential energy and electric potential and perhaps begin Chapter
More informationElectric Potential Energy Chapter 16
Electric Potential Energy Chapter 16 Electric Energy and Capacitance Sections: 1, 2, 4, 6, 7, 8, 9 The electrostatic force is a conservative force It is possible to define an electrical potential energy
More informationAgenda for Today. Elements of Physics II. Conductors and Insulators Movement of charges Conservation of charge Static electricity Electroscope
Physics 132: Lecture e 5 Elements of Physics II Agenda for Today Conductors and Insulators Movement of charges Conservation of charge Static electricity Electroscope Physics 201: Lecture 1, Pg 1 Problem
More informationPhysics 202, Lecture 8
Physics 202, Lecture 8 Today s Topics Middle Term 1 Review When and where About Exam 1 Wednesday Feb. 22 nd 5:30-7:00 pm (Rooms will be announced this Friday by email) Format Closed book One 8x11 formula
More informationMP ) 12:40-2:40 3:00-4:00 PM
PHY294H l Professor: Joey Huston l email:huston@msu.edu l office: BPS3230 l Homework will be with Mastering Physics (and an average of 1 handwritten problem per week) Problem 29.77 (already assigned) will
More informationLecture 14.1 :! Electromagnetic Fields
Lecture 14.1 :! Electromagnetic Fields Lecture Outline:! LR Circuits! E & B Transformations! The Displacement Current!! Textbook Reading:! Ch. 33.10-34.3 April 14, 2015 1 Announcements Leo Anthony Soderberg
More informationPHYSICS 1/23/2019. Chapter 25 Lecture. Chapter 25 The Electric Potential. Chapter 25 Preview
PHYSICS FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E Chapter 25 Lecture RANDALL D. KNIGHT Chapter 25 The Electric Potential IN THIS CHAPTER, you will learn to use the electric potential and electric
More informationPHYS 1441 Section 002 Lecture #7
PHYS 1441 Section 002 Lecture #7 Monday, Sept. 25, 2017 Chapter 22 One last Gauss Law Example Chapter 23 Electric Potential Electric Potential Energy Electric Potential due to Point Charges Shape of the
More informationFinishing Chapter 26 on dipoles.. Electric Potential Energy of: Point Charges Dipoles Electric Potential: V Voltage: ΔV
PHY132 Introduction to Physics II Class 11 Outline: Finishing Chapter 26 on dipoles.. Electric Potential Energy of: Point Charges Dipoles Electric Potential: V Voltage: ΔV QuickCheck 26.13 Which dipole
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 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 informationPHYSICS 100. Introduction to Physics. Bridges the gap between school science and Physics 101, Physics 120, Physics 125 or Physics 140
PHYSICS 100 Introduction to Physics Bridges the gap between school science and Physics 101, Physics 120, Physics 125 or Physics 140 Only for those WITHOUT Physics 12 or equiv. (C+ or better). If you have
More informationLos Altos Physics Honors. Electrostatics: Electric Fields, Electric Forces, Electric Potentials and. Electric Potential Energy.
Los Altos Physics Honors Electrostatics: Electric Fields, Electric Forces, Electric Potentials and Electric Potential Energy Workbook adam.randall@mvla.net www.laphysics.com dls.mvla.net/los_altos Spring
More informationElectric potential energy The concept of electric potential and potential difference Motion of charges in electric field
In this chapter, you will learn: Electric potential energy The concept of electric potential and potential difference Motion of charges in electric field 2.1 Electric potential energy When a charged particle
More informationElectricity and Magnetism. Electric Potential Energy and Voltage
Electricity and Magnetism Electric Potential Energy and Voltage Work and Potential Energy Recall from Mechanics that E mech = K + U is a conserved quantity for particles that interact via conservative
More informationThe Electric Potential Energy
Lecture 6 Chapter 25 The Electric Potential Energy Course website: http://aculty.uml.edu/andriy_danylov/teaching/physicsii Today we are going to discuss: Chapter 25: Section 25.1 Electric Potential Energy
More informationMTE1 results. Mean 75% = 90/120
MTE1 results Mean 75% = 90/120 Scores available at Learn@UW, your TAs have exams If your score is an F or a D, talk to us and your TAs for suggestions on how to improve From last times Electric charges
More informationPhysics 202, Lecture Today s Topics Middle T erm Term 1 Review
Physics 202, Lecture 7 Today s Topics Middle Term 1 Review About Exam 1 When and where Monday Sept. 27 th 5:30-7:00 pm 2301, 2241 Chamberlin (room allocation to be announced) nced) Format Close book One
More informationElectric Potential. Chapter 23. PowerPoint Lectures for University Physics, Twelfth Edition Hugh D. Young and Roger A. Freedman
Chapter 23 Electric Potential PowerPoint Lectures for University Physics, Twelfth Edition Hugh D. Young and Roger A. Freedman Lectures by Reza Khanbabaie Goals for Chapter 23 Reminder about gravitational
More informationThe 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 informationElectric Potential. 1/28/14 Physics for Scientists & Engineers 2, Chapter 23 1
Electric Potential 1/28/14 Physics for Scientists & Engineers 2, Chapter 23 1 Notes! Correction set 1 Due Thursday evening at 10pm Name: Correction #1 RS Must answer all questions correctly to receive
More informationElectrostatics Notes 2 Electric Field on a Single Charge
Electrostatics Notes 2 Electric Field on a Single Charge There are many similarities between gravitational and electrostatic forces. One such similarity is that both forces can be exerted on objects that
More informationPHYS 1441 Section 002 Lecture #6
PHYS 1441 Section 002 Lecture #6 Monday, Sept. 18, 2017 Chapter 21 Motion of a Charged Particle in an Electric Field Electric Dipoles Chapter 22 Electric Flux Gauss Law with many charges What is Gauss
More information(3.5.1) V E x, E, (3.5.2)
Lecture 3.5 Capacitors Today we shall continue our discussion of electrostatics and, in particular, the concept of electrostatic potential energy and electric potential. The main example which we have
More informationElectric Field of a uniformly Charged Thin Spherical Shell
Electric Field of a uniformly Charged Thin Spherical Shell The calculation of the field outside the shell is identical to that of a point charge. The electric field inside the shell is zero. What are the
More informationElectric Potential Energy Conservative Force
Electric Potential Energy Conservative Force Conservative force or field is a force field in which the total mechanical energy of an isolated system is conserved. Examples, Gravitation, Electrostatic,
More informationLecture 13.2 :! Inductors
Lecture 13.2 :! Inductors Lecture Outline:! Induced Fields! Inductors! LC Circuits! LR Circuits!! Textbook Reading:! Ch. 33.6-33.10 April 9, 2015 1 Announcements! HW #10 due on Tuesday, April 14, at 9am.!
More informationPHYS 1444 Section 003 Lecture #6
PHYS 1444 Section 003 Lecture #6 Thursday Sep. 13, 2012 Dr. Andrew Brandt Chapter 23: Electric Potential 1 Electric Potential Energy Concept of energy is very useful solving mechanical problems Conservation
More informationPHYSICS. Electrostatics
Electrostatics Coulomb s Law: SYNOPSIS SI unit of electric intensity is NC -1 Dimensions The electric intensity due to isolated point charge, Electric dipole moment, P = q (2a), SI unit is C m Torque on
More informationChapter 19 Electric Potential Energy and Electric Potential Sunday, January 31, Key concepts:
Chapter 19 Electric Potential Energy and Electric Potential Sunday, January 31, 2010 10:37 PM Key concepts: electric potential electric potential energy the electron-volt (ev), a convenient unit of energy
More informationPHYS 272 (Spring 2018): Introductory Physics: Fields Homeworks
PHYS 272 (Spring 2018): Introductory Physics: Fields Homeworks Note: the 1st homework is simply signing the honor pledge (but still it is compulsory); the actual homework starts with #2. And, please sign
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 informationCoulomb s Law. Phys102 Lecture 2. Key Points. Coulomb s Law The electric field (E is a vector!) References
Phys102 Lecture 2 Phys102 Lecture 2-1 Coulomb s Law Key Points Coulomb s Law The electric field (E is a vector!) References SFU Ed: 21-5,6,7,8,9,10. 6 th Ed: 16-6,7,8,9,+. Phys102 Lecture 2 Phys102 Lecture
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 informationPHYS 1444 Section 004 Lecture #22
PHYS 1444 Section 004 Lecture #22 Monday, April 23, 2012 Dr. Extension of Ampere s Law Gauss Law of Magnetism Maxwell s Equations Production of Electromagnetic Waves Today s homework is #13, due 10pm,
More informationChapter 19 Electric Potential and Electric Field Sunday, January 31, Key concepts:
Chapter 19 Electric Potential and Electric Field Sunday, January 31, 2010 10:37 PM Key concepts: electric potential electric potential energy the electron-volt (ev), a convenient unit of energy when dealing
More informationChapter 16. Electric Energy and Capacitance
Chapter 16 Electric Energy and Capacitance Electric Potential Energy The electrostatic force is a conservative force It is possible to define an electrical potential energy function with this force Work
More informationPH 1120 Electricity and Magnetism Term B, 2009 STUDY GUIDE #2
PH 1120 Electricity and Magnetism Term B, 2009 STUDY GUIDE #2 In this part of the course we will study the following topics: Electric potential difference and electric potential for a uniform field Electric
More informationPhysics 115. Energy in E fields Electric Current Batteries Resistance. General Physics II. Session 21
Physics 115 General Physics II Session 21 Energy in E fields Electric Current Batteries Resistance R. J. Wilkes Email: phy115a@u.washington.edu Home page: http://courses.washington.edu/phy115a/ 5/6/14
More informationAnnouncements 2 Oct 2014
Announcements 2 Oct 2014 1. Prayer 2. Exam 1 starts today! a. Thursday Oct 2 Tuesday Oct 7 (2 pm) in the Testing Center, late fee after Oct 6, 2 pm b. Covers through today's lecture (unless we don't quite
More informationMatthew W. Milligan. Electric Fields. a figment reality of our imagination
Matthew W. Milligan Electric Fields a figment reality of our imagination Electrostatics I. Charge and Force - concepts and definition - Coulomb s Law II. Field and Potential - electric field strength &
More informationWelcome to Physics 211! General Physics I
Welcome to Physics 211! General Physics I Physics 211 Fall 2015 Lecture 01-1 1 Physics 215 Honors & Majors Are you interested in becoming a physics major? Do you have a strong background in physics and
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 informationChapters 22/23: Potential/Capacitance Tuesday September 20 th
Chapters 22/23: Potential/Capacitance Tuesday September 20 th Mini Exam 2 on Thursday: Covers Chs. 21 and 22 (Gauss law and potential) Covers LONCAPA #3 to #6 (due this Wed.) No formula sheet allowed!!
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 informationElectric Potential (Chapter 25)
Electric Potential (Chapter 25) Electric potential energy, U Electric potential energy in a constant field Conservation of energy Electric potential, V Relation to the electric field strength The potential
More informationPhysics 2D Lecture Slides Lecture 1: Jan
Physics 2D Lecture Slides Lecture 1: Jan 5 2004 Vivek Sharma UCSD Physics Modern Physics (PHYS 2D) Exploration of physical ideas and phenomena related to High velocities and acceleration ( Einstein s Theory
More informationPhysics 115. AC circuits Reactances Phase relationships Evaluation. General Physics II. Session 35. R. J. Wilkes
Session 35 Physics 115 General Physics II AC circuits Reactances Phase relationships Evaluation R. J. Wilkes Email: phy115a@u.washington.edu 06/05/14 1 Lecture Schedule Today 2 Announcements Please pick
More informationElectrostatics and Electric Potential - Outline
Electrostatics and Electric Potential - Outline 1. Understand the basic properties of electric charge, including conservation of charge and that charges are quantized. 2. Differentiate between conductors
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 informationCapacitors II. Physics 2415 Lecture 9. Michael Fowler, UVa
Capacitors II Physics 2415 Lecture 9 Michael Fowler, UVa Today s Topics First, some review then Storing energy in a capacitor How energy is stored in the electric field Dielectrics: why they strengthen
More informationLecture 16.1 :! Final Exam Review, Part 2
Lecture 16.1 :! Final Exam Review, Part 2 April 28, 2015 1 Announcements Online Evaluation e-mails should have been sent to you.! Please fill out the evaluation form. May 6 is deadline.! Remember that
More informationPhysics 1402: Lecture 12 Today s Agenda
Physics 1402: Lecture 12 Today s Agenda Announcements: Lectures posted on: www.phys.uconn.edu/~rcote/ HW assignments, solutions etc. Homework #4: On Masterphysics : due next Friday at 8:00 AM Go to masteringphysics.com
More informationGeneral Physics (PHY 2140)
General Physics (PHY 2140) Lecture 2 Electrostatics Electric flux and Gauss s law Electrical energy potential difference and electric potential potential energy of charged conductors http://www.physics.wayne.edu/~alan/
More informationAgenda for Today. Elements of Physics II. Capacitors Parallel-plate. Charging of capacitors
Capacitors Parallel-plate Physics 132: Lecture e 7 Elements of Physics II Charging of capacitors Agenda for Today Combinations of capacitors Energy stored in a capacitor Dielectrics in capacitors Physics
More informationCapacitors. HPP Activity 68v1. Charge Inside the Body A Close Look at Cell Membranes
HPP Activity 68v1 Capacitors Charge Inside the Body A Close Look at Cell Membranes Our bodies store and use charge to transmit signals across nerves and to tell certain cells what to do and when to do
More informationEnd-of-Chapter Exercises
End-of-Chapter Exercises Exercises 1 12 are primarily conceptual questions designed to see whether you understand the main concepts of the chapter. 1. (a) If the electric field at a particular point is
More informationPhysics 202, Lecture 8. Exam 1
Physics 202, Lecture 8 Today s Topics More on Exam 1: logistics and mini-review Current And Resistance (Ch. 27) Current: Macroscopic and Microscopic Resistance: Macroscopic and Microscopic Electrical Power
More informationPhysics 2D Lecture Slides Sep 26. Vivek Sharma UCSD Physics
Physics 2D Lecture Slides Sep 26 Vivek Sharma UCSD Physics Modern Physics (PHYS 2D) Exploration of physical ideas and phenomena related to High velocities and acceleration ( Einstein s Theory of Relativity)
More informationAnnouncements 13 Nov 2014
Announcements 13 Nov 2014 1. Prayer 2. Exam 3 starts on Tues Nov 25 a. Covers Ch 9-12, HW 18-24 b. Late fee on Wed after Thanksgiving, 3 pm c. Closes on Thursday after Thanksgiving, 3 pm d. Jerika review
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 informationUNIVERSITY OF TORONTO Department of Electrical and Computer Engineering ECE320H1-F: Fields and Waves, Course Outline Fall 2013
UNIVERSITY OF TORONTO Department of Electrical and Computer Engineering ECE320H1-F: Fields and Waves, Course Outline Fall 2013 Name Office Room Email Address Lecture Times Professor Mo Mojahedi SF2001D
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 informationPHY132 Introduction to Physics II Class 9 Outline:
PHY132 Introduction to Physics II Class 9 Outline: Finishing off chapter 25, Starting chapter 26.. The Field Model The Electric Field of a Point Charge, and many point charges Class 9 Preclass Quiz on
More informationPhysics 1302W.500 Lecture 9 Introductory Physics for Scientists and Engineering II
Physics 1302W.500 Lecture 9 Introductory Physics for Scientists and Engineering II In today s lecture, we will finish our discussion of Gauss law. Slide 25-1 Applying Gauss s law Procedure: Calculating
More informationPhysics 122 Class #11 Outline. Announcements Coulomb's Law Interferometer Interference Single slit Huyghens principle
Physics 1 Class #11 Outline Announcements Coulomb's Law Interferometer Interference Single slit Huyghens principle Reading This Week ALL of Chapter 5 It is key to rest of course. Next Week Chapter 6 Main
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 informationPhysics 1B Electricity & Magnetism. Frank Wuerthwein (Prof) Edward Ronan (TA) UCSD
Physics 1B Electricity & Magnetism Frank Wuerthwein (Prof) Edward Ronan (TA) UCSD Outline of today Continue Chapter 20. Electric potential (or voltage) and potential energy Remember: Quiz 1 is next Friday,
More informationGeneral Physics (PHY 2140)
General Physics (PHY 2140) Lecture 5 Electrostatics Electrical energy potential difference and electric potential potential energy of charged conductors Capacitance and capacitors http://www.physics.wayne.edu/~apetrov/phy2140/
More informationPhysics 12 ELECTROSTATICS
Physics 12 ELECTROSTATICS F = kq 1Q 2 r2 E = V d V = kq r E p = kq 1Q 2 r F = qe V = E p Q 1 000 000 Volts 1 000 000 Volts NAME: Block: Text References 3 rd Ed. Giancolli Pg. 416-30 4 th Ed. Giancolli
More informationGeneral Physics (PHY 2140)
General Physics (PHY 2140) Lecture 4 Electrostatics Electric flux and Gauss s law Electrical energy potential difference and electric potential potential energy of charged conductors http://www.physics.wayne.edu/~apetrov/phy2140/
More informationSection 1: Electric Fields
PHY 132 Outline of Lecture Notes i Section 1: Electric Fields A property called charge is part of the basic nature of protons and electrons. Large scale objects become charged by gaining or losing electrons.
More informationGeneral Chemistry I: Structure
General Chemistry I: Structure Chemistry 121 Dr. Jay H. Baltisberger Science Bldg. Room 304 x6274 In this course I hope to introduce you to the fundamentals of chemistry. As an introductory course which
More informationF 13. The two forces are shown if Q 2 and Q 3 are connected, their charges are equal. F 12 = F 13 only choice A is possible. Ans: Q2.
Q1. Three fixed point charges are arranged as shown in Figure 1, where initially Q 1 = 10 µc, Q = 15 µc, and Q 3 = 5 µc. If charges Q and Q 3 are connected by a very thin conducting wire and then disconnected,
More informationElectric Potential. 1/22/14 Physics for Scientists & Engineers 2, Chapter 23 1
Electric Potential 1/22/14 Physics for Scientists & Engineers 2, Chapter 23 1 Announcements! First exam is next Tuesday, January 28 45 minute exam during lecture time You can bring a 5 by 8 size cheat
More informationGEORGETOWN UNIVERSITY Department of Chemistry General Chemistry II - Summer General Information for CHEM 002 and CHEM 010
GEORGETOWN UNIVERSITY Department of Chemistry General Chemistry II - Summer 2018 General Information for CHEM 002 and CHEM 010 Prof. Diana C. Glick (Lecture and Lab) Regents Hall 211A 687-5961 glickdc@georgetown.edu
More informationCHEMISTRY 101 DETAILED WEEKLY TEXTBOOK HOMEWORK & READING SCHEDULE*
CHEMISTRY 101 COURSE POLICIES 15 CHEMISTRY 101 DETAILED WEEKLY TEXTBOOK HOMEWORK & READING SCHEDULE* *Refer to textbook homework assignment and pre-lecture assignment for corresponding chapters to read.
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 informationCh. 16 and 17 Review Problems
Ch. 16 and 17 Review Problems NAME 1) Is it possible for two negative charges to attract each other? A) Yes, they always attract. B) Yes, they will attract if they are close enough. C) Yes, they will attract
More informationGEOLOGY 100 Planet Earth Spring Semester, 2007
GEOLOGY 100 Planet Earth Spring Semester, 2007 Instructor: Michael A. Stewart, 250 Natural History Building Phone: 244-5025 Email: stewart1@uiuc.edu Office hours: Friday 1:00-2:30 pm by appointment Discussion
More informationAgenda for Today. Elements of Physics II. Capacitors Parallel-plate. Charging of capacitors
Capacitors Parallel-plate Physics 132: Lecture e 7 Elements of Physics II Charging of capacitors Agenda for Today Combinations of capacitors Energy stored in a capacitor Dielectrics in capacitors Physics
More informationElectric Fields and Potentials
Electric Fields and Potentials INTRODUCTION Physicists use the concept of a field to explain the interaction of particles or bodies through space, i.e., the action-at-a-distance force between two bodies
More informationCHEMISTRY 101 DETAILED WEEKLY TEXTBOOK HOMEWORK & READING SCHEDULE *
CHEMISTRY 101 COURSE POLICIES 15 CHEMISTRY 101 DETAILED WEEKLY TEXTBOOK HOMEWORK & READING SCHEDULE * * Refer to textbook homework assignment and pre-lecture assignment for corresponding chapters to read.
More informationChapter 21 Electric Potential
Chapter 21 Electric Potential Chapter Goal: To calculate and use the electric potential and electric potential energy. Slide 21-1 Chapter 21 Preview Looking Ahead Text: p. 665 Slide 21-2 Review of Potential
More informationElectric Charges and Forces. Lecture 1. Chapter 25. Physics II. Course website:
Lecture 1 Chapter 25 Physics II Electric Charges and Forces 95.144 Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsii Course Website Everything you need to know about the course can
More informationVersion: A. Earth s gravitational field g = 9.81 N/kg Mass of a Proton m p = kg
PHYS 2212 G & J Quiz and Exam Formulæ & Constants Fall 2017 Fundamental Charge e = 1.602 10 19 C Mass of an Electron m e = 9.109 10 31 kg Earth s gravitational field g = 9.81 N/kg Mass of a Proton m p
More information