PHYS 272: Electric and Magnetic Interactions Electric Fields and Circuits

Size: px
Start display at page:

Download "PHYS 272: Electric and Magnetic Interactions Electric Fields and Circuits"

Transcription

1 Jonathan Nistor (Purdue University) 7/09/ / 14 PHYS 272: Electric and Magnetic Interactions Electric Fields and Circuits Jonathan Nistor Monday, July 9 th, 2012

2 Jonathan Nistor (Purdue University) 7/09/ / 14 Electric Field and Circuits 19.1 Introduction and Overview 19.2 Current throughout a circuit 19.3 Electric Field and Current 19.4 What charges make the E-field in the wires

3 Overview Electron and Conventional Currents Recall that the electron current, i, is defined as the number of electrons per second that enter a section of a conductor For a metal with a cross sectional area A, and density of mobile electrons, n, then: where Units: # of electrons/sec is the mean (average) drift speed of the electrons (1) Conventional current,, is define as the amount of charge (in coulombs) entering a region per second. Therefore, Units: Coulombs/sec (2) Conventional current is assumed to consist of the motion of positive charges, and therefore flows in the direction of E net Jonathan Nistor (Purdue University) 7/09/ / 14

4 Jonathan Nistor (Purdue University) 7/09/ / 14 Overview Electron and Conventional Currents Conventional current is assumed to consist of the motion of positive charges, and therefore flows in the direction of E net Conventional current E Electron current Electron current, i,points in the direction of the drift velocity,

5 Jonathan Nistor (Purdue University) 7/09/ / 14 Overview Equilibrium and Steady-State A metal is in Equilibrium when there is no current flow: i.e. No charges are moving. Does E net necessarily have to be zero? A conductor is in a steady-state if charges are moving, but their drift velocities at any location do not change with time. Furthermore, there is no change in the deposits of excess charge anywhere This doesn t mean that the electron drift velocity must be the same at every location. The drift velocities of charges may be different at different locations:

6 Jonathan Nistor (Purdue University) 7/09/ / 14 The Current Node Rule nodes Conservation of charge is a fundamental physical principle which guarantees that the total net charge in a system in conserved (constant) As such, if a conductor is in the steady state, where no excess deposits of charge occur, then the amount of charge entering a particular region (node), must be equal to the amount of charge leaving that same region in the same amount of time. Written as the current node rule (Kirchhoff 1 st Law) In the steady state, the electron current entering a node in a circuit is equal to the electron current leaving that node i 1 = i 2 i 2 = i 3 + i 4

7 Jonathan Nistor (Purdue University) 7/09/ / 14 Current Node Rule: Example Write the node equation for this circuit. What is the value of I 2? I 1 + I 4 = I 2 + I 3 I 2 = I 1 + I 4 - I 3 = 3A Write the node equations for this circuit

8 Jonathan Nistor (Purdue University) 7/09/ / 14 Current Node Rule: Generalized nodes node #1 node #2 How many non-trivial nodes are there? (1) (2) (3) node #3 In general, a node can be any boundary which contains portions of a circuit in steady-state

9 Jonathan Nistor (Purdue University) 7/09/ / 14 Electric Field and Current In a current-carrying wire, there must be an electric field to drive the sea of mobile charges What is the relationship between current and the electric field? Why is an electric field require to maintain a flow of charge (current)? i.e. Once current is flowing, why is an electric force required to keep the electrons moving at a constant drift speed? Do the electrons push each other? Can there be excess charges inside a conductor in the steady state? We already know that there cannot be excess charges inside a conductor in equilibrium! What charges produce the electric field inside the wire?

10 Jonathan Nistor (Purdue University) 7/09/ / 14 The Drude Model What is the relationship between current and the electric field? Why is an electric field require to maintain a flow of charge (current)? E Start From the Momentum Principle: p Fnet t eet p p 0 p eet The speed of the electron is: v m The average drift speed is: v ee t m e e m e eet where t is the average time between collisions

11 Jonathan Nistor (Purdue University) 7/09/ / 14 The Drude Model The average drift speed is: t v ee t m e is a property of the conductor. Dependent on: Lattice arrangement of atomic cores Density of metal Temperature of metal, why? t is NOT dependent on the applied electric field Therefore, v ~ E (for constant temperatures) where t is the average time between collisions We can write, where u is called the electron mobility The electron current is therefore: Paul Drude ( )

12 Jonathan Nistor (Purdue University) 7/09/ / 14 Typical E-Field in a wire Drift speed in a copper wire in a typical circuit is m/s. The mobility of copper is u= (m/s)/(n/c). Calculate E. E v u m/s (m/s)/(n/c) N/C Electric field in a wire in a typical circuit is very small

13 Electric Field and Drift Speed In steady state current is the same everywhere in a series circuit. i E thin E thick i What is the relationship between the drift speeds in the thin and thick wires? i nav Athick nathinv thin nathick v v thick thin vthick A Note: density of electrons n cannot change if same metal What about E? v ue A thin thick thick uethin uethick Ethin Ethick Athin Athin Jonathan Nistor (Purdue University) 7/09/ / 14 A

14 Direction of Electric Field in a Wire E must be parallel to the wire, why? E is the same along the wire, how do we know this? Is E uniform across the wire? V ABCDA B E A C D A 1 dl E3 dl E2 dl E3 dl V AB B E 1 E 2 C D 0 0 Jonathan Nistor (Purdue University) 7/09/ / 14 V CD 0

Last Time. Magnetic Field of a Straight Wire Magnetic Field of a Current Loop Magnetic Dipole Moment Bar Magnet Electron Spin

Last Time. Magnetic Field of a Straight Wire Magnetic Field of a Current Loop Magnetic Dipole Moment Bar Magnet Electron Spin Last Time Magnetic Field of a Straight Wire Magnetic Field of a Current Loop Magnetic Dipole Moment Bar Magnet Electron Spin 1 Today Equilibrium vs. Steady State in a Circuit What is "used up" in a circuit?

More information

Last Time. Equilibrium vs. Steady State in a Circuit What is "used up" in a circuit? Kirchhoff's Current Node Law E-field inside a wire

Last Time. Equilibrium vs. Steady State in a Circuit What is used up in a circuit? Kirchhoff's Current Node Law E-field inside a wire Last Time Equilibrium vs. Steady State in a Circuit What is "used up" in a circuit? Kirchhoff's Current Node Law E-field inside a wire 1 Electric Field Inside the Wire Constant current in the wire Constant

More information

Electric currents (primarily, in metals)

Electric currents (primarily, in metals) Electric currents (primarily, in metals) Benjamin Franklin was experimenting electricity in the mid- XVIII Century. Nobody knew if it was the positive charges or negative charges carrying the current through

More information

Need to finish these notes off, a candidate came this day, and I didn t actually run class.

Need to finish these notes off, a candidate came this day, and I didn t actually run class. Fri., 2/20 18.8-10 Energy, Applications of the Theory Exp 18,19,22-24 Spring Recess Mon., 3/2 Tues., 3/3 Wed., 3/4 Thurs., 3/5 19.1-5 Capacitor Circuits 19.6-.14 Capacitor & Resistor Circuits Quiz Ch 18,

More information

Chapter 26 & 27. Electric Current and Direct- Current Circuits

Chapter 26 & 27. Electric Current and Direct- Current Circuits Chapter 26 & 27 Electric Current and Direct- Current Circuits Electric Current and Direct- Current Circuits Current and Motion of Charges Resistance and Ohm s Law Energy in Electric Circuits Combination

More information

Matter & Interactions Chapter 18 Solutions

Matter & Interactions Chapter 18 Solutions Q12: To quote from pg. 769 of the textbook, It is important to keep in mind that although the units of emf are volts, the emf is not a potential difference. Potential difference is a path integral of the

More information

Chapter 14: Electric Fields and Matter

Chapter 14: Electric Fields and Matter Chapter 14: Electric Fields and Matter We extend the concepts of charge and electric fields due to point particles (and dipoles) to macroscopic objects In terms of their response to electric fields, we

More information

PHY102 Electricity Course Summary

PHY102 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 information

Physics 1302W.400 Lecture 21 Introductory Physics for Scientists and Engineering II

Physics 1302W.400 Lecture 21 Introductory Physics for Scientists and Engineering II Physics 1302W.400 Lecture 21 Introductory Physics for Scientists and Engineering II In today s lecture, we will learn to: Calculate the resistance of a conductor depending on the material and shape Apply

More information

1 Written and composed by: Prof. Muhammad Ali Malik (M. Phil. Physics), Govt. Degree College, Naushera

1 Written and composed by: Prof. Muhammad Ali Malik (M. Phil. Physics), Govt. Degree College, Naushera CURRENT ELECTRICITY Q # 1. What do you know about electric current? Ans. Electric Current The amount of electric charge that flows through a cross section of a conductor per unit time is known as electric

More information

PHYSICS 272 Electric & Magnetic Interactions

PHYSICS 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 information

Potential. The electrostatic field Is conservative (just like gravity) The (minimum) work done to move q from a to b:

Potential. The electrostatic field Is conservative (just like gravity) The (minimum) work done to move q from a to b: The electrostatic field Is conservative (just like gravity) dl Potential The (minimum) work done to move q from a to b: W q b a b a F dl E dl The meaning of the negative sign: An external force F is exerted

More information

matschek (ccm2548) Ch19-h1 chiu (57890) 1

matschek (ccm2548) Ch19-h1 chiu (57890) 1 matschek (ccm2548) Ch19-h1 chiu (57890) 1 This print-out should have 15 questions. Multiple-choice questions may continue on the next column or page find all choices before answering. 001 (part 1 of 2)

More information

EECS 117 Lecture 13: Method of Images / Steady Currents

EECS 117 Lecture 13: Method of Images / Steady Currents EECS 117 Lecture 13: Method of Images / Steady Currents Prof. Niknejad University of California, Berkeley University of California, Berkeley EECS 217 Lecture 13 p. 1/21 Point Charge Near Ground Plane Consider

More information

FXA 2008 ELECTRIC CHARGE (Q) 1. Candidates should be able to : Electric charge is a property possessed by protons and electrons.

FXA 2008 ELECTRIC CHARGE (Q) 1. Candidates should be able to : Electric charge is a property possessed by protons and electrons. ELECTRIC CHARGE (Q) 1 Candidates should be able to : Explain that electric current is a net flow of charged particles. Explain that electric current in a metal is due to the movement of electrons, whereas

More information

Chapter 25: Electric Current

Chapter 25: Electric Current Chapter 25: Electric Current Conductors and Charge Carriers Consider a conducting piece of metal: The valence electrons are weakly bound to the nuclei form a fluidlike sea of electrons that can move through

More information

2015 EdExcel A-Level Physics Topic 3. Resistivity and I=nAqv

2015 EdExcel A-Level Physics Topic 3. Resistivity and I=nAqv 2015 EdExcel A-Level Physics Topic 3 Resistivity and I=nAqv 10/25/2017 Factors affecting the resistance of a wire The resistance of a wire depends on 3 things: the length of the wire, the width of the

More information

E40M Charge, Current, Voltage and Electrical Circuits. M. Horowitz, J. Plummer, R. Howe 1

E40M Charge, Current, Voltage and Electrical Circuits. M. Horowitz, J. Plummer, R. Howe 1 E40M Charge, Current, Voltage and Electrical Circuits M. Horowitz, J. Plummer, R. Howe 1 Understanding the Solar Charger Lab Project #1 We need to understand how: 1. Current, voltage and power behave in

More information

10/14/2018. Current. Current. QuickCheck 30.3

10/14/2018. Current. Current. QuickCheck 30.3 Current If QCurrent is the total amount of charge that has moved past a point in a wire, we define the current I in the wire to be the rate of charge flow: The SI unit for current is the coulomb per second,

More information

PHYSICS. Chapter 27 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT

PHYSICS. Chapter 27 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT PHYSICS FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E Chapter 27 Lecture RANDALL D. KNIGHT Chapter 27 Current and Resistance IN THIS CHAPTER, you will learn how and why charge moves through a wire

More information

PHYS102 - Gauss s Law.

PHYS102 - Gauss s Law. PHYS102 - Gauss s Law. Dr. Suess February 2, 2007 PRS Questions 2 Question #1.............................................................................. 2 Answer to Question #1......................................................................

More information

AP Physics C. Electric Circuits III.C

AP Physics C. Electric Circuits III.C AP Physics C Electric Circuits III.C III.C.1 Current, Resistance and Power The direction of conventional current Suppose the cross-sectional area of the conductor changes. If a conductor has no current,

More information

Chapter 3: Current and Resistance. Direct Current Circuits

Chapter 3: Current and Resistance. Direct Current Circuits Chapter 3: Current and Resistance. Direct Current Circuits 3.1. Electric Current 3.2. Resistance and Resistivity 3.3. Ohm s Law and a Microscopic View of Ohm s Law 3.4. Semiconductors and Superconductors

More information

Semiconductor Physics. Lecture 3

Semiconductor Physics. Lecture 3 Semiconductor Physics Lecture 3 Intrinsic carrier density Intrinsic carrier density Law of mass action Valid also if we add an impurity which either donates extra electrons or holes the number of carriers

More information

Chapter 33 - Electric Fields and Potential. Chapter 34 - Electric Current

Chapter 33 - Electric Fields and Potential. Chapter 34 - Electric Current Chapter 33 - Electric Fields and Potential Chapter 34 - Electric Current Electric Force acts through a field An electric field surrounds every electric charge. It exerts a force that causes electric charges

More information

Physics 12 Final exam review key

Physics 12 Final exam review key Physics 12 Final exam review key 1) A scalar field differs from a vector field in that A. a scalar field acts in only one direction B. a vector field acts in only one direction C. direction is irrelevant

More information

Reading from Young & Freedman: For this topic, read the introduction to chapter 25 and sections 25.1 to 25.3 & 25.6.

Reading from Young & Freedman: For this topic, read the introduction to chapter 25 and sections 25.1 to 25.3 & 25.6. PHY10 Electricity Topic 6 (Lectures 9 & 10) Electric Current and Resistance n this topic, we will cover: 1) Current in a conductor ) Resistivity 3) Resistance 4) Oh s Law 5) The Drude Model of conduction

More information

The Steady Current Field

The Steady Current Field Electromagnetic Fields Lecture 5 The Steady Current Field What is current? Electric current: Flow of electric charge. Electric current in metals A solid conductive metal contains free electrons. When a

More information

Phys102 General Physics II. Chapter 24: Gauss s Law

Phys102 General Physics II. Chapter 24: Gauss s Law Phys102 General Physics II Gauss Law Chapter 24: Gauss s Law Flux Electric Flux Gauss Law Coulombs Law from Gauss Law Isolated conductor and Electric field outside conductor Application of Gauss Law Charged

More information

By Mir Mohammed Abbas II PCMB 'A' CHAPTER FORMULAS & NOTES. 1. Current through a given area of a conductor is the net charge passing

By Mir Mohammed Abbas II PCMB 'A' CHAPTER FORMULAS & NOTES. 1. Current through a given area of a conductor is the net charge passing Formulae For u CURRENT ELECTRICITY 1 By Mir Mohammed Abbas II PCMB 'A' 1 Important Terms, Definitions & Formulae CHAPTER FORMULAS & NOTES 1. Current through a given area of a conductor is the net charge

More information

Chapter 27. Current And Resistance

Chapter 27. Current And Resistance Chapter 27 Current And Resistance Electric Current Electric current is the rate of flow of charge through some region of space The SI unit of current is the ampere (A) 1 A = 1 C / s The symbol for electric

More information

Exam 1--PHYS 202--Spring 2013

Exam 1--PHYS 202--Spring 2013 Name: Class: Date: Exam 1--PHYS 202--Spring 2013 Multiple Choice Identify the choice that best completes the statement or answers the question 1 A metallic object holds a charge of 38 10 6 C What total

More information

Physics 202: Lecture 5, Pg 1

Physics 202: Lecture 5, Pg 1 Resistance Resistors Series Parallel Ohm s law Electric Circuits Current Physics 132: Lecture e 15 Elements of Physics II Kirchhoff s laws Agenda for Today Physics 202: Lecture 5, Pg 1 Electric Current

More information

Gauss s Law. Phys102 Lecture 4. Key Points. Electric Flux Gauss s Law Applications of Gauss s Law. References. SFU Ed: 22-1,2,3. 6 th Ed: 16-10,+.

Gauss s Law. Phys102 Lecture 4. Key Points. Electric Flux Gauss s Law Applications of Gauss s Law. References. SFU Ed: 22-1,2,3. 6 th Ed: 16-10,+. Phys102 Lecture 4 Phys102 Lecture 4-1 Gauss s Law Key Points Electric Flux Gauss s Law Applications of Gauss s Law References SFU Ed: 22-1,2,3. 6 th Ed: 16-10,+. Electric Flux Electric flux: The direction

More information

Exam 1--PHYS 102--Spring 2013

Exam 1--PHYS 102--Spring 2013 ame: Class: Date: Exam 1--PHYS 102--Spring 2013 Multiple Choice Identify the choice that best completes the statement or answers the question. 1. A metallic object holds a charge of 3.8 10 6 C. What total

More information

Chapter 27. Current and Resistance

Chapter 27. Current and Resistance Chapter 27 Current and Resistance Electric Current Most practical applications of electricity deal with electric currents. The electric charges move through some region of space. The resistor is a new

More information

Electric Currents and Circuits

Electric Currents and Circuits Nicholas J. Giordano www.cengage.com/physics/giordano Chapter 19 Electric Currents and Circuits Marilyn Akins, PhD Broome Community College Electric Circuits The motion of charges leads to the idea of

More information

Current and Resistance

Current and Resistance Chapter 26 Current and Resistance Copyright 26-1 Electric Current As Fig. (a) reminds us, any isolated conducting loop regardless of whether it has an excess charge is all at the same potential. No electric

More information

A) B/2 B) 4B C) B/4 D) 8B E) 2B

A) B/2 B) 4B C) B/4 D) 8B E) 2B A long straight wire carries a current I. If the magnetic field a distance d from the wire has a magnitude B, what is the magnitude of the magnetic field at a distance 2d from the wire? A) B/2 B) 4B C)

More information

1. How much charge is stored in a capacitor, whose capacitance C = 2µF, connected to a 12V battery?

1. How much charge is stored in a capacitor, whose capacitance C = 2µF, connected to a 12V battery? IMP 113: 2 nd test (Union College: Spring 2010) Instructions: 1. Read all directions. 2. In keeping with the Union College policy on academic honesty, you should neither accept nor provide unauthorized

More information

Electrostatics. 4πε 2) + Q / 2 4) 4 Q

Electrostatics. 4πε 2) + Q / 2 4) 4 Q Two spheres A and B of radius a and b respectively are at the same potential The ratio of the surface charge density of A to B is: ) a / b ) b / a a / b b / a Two free protons are separated by a distance

More information

Current. source charges. test charg. 1. Charges in motion

Current. source charges. test charg. 1. Charges in motion Current 1. Charges in motion 1. Cause of motion 2. Where is it going? 3. Let's keep this going. 2. Current 1. Flow of particles in pipes. 2. A constant problem 3. Conservation Laws 4. Microscopic motion

More information

Conducting surface - equipotential. Potential varies across the conducting surface. Lecture 9: Electrical Resistance.

Conducting surface - equipotential. Potential varies across the conducting surface. Lecture 9: Electrical Resistance. Lecture 9: Electrical Resistance Electrostatics (time-independent E, I = 0) Stationary Currents (time-independent E and I 0) E inside = 0 Conducting surface - equipotential E inside 0 Potential varies

More information

The Cyclotron I. 1. Motion of the charges occurs in two semicircular containers, D 1. and D 2

The Cyclotron I. 1. Motion of the charges occurs in two semicircular containers, D 1. and D 2 1. Motion of the charges occurs in two semicircular containers, D 1 and D 2 referred to as the Dees 2. The Dees are evacuated in order to minimize energy loss from collisions 3. A high frrequency alternating

More information

CHAPTER 7 ELECTRODYNAMICS

CHAPTER 7 ELECTRODYNAMICS CHAPTER 7 ELECTRODYNAMICS Outlines 1. Electromotive Force 2. Electromagnetic Induction 3. Maxwell s Equations Michael Faraday James C. Maxwell 2 Summary of Electrostatics and Magnetostatics ρ/ε This semester,

More information

(a) zero. B 2 l 2. (c) (b)

(a) zero. B 2 l 2. (c) (b) 1. Two identical co-axial circular loops carry equal currents circulating in the same direction: (a) The current in each coil decrease as the coils approach each other. (b) The current in each coil increase

More information

General Physics - E&M (PHY 1308) - Lecture Notes. General Physics - E&M (PHY 1308) Lecture Notes

General Physics - E&M (PHY 1308) - Lecture Notes. General Physics - E&M (PHY 1308) Lecture Notes General Physics - E&M (PHY 1308) Lecture Notes Lecture 029: Forms of Induction and Self-Inductance SteveSekula, 8 November 2010 (created 7 November 2010) Goals of this Lecture no tags Further understand

More information

Chapter 21: Gauss law Tuesday September 13 th. Gauss law and conductors Electrostatic potential energy (more likely on Thu.)

Chapter 21: Gauss law Tuesday September 13 th. Gauss law and conductors Electrostatic potential energy (more likely on Thu.) Chapter 21: Gauss law Tuesday September 13 th LABS START THIS WEEK Quick review of Gauss law The flux of a vector field The shell theorem Gauss law for other symmetries A uniformly charged sheet A uniformly

More information

Phys 0175 Midterm Exam III Solutions Apr 3, 2008

Phys 0175 Midterm Exam III Solutions Apr 3, 2008 Phys 0175 Midterm Exam III Solutions Apr 3, 2008 1. (8 pts) A particular capacitor has a separation between its plates of 0.03 mm. The area of one plate is 16 m 2. The capacitor is initially uncharged.

More information

ECE 1311: Electric Circuits. Chapter 2: Basic laws

ECE 1311: Electric Circuits. Chapter 2: Basic laws ECE 1311: Electric Circuits Chapter 2: Basic laws Basic Law Overview Ideal sources series and parallel Ohm s law Definitions open circuits, short circuits, conductance, nodes, branches, loops Kirchhoff's

More information

Physics 272: Electricity and Magnetism. Mark Palenik Thursday June 14 th

Physics 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 information

Chapter 26 Current and Resistance

Chapter 26 Current and Resistance Chapter 26 Current and Resistance Electric Current Although an electric current is a stream of moving charges, not all moving charges constitute an electric current. If there is to be an electric current

More information

B Field Creation Detecting B fields. Magnetic Fields. PHYS David Blasing. Wednesday June 26th 1 / 26

B Field Creation Detecting B fields. Magnetic Fields. PHYS David Blasing. Wednesday June 26th 1 / 26 Magnetic Fields PHYS 272 - David Blasing Wednesday June 26th 1 / 26 Magnetic ( B) Fields This is a significant change, until now we have discussed just E fields. Now we are talking about a totally different

More information

Note 5: Current and Resistance

Note 5: Current and Resistance Note 5: Current and Resistance In conductors, a large number of conduction electrons carry electricity. If current flows, electrostatics does not apply anymore (it is a dynamic phenomenon) and there can

More information

E40M Charge, Current, Voltage and Electrical Circuits KCL, KVL, Power & Energy Flow. M. Horowitz, J. Plummer, R. Howe 1

E40M Charge, Current, Voltage and Electrical Circuits KCL, KVL, Power & Energy Flow. M. Horowitz, J. Plummer, R. Howe 1 E40M Charge, Current, Voltage and Electrical Circuits KCL, KVL, Power & Energy Flow M. Horowitz, J. Plummer, R. Howe 1 Reading For Topics In These Slides Chapter 1 in the course reader OR A&L 1.6-1.7 -

More information

The Steady Magnetic Field LECTURE 7

The Steady Magnetic Field LECTURE 7 The Steady Magnetic Field LECTURE 7 Learning Objectives Understand the Biot-Savart Law Understand the Ampere s Circuital Law Explain the Application of Ampere s Law Motivating the Magnetic Field Concept:

More information

PHYS 2135 Engineering Physics II Fall Course Information: Canvas and Course Website Begin with Course Handbook and Syllabus

PHYS 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 information

f n+2 f n = 2 = = 40 H z

f n+2 f n = 2 = = 40 H z Coordinator: Dr.I.M.Nasser Monday, May 18, 2015 Page: 1 Q1. Q2. One end of a stretched string vibrates with a period of 1.5 s. This results in a wave propagating at a speed of 8.0 m/s along the string.

More information

A free web support in Education. Internal resistance of the battery, r = 3 Ω. Maximum current drawn from the battery = I According to Ohm s law,

A free web support in Education. Internal resistance of the battery, r = 3 Ω. Maximum current drawn from the battery = I According to Ohm s law, Exercises Question 3.1: The storage battery of a car has an emf of 12 V. If the internal resistance of the battery is 0.4Ω, what is the maximum current that can be drawn from the battery? Answer 3.1: Emf

More information

Chapter 27. Current And Resistance

Chapter 27. Current And Resistance Chapter 27 Current And Resistance Electric Current Electric current is the rate of flow of charge through some region of space The SI unit of current is the ampere (A) 1 A = 1 C / s The symbol for electric

More information

Reading Question 30.2

Reading Question 30.2 Reading Question 30.2 The speed of electrons in a typical current-carrying wire is A. Extremely slow ( 10 4 m/s). B. Moderate ( 1 m/s). C. Very fast ( 10 4 m/s). D. The speed of light. Slide 30-13 Electric

More information

Lecture 14. Magnetic Forces on Currents. Hall Effect. Magnetic Force on a Wire Segment. Torque on a Current-Carrying Loop.

Lecture 14. Magnetic Forces on Currents. Hall Effect. Magnetic Force on a Wire Segment. Torque on a Current-Carrying Loop. Lecture 14. Magnetic Forces on Currents. Outline: Hall Effect. Magnetic Force on a Wire Segment. Torque on a Current-Carrying Loop. Lecture 13: Magnetic Forces on Moving Charges - we considered individual

More information

R. W. Erickson. Department of Electrical, Computer, and Energy Engineering University of Colorado, Boulder

R. W. Erickson. Department of Electrical, Computer, and Energy Engineering University of Colorado, Boulder R. W. Erickson Department of Electrical, Computer, and Energy Engineering University of Colorado, Boulder Part III. Magnetics 13 Basic Magnetics Theory 14 Inductor Design 15 Transformer Design 1 Chapter

More information

A) I B) II C) III D) IV E) V

A) I B) II C) III D) IV E) V 1. A square loop of wire moves with a constant speed v from a field-free region into a region of uniform B field, as shown. Which of the five graphs correctly shows the induced current i in the loop as

More information

AP Physics Study Guide Chapter 17 Electric Potential and Energy Name. Circle the vector quantities below and underline the scalar quantities below

AP Physics Study Guide Chapter 17 Electric Potential and Energy Name. Circle the vector quantities below and underline the scalar quantities below AP Physics Study Guide Chapter 17 Electric Potential and Energy Name Circle the vector quantities below and underline the scalar quantities below electric potential electric field electric potential energy

More information

PHYSICS - CLUTCH CH 22: ELECTRIC FORCE & FIELD; GAUSS' LAW

PHYSICS - CLUTCH CH 22: ELECTRIC FORCE & FIELD; GAUSS' LAW !! www.clutchprep.com CONCEPT: ELECTRIC CHARGE e Atoms are built up of protons, neutrons and electrons p, n e ELECTRIC CHARGE is a property of matter, similar to MASS: MASS (m) ELECTRIC CHARGE (Q) - Mass

More information

9. Light-matter interactions - metals

9. Light-matter interactions - metals 9. Light-matter interactions - metals Complex dielectric function and complex refractive index The Drude model Optical properties of metals - skin depth - reflectivity A few announcements Reminder: no

More information

Physics 102 Spring 2007: Final Exam Multiple-Choice Questions

Physics 102 Spring 2007: Final Exam Multiple-Choice Questions Last Name: First Name: Physics 102 Spring 2007: Final Exam Multiple-Choice Questions 1. The circuit on the left in the figure below contains a battery of potential V and a variable resistor R V. The circuit

More information

Name: Class: Date: Multiple Choice Identify the letter of the choice that best completes the statement or answers the question.

Name: Class: Date: Multiple Choice Identify the letter of the choice that best completes the statement or answers the question. Name: Class: _ Date: _ w9final Multiple Choice Identify the letter of the choice that best completes the statement or answers the question. 1. If C = 36 µf, determine the equivalent capacitance for the

More information

Phys102 Second Major-161 Zero Version Coordinator: Dr. Naqvi Monday, December 12, 2016 Page: 1

Phys102 Second Major-161 Zero Version Coordinator: Dr. Naqvi Monday, December 12, 2016 Page: 1 Coordinator: Dr. Naqvi Monday, December 12, 2016 Page: 1 Q1. Two point charges, with charges q1 and q2, are placed a distance r apart. Which of the following statements is TRUE if the electric field due

More information

Lecture 24 Chapter 22 Electrostatics II Electric Field & Potential. Chapter 23 Electric Current. From last time--

Lecture 24 Chapter 22 Electrostatics II Electric Field & Potential. Chapter 23 Electric Current. From last time-- Lecture 24 Chapter 22 Electrostatics II Electric Field & Potential Chapter 23 Electric Current 21-Oct-10 From last time-- Electric charge (q), measured in Coulombs (C) Positive and negative charge Electric

More information

Electrons in a periodic potential: Free electron approximation

Electrons in a periodic potential: Free electron approximation Dr. A. Sapelin, Jan 01 Electrons in a periodic potential: ree electron approximation ree electron ermi gas - gas of non-interacting electrons subject to Pauli principle Wealy bound electrons move freely

More information

16EC401 BASIC ELECTRONIC DEVICES UNIT I PN JUNCTION DIODE. Energy Band Diagram of Conductor, Insulator and Semiconductor:

16EC401 BASIC ELECTRONIC DEVICES UNIT I PN JUNCTION DIODE. Energy Band Diagram of Conductor, Insulator and Semiconductor: 16EC401 BASIC ELECTRONIC DEVICES UNIT I PN JUNCTION DIODE Energy bands in Intrinsic and Extrinsic silicon: Energy Band Diagram of Conductor, Insulator and Semiconductor: 1 2 Carrier transport: Any motion

More information

General Physics (PHY 2140)

General 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 information

ESE 372 / Spring 2013 / Lecture 5 Metal Oxide Semiconductor Field Effect Transistor

ESE 372 / Spring 2013 / Lecture 5 Metal Oxide Semiconductor Field Effect Transistor Metal Oxide Semiconductor Field Effect Transistor V G V G 1 Metal Oxide Semiconductor Field Effect Transistor We will need to understand how this current flows through Si What is electric current? 2 Back

More information

PHY2054 Summer 2006 Exam 1 06 June 2006

PHY2054 Summer 2006 Exam 1 06 June 2006 PHY2054 Summer 2006 Exam 1 06 June 2006 Solutions Unless otherwise indicated, (1) is the correct answer. Solutions are, of necessity (due to the writer's self-taught & primitive word-processing skills),

More information

General Physics (PHY 2140)

General 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 information

PHYS 272 Fall 2010 Thursday, December 16, 2010

PHYS 272 Fall 2010 Thursday, December 16, 2010 PHYS 272 Fall 2010 Thursday, December 16, 2010 Final Exam The final exam has only this machine-graded part of 22 multiple choice questions. Each multiple choice problem is worth 10 points. Using a pencil,

More information

Physics 2212 G Quiz #4 Solutions Spring 2018 = E

Physics 2212 G Quiz #4 Solutions Spring 2018 = E Physics 2212 G Quiz #4 Solutions Spring 2018 I. (16 points) The circuit shown has an emf E, three resistors with resistance, and one resistor with resistance 3. What is the current through the resistor

More information

General Physics II (PHYS 104) Exam 2: March 21, 2002

General Physics II (PHYS 104) Exam 2: March 21, 2002 General Physics II (PHYS 104) Exam 2: March 21, 2002 Name: Multiple Choice (3 points each): Answer the following multiple choice questions. Clearly circle the response (or responses) that provides the

More information

Physics 202, Lecture 11

Physics 202, Lecture 11 Physics 202, Lecture 11 Today s Topics Magnetic Fields and Forces (Ch. 27) Magnetic materials Magnetic forces on moving point charges Magnetic forces on currents, current loops Motion of charge in uniform

More information

Chapter 9. Electric current. Developing ideas

Chapter 9. Electric current. Developing ideas Chapter 9 Electric current Objectives e-learning Developing ideas Electricity plays a vital part in our lives. We use electricity as a way of transferring energy from place to place for heating, lighting

More information

Lesson 10 Steady Electric Currents

Lesson 10 Steady Electric Currents Lesson Steady lectric Currents 楊尚達 Shang-Da Yang Institute of Photonics Technologies Department of lectrical ngineering National Tsing Hua Uniersity, Taiwan Outline Current density Current laws Boundary

More information

Exam 1 Solutions. The ratio of forces is 1.0, as can be seen from Coulomb s law or Newton s third law.

Exam 1 Solutions. The ratio of forces is 1.0, as can be seen from Coulomb s law or Newton s third law. Prof. Eugene Dunnam Prof. Paul Avery Feb. 6, 007 Exam 1 Solutions 1. A charge Q 1 and a charge Q = 1000Q 1 are located 5 cm apart. The ratio of the electrostatic force on Q 1 to that on Q is: (1) none

More information

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

Describe the forces and torques exerted on an electric dipole in a field. Learning Outcomes - PHYS 2015 Electric charges and forces: Describe the electrical nature of matter; Explain how an object can be charged; Distinguish between electrical conductors and insulators and the

More information

(Please print full name, underlining family name.)

(Please print full name, underlining family name.) (2016) Nationality No. PHYSICS Name (Please print full name, underlining family name.) Marks. 1. Suppose a system of three objects: a book, a table, and the earth. Let W be the gravitational force acting

More information

What are the two types of current? The two types of current are direct current and alternating current.

What are the two types of current? The two types of current are direct current and alternating current. Electric Current What are the two types of current? The two types of current are direct current and alternating current. Electric Current The continuous flow of electric charge is an electric current.

More information

Welcome 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 Welcome back to PHY101: Major Concepts in Physics I Photo: J. M. Schwarz Announcements In class today we will finish Chapter 18 on circuits and begin Chapter 19 (sections 1 and 8) on magnetic fields. There

More information

Slide 1. Temperatures Light (Optoelectronics) Magnetic Fields Strain Pressure Displacement and Rotation Acceleration Electronic Sensors

Slide 1. Temperatures Light (Optoelectronics) Magnetic Fields Strain Pressure Displacement and Rotation Acceleration Electronic Sensors Slide 1 Electronic Sensors Electronic sensors can be designed to detect a variety of quantitative aspects of a given physical system. Such quantities include: Temperatures Light (Optoelectronics) Magnetic

More information

Name: Class: Date: Multiple Choice Identify the letter of the choice that best completes the statement or answers the question.

Name: Class: Date: Multiple Choice Identify the letter of the choice that best completes the statement or answers the question. Name: Class: Date: AP REVIEW 4 Multiple Choice Identify the letter of the choice that best completes the statement or answers the question. 1. If a positively charged glass rod is used to charge a metal

More information

AP PHYSICS 2 Essential Knowledge and Learning Objectives Arranged Topically

AP PHYSICS 2 Essential Knowledge and Learning Objectives Arranged Topically with AP PHYSICS 2 Essential Knowledge and Learning Objectives Arranged Topically o Big Ideas o Enduring Understandings o Essential Knowledges o Learning Objectives o Science Practices o Correlation to

More information

4 Electric circuits. Serial and parallel resistors V 3 V 2 V Serial connection of resistors:

4 Electric circuits. Serial and parallel resistors V 3 V 2 V Serial connection of resistors: 4 lectric circuits PHY67 Spring 006 Serial and parallel resistors Serial connection of resistors: As the current I through each of serially connected resistors is the same, one can use Ohm s law and write...

More information

Part 11 - Physics Paper 2 Magnetism and Electromagnetism Combined Science Application Questions

Part 11 - Physics Paper 2 Magnetism and Electromagnetism Combined Science Application Questions Part 11 - Physics Paper 2 Magnetism and Electromagnetism Combined Science Application Questions Internal energy and energy transfers Internal energy and energy transfers Changes of state and the particle

More information

General Physics (PHY 2140)

General 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 information

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. Exam Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) A jeweler needs to electroplate gold (atomic mass 196.97 u) onto a bracelet. He knows

More information

Lecture 4: London s Equations. Drude Model of Conductivity

Lecture 4: London s Equations. Drude Model of Conductivity Lecture 4: London s Equations Outline 1. Drude Model of Conductivity 2. Superelectron model of perfect conductivity First London Equation Perfect Conductor vs Perfect Conducting Regime 3. Superconductor:

More information

11. ELECTRIC CURRENT. Questions and Answers between the forces F e and F c. 3. Write the difference between potential difference and emf. A.

11. ELECTRIC CURRENT. Questions and Answers between the forces F e and F c. 3. Write the difference between potential difference and emf. A. CLSS-10 1. Explain how electron flow causes electric current with Lorentz-Drude theory of electrons?. Drude and Lorentz, proposed that conductors like metals contain a large number of free electrons while

More information

wire z axis Under these assumptions, if we model the electrons by plane waves in the z direction we get n E, n, 1,2,

wire z axis Under these assumptions, if we model the electrons by plane waves in the z direction we get n E, n, 1,2, Part 4. Two Terminal Quantum Wire Devices Part 4. Two Terminal Quantum Wire Devices Let s consider a quantum wire between two contacts. As we saw in Part, a quantum wire is a one-dimensional conductor.

More information

Chapter 20. Capacitors, Resistors and Batteries

Chapter 20. Capacitors, Resistors and Batteries Chapter 20 Capacitors, Resistors and Batteries How is Discharging Possible?! E Positive and negative charges are attracted to each other: how can they leave the plates? Fringe field is not zero! Electrons

More information

Physics 22: Homework 4

Physics 22: Homework 4 Physics 22: Homework 4 The following exercises encompass problems dealing with capacitor circuits, resistance, current, and resistor circuits. 1. As in Figure 1, consider three identical capacitors each

More information