physics 4/7/2016 Chapter 31 Lecture Chapter 31 Fundamentals of Circuits Chapter 31 Preview a strategic approach THIRD EDITION

Similar documents
Agenda for Today. Elements of Physics II. Resistance Resistors Series Parallel Ohm s law Electric Circuits. Current Kirchoff s laws

Clicker Session Currents, DC Circuits

Chapter 21 Electric Current and Direct- Current Circuits

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

Lecture Outline Chapter 21. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

Parallel Resistors (32.6)

Parallel Resistors (32.6)

Chapter 19. Electric Current, Resistance, and DC Circuit Analysis

Tactics Box 23.1 Using Kirchhoff's Loop Law

Chapter 26 Direct-Current Circuits

ConcepTest PowerPoints

Chapter 21 Electric Current and Direct- Current Circuits

Circuits. 1. The Schematic

ConcepTest Clicker Questions. Chapter 26 Physics: for Scientists & Engineers with Modern Physics, 4th edition Giancoli

Circuits. PHY2054: Chapter 18 1

Chapter 26 Examples : DC Circuits Key concepts:

Chapter 19 Lecture Notes

Physics 115. General Physics II. Session 24 Circuits Series and parallel R Meters Kirchoff s Rules

Electric Charge. Electric Charge ( q ) unbalanced charges positive and negative charges. n Units Coulombs (C)

Direct Current Circuits. February 18, 2014 Physics for Scientists & Engineers 2, Chapter 26 1

Current. I = ei e = en e Av d. The current, which is Coulomb s per second, is simply

Power lines. Why do birds sitting on a high-voltage power line survive?

Electrodynamics. Review 8

Chapter 17. Current and Resistance. Sections: 1, 3, 4, 6, 7, 9

Chapter 26 Direct-Current Circuits

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

PHY232 Spring 2008 Jon Pumplin (Original ppt courtesy of Remco Zegers) Direct current Circuits

Chapter 7 Direct-Current Circuits

Class 8. Resistivity and Resistance Circuits. Physics 106. Winter Press CTRL-L to view as a slide show. Class 8. Physics 106.

ConcepTest PowerPoints

PH 222-2C Fall Circuits. Lectures Chapter 27 (Halliday/Resnick/Walker, Fundamentals of Physics 8 th edition)

Electric Current. Chapter 17. Electric Current, cont QUICK QUIZ Current and Resistance. Sections: 1, 3, 4, 6, 7, 9

Chapter 28. Direct Current Circuits

Physics 1214 Chapter 19: Current, Resistance, and Direct-Current Circuits

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

1) Two lightbulbs, one rated 30 W at 120 V and another rated 40 W at 120 V, are arranged in two different circuits.

M. C. Escher: Waterfall. 18/9/2015 [tsl425 1/29]

Chapter 16. Current and Drift Speed. Electric Current, cont. Current and Drift Speed, cont. Current and Drift Speed, final

SIMPLE D.C. CIRCUITS AND MEASUREMENTS Background

Chapter 20 Electric Circuits

Electric Currents. Resistors (Chapters 27-28)

Chapter 27. Circuits

Closed loop of moving charges (electrons move - flow of negative charges; positive ions move - flow of positive charges. Nucleus not moving)

Physics Tutorial - Currents and Circuits

Electric Charge and Electric field

physics for you February 11 Page 68

Name: Class: Date: 1. Friction can result in the transfer of protons from one object to another as the objects rub against each other.

RC Circuits. Lecture 13. Chapter 31. Physics II. Course website:

AC vs. DC Circuits. Constant voltage circuits. The voltage from an outlet is alternating voltage

ELECTRIC CURRENTS D R M A R T A S T A S I A K D E P A R T M E N T O F C Y T O B I O L O G Y A N D P R O T E O M I C S

Use these circuit diagrams to answer question 1. A B C

Physics 7B-1 (A/B) Professor Cebra. Winter 2010 Lecture 2. Simple Circuits. Slide 1 of 20

Chapter 25 Electric Currents and Resistance. Copyright 2009 Pearson Education, Inc.

Current and Resistance

PHYSICS. Chapter 30 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT

ELECTRICITY & CIRCUITS

Power in Resistive Electric Circuits

PEP 2017 Assignment 12

Electromotive Force. The electromotive force (emf), ε, of a battery is the maximum possible voltage that the battery can provide between its terminals

Chapter 28 Solutions

52 VOLTAGE, CURRENT, RESISTANCE, AND POWER

ΔV of battery. = ε - Ir or εmf = I(R+r) (for this particular series circuit) March 04, Emf and internal resistance. Emf and internal resistance

Chapter 3: Electric Current And Direct-Current Circuits

Lecture 12 Chapter 28 RC Circuits Course website:

ELECTRICITY. Prepared by: M. S. KumarSwamy, TGT(Maths) Page

Chapter 18. Direct Current Circuits

PHYS 1444 Section 02 Review #2

Physics 2401 Summer 2, 2008 Exam II

Physics for Scientists & Engineers 2

Chapter 28. Direct Current Circuits

Chapter 6 DIRECT CURRENT CIRCUITS. Recommended Problems: 6,9,11,13,14,15,16,19,20,21,24,25,26,28,29,30,31,33,37,68,71.

1. A1, B3 2. A1, B2 3. A3, B2 4. A2, B2 5. A3, B3 6. A1, B1 7. A2, B1 8. A2, B3 9. A3, B1

Chapter 17 Electric Current and Resistance Pearson Education, Inc.c

Electricity & Magnetism

ELECTRIC CURRENT. Ions CHAPTER Electrons. ELECTRIC CURRENT and DIRECT-CURRENT CIRCUITS

5. In parallel V 1 = V 2. Q 1 = C 1 V 1 and Q 2 = C 2 V 2 so Q 1 /Q 2 = C 1 /C 2 = 1.5 D

ENERGY AND TIME CONSTANTS IN RC CIRCUITS By: Iwana Loveu Student No Lab Section: 0003 Date: February 8, 2004

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

week 6 chapter 31 Current and Resistance

Topic 5.2 Heating Effect of Electric Currents

Capacitance, Resistance, DC Circuits

A Review of Circuitry

AP Physics C. Electric Circuits III.C

Chapter 2. Engr228 Circuit Analysis. Dr Curtis Nelson

AP Physics C - E & M

Copyright 2008 Pearson Education, Inc., publishing as Pearson Addison-Wesley.

1. How does a light bulb work?

Capacitance. A different kind of capacitor: Work must be done to charge a capacitor. Capacitors in circuits. Capacitor connected to a battery

Electric Current & DC Circuits

Electric charge is conserved the arithmetic sum of the total charge cannot change in any interaction.

Physics 212. Lecture 11. RC Circuits. Change in schedule Exam 2 will be on Thursday, July 12 from 8 9:30 AM. Physics 212 Lecture 11, Slide 1

1 of 23. Boardworks Ltd Electrical Power

Physics 142 Steady Currents Page 1. Steady Currents

2/25/2014. Circuits. Properties of a Current. Conservation of Current. Definition of a Current A. I A > I B > I C B. I B > I A C. I C D. I A E.

Resistivity and Temperature Coefficients (at 20 C)

To receive full credit, you must show all your work (including steps taken, calculations, and formulas used).

MasteringPhysics: Assignment Print View. Problem 30.50

Lecture 11. Power in Electric Circuits, Kirchhoff s Rules

Exam 3--PHYS 102--S14

Introduction. Pre-lab questions: Physics 1BL KIRCHOFF S RULES Winter 2010

Transcription:

Chapter 31 Lecture physics FOR SCIENTISTS AND ENGINEERS a strategic approach THIRD EDITION randall d. knight Chapter 31 Fundamentals of Circuits Chapter Goal: To understand the fundamental physical principles that govern electric circuits. Slide 31-2 Chapter 31 Preview Slide 31-3 1

Chapter 31 Preview Slide 31-4 Chapter 31 Preview Slide 31-5 Chapter 31 Preview Slide 31-6 2

Chapter 31 Preview Slide 31-7 Chapter 31 Preview Slide 31-8 Chapter 31 Reading Quiz Slide 31-9 3

Reading Question 31.1 How many laws are named after Kirchhoff? A. 0. B. 1. C. 2. D. 3. E. 4. Slide 31-10 Reading Question 31.1 How many laws are named after Kirchhoff? A. 0. B. 1. C. 2. D. 3. E. 4. Slide 31-11 Reading Question 31.2 What property of a real battery makes its potential difference slightly different than that of an ideal battery? A. Short circuit. B. Chemical potential. C. Internal resistance. D. Effective capacitance. E. Inductive constant. Slide 31-12 4

Reading Question 31.2 What property of a real battery makes its potential difference slightly different than that of an ideal battery? A. Short circuit. B. Chemical potential. C. Internal resistance. D. Effective capacitance. E. Inductive constant. Slide 31-13 Reading Question 31.3 In an RC circuit, what is the name of the quantity represented by the symbol τ? A. Period. B. Torque. C. Terminal voltage. D. Time constant. E. Coefficient of thermal expansion. Slide 31-14 Reading Question 31.3 In an RC circuit, what is the name of the quantity represented by the symbol τ? A. Period. B. Torque. C. Terminal voltage. D. Time constant. E. Coefficient of thermal expansion. Slide 31-15 5

Reading Question 31.4 Which of the following are ohmic materials: A. Batteries. B. Wires. C. Resistors. D. Materials a and b. E. Materials b and c. Slide 31-16 Reading Question 31.4 Which of the following are ohmic materials: A. Batteries. B. Wires. C. Resistors. D. Materials a and b. E. Materials b and c. Slide 31-17 Reading Question 31.5 The equivalent resistance for a group of parallel resistors is A. Less than any resistor in the group. B. Equal to the smallest resistance in the group. C. Equal to the average resistance of the group. D. Equal to the largest resistance in the group. E. Larger than any resistor in the group. Slide 31-18 6

Reading Question 31.5 The equivalent resistance for a group of parallel resistors is A. Less than any resistor in the group. B. Equal to the smallest resistance in the group. C. Equal to the average resistance of the group. D. Equal to the largest resistance in the group. E. Larger than any resistor in the group. Slide 31-19 Chapter 31 Content, Examples, and QuickCheck Questions Slide 31-20 Circuit Diagrams The top figure shows a literal picture of a resistor and a capacitor connected by wires to a battery. The bottom figure is a circuit diagram of the same circuit. A circuit diagram is a logical picture of what is connected to what. Slide 31-21 7

Circuit Elements Slide 31-22 Circuit Diagrams A circuit diagram replaces pictures of the circuit elements with symbols. The longer line at one end of the battery symbol represents the positive terminal of the battery. The battery s emf is shown beside the battery. + and symbols, even though somewhat redundant, are shown beside the terminals. Slide 31-23 QuickCheck 31.1 Does the bulb light? A. Yes. B. No. C. I m not sure. Slide 31-24 8

QuickCheck 31.1 Does the bulb light? A. Yes. B. No. Not a complete circuit C. I m not sure. Slide 31-25 QuickCheck 31.2 The three bulbs are identical and the two batteries are identical. Compare the brightnesses of the bulbs. A. A > B > C. B. A > C > B. C. A > B = C. D. A < B = C. E. A = B = C. Slide 31-26 QuickCheck 31.2 The three bulbs are identical and the two batteries are identical. Compare the brightnesses of the bulbs. A. A > B > C. B. A > C > B. C. A > B = C. D. A < B = C. E. A = B = C. This question is checking your initial intuition. We ll return to it later. Slide 31-27 9

QuickCheck 31.3 The three bulbs are identical and the two batteries are identical. Compare the brightnesses of the bulbs. A. A > B > C. B. A > C > B. C. A > B = C. D. A < B = C. E. A = B = C. Slide 31-28 QuickCheck 31.3 The three bulbs are identical and the two batteries are identical. Compare the brightnesses of the bulbs. A. A > B > C. B. A > C > B. C. A > B = C. D. A < B = C. E. A = B = C. This question is checking your initial intuition. We ll return to it later. Slide 31-29 Kirchhoff s Junction Law For a junction, the law of conservation of current requires that: where the Σ symbol means summation. This basic conservation statement is called Kirchhoff s junction law. Slide 31-30 10

Kirchhoff s Loop Law For any path that starts and ends at the same point: The sum of all the potential differences encountered while moving around a loop or closed path is zero. This statement is known as Kirchhoff s loop law. Slide 31-31 Tactics: Using Kirchhoff s Loop Law Slide 31-32 Tactics: Using Kirchhoff s Loop Law Slide 31-33 11

QuickCheck 31.4 The current through the 3 Ω resistor is A. 9 A. B. 6 A. C. 5 A. D. 3 A. E. 1 A. Slide 31-34 QuickCheck 31.4 The current through the 3 Ω resistor is A. 9 A. B. 6 A. C. 5 A. D. 3 A. E. 1 A. Slide 31-35 The Basic Circuit The most basic electric circuit is a single resistor connected to the two terminals of a battery. Figure (a) shows a literal picture of the circuit elements and the connecting wires. Figure (b) is the circuit diagram. This is a complete circuit, forming a continuous path between the battery terminals. Slide 31-36 12

Analyzing the Basic Circuit Slide 31-37 Lightbulb Puzzle #1 The figure shows two identical lightbulbs in a circuit. The current through both bulbs is exactly the same! It s not the current that the bulbs use up, it s energy. The battery creates a potential difference, which supplies potential energy to the charges. As the charges move through the lightbulbs, they lose some of their potential energy, transferring the energy to the bulbs. Slide 31-38 QuickCheck 31.5 The potential difference across the 10 resistor is A. 30 V. B. 20 V. C. 15 V. D. 10 V. E. 5 V. Slide 31-39 13

QuickCheck 31.5 The potential difference across the 10 resistor is A. 30 V. B. 20 V. C. 15 V. D. 10 V. E. 5 V. Slide 31-40 QuickCheck 31.6 What things about the resistors in this circuit are the same for all three? A. Current I. B. Potential difference V. C. Resistance R. D. A and B. E. B and C. Slide 31-41 QuickCheck 31.6 What things about the resistors in this circuit are the same for all three? A. Current I. B. Potential difference V. C. Resistance R. D. A and B. E. B and C. Slide 31-42 14

Energy and Power The power supplied by a battery is: The units of power are J/s or W. The power dissipated by a resistor is: Or, in terms of the potential drop across the resistor: Slide 31-43 Example 31.2 Delivering Power Slide 31-44 Power Dissipation in a Resistor A current-carrying resistor dissipates power because the electric force does work on the charges. Slide 31-45 15

QuickCheck 31.7 Which resistor dissipates more power? A. The 9 Ω resistor. B. The 1 Ω resistor. C. They dissipate the same power. Slide 31-46 QuickCheck 31.7 Which resistor dissipates more power? A. The 9 Ω resistor. B. The 1 Ω resistor. C. They dissipate the same power. Slide 31-47 QuickCheck 31.8 Which has a larger resistance, a 60 W lightbulb or a 100 W lightbulb? A. The 60 W bulb. B. The 100 W bulb. C. Their resistances are the same. D. There s not enough information to tell. Slide 31-48 16

QuickCheck 31.8 Which has a larger resistance, a 60 W lightbulb or a 100 W lightbulb? A. The 60 W bulb. B. The 100 W bulb. C. Their resistances are the same. D. There s not enough information to tell. Slide 31-49 Example 31.3 The Power of Light Slide 31-50 Example 31.3 The Power of Light Slide 31-51 17

QuickCheck 31.9 Which bulb is brighter? A. The 60 W bulb. B. The 100 W bulb. C. Their brightnesses are the same. D. There s not enough information to tell. Slide 31-52 QuickCheck 31.9 Which bulb is brighter? A. The 60 W bulb. B. The 100 W bulb. C. Their brightnesses are the same. D. There s not enough information to tell. P = I 2 R and both have the same current. Slide 31-53 Example 31.4 The Power of Sound Slide 31-54 18

Kilowatt Hours The product of watts and seconds is joules, the SI unit of energy. However, most electric companies prefers to use the kilowatt hour, to measure the energy you use each month. Examples: A 4000 W electric water heater uses 40 kwh of energy in 10 hours. A 1500 W hair dryer uses 0.25 kwh of energy in 10 minutes. The average cost of electricity in the United States is 10 per kwh ($0.10/kWh). Slide 31-55 Lightbulb Puzzle #2 The figure shows three identical lightbulbs in two different circuits. The voltage drop across A is the same as the total voltage drop across both B and C. More current will pass through Bulb A, and it will be brighter than either B or C. Slide 31-56 Series Resistors The figure below shows two resisters connected in series between points a and b. The total potential difference between points a and b is the sum of the individual potential differences across R 1 and R 2 : Slide 31-57 19

Series Resistors Suppose we replace R 1 and R 2 with a single resistor with the same current I and the same potential difference V ab. Ohm s law gives resistance between points a and b: Slide 31-58 Series Resistors Resistors that are aligned end to end, with no junctions between them, are called series resistors or, sometimes, resistors in series. The current I is the same through all resistors placed in series. If we have N resistors in series, their equivalent resistance is: The behavior of the circuit will be unchanged if the N series resistors are replaced by the single resistor R eq. Slide 31-59 QuickCheck 31.10 The battery current I is A. 3 A. B. 2 A. C. 1 A. D. 2/3 A. E. 1/2 A. Slide 31-60 20

QuickCheck 31.10 The battery current I is A. 3 A. B. 2 A. C. 1 A. D. 2/3 A. E. 1/2 A. Slide 31-61 Example 31.5 A Series Resistor Circuit Slide 31-62 Example 31.5 A Series Resistor Circuit Slide 31-63 21

Example 31.5 A Series Resistor Circuit Slide 31-64 Example 31.5 A Series Resistor Circuit Slide 31-65 Ammeters Figure (a) shows a simple one-resistor circuit. We can measure the current by breaking the connection and inserting an ammeter in series. The resistance of the ammeter is negligible. The potential difference across the resistor must be V R = IR = 3.0 V. So the battery s emf must be 3.0 V. Slide 31-66 22

Real Batteries Real batteries have what is called an internal resistance, which is symbolized by r. Slide 31-67 Real Batteries A single resistor connected to a real battery is in series with the battery s internal resistance, giving R eq = R + r. Slide 31-68 Example 31.6 Lighting Up a Flashlight Slide 31-69 23

Example 31.6 Lighting Up a Flashlight Slide 31-70 A Short Circuit The figure shows an ideal wire shorting out a battery. If the battery were ideal, shorting it with an ideal wire (R = 0 Ω) would cause the current to be infinite! In reality, the battery s internal resistance r becomes the only resistance in the circuit. The short-circuit current is: Slide 31-71 Example 31.7 A Short-Circuited Battery Slide 31-72 24

Lightbulb Puzzle #3 The figure shows three identical lightbulbs in a circuit. When the switch is closed, an alternate pathway for the current to get from bulb A back to the battery is created. This decreases the overall resistance of the circuit, and the brightess of bulb A increases. Slide 31-73 Parallel Resistors The figure below shows two resisters connected in parallel between points c and d. By Kirchhoff s junction law, the input current is the sum of the current through each resistor: I = I 1 + I 2. Slide 31-74 Series Resistors Suppose we replace R 1 and R 2 with a single resistor with the same current I and the same potential difference V cd. Ohm s law gives resistance between points c and d: Slide 31-75 25

Parallel Resistors Resistors connected at both ends are called parallel resistors or, sometimes, resistors in parallel. The left ends of all the resistors connected in parallel are held at the same potential V 1, and the right ends are all held at the same potential V 2. The potential differences V are the same across all resistors placed in parallel. If we have N resistors in parallel, their equivalent resistance is: The behavior of the circuit will be unchanged if the N parallel resistors are replaced by the single resistor R eq. Slide 31-76 QuickCheck 31.11 The battery current I is A. 3 A. B. 2 A. C. 1 A. D. 2/3 A. E. 1/2 A. Slide 31-77 QuickCheck 31.11 The battery current I is A. 3 A. B. 2 A. C. 1 A. D. 2/3 A. E. 1/2 A. Slide 31-78 26

Example 31.8 A Parallel Resistor Circuit Slide 31-79 Example 31.8 A Parallel Resistor Circuit Slide 31-80 Example 31.8 A Parallel Resistor Circuit Slide 31-81 27

QuickCheck 31.12 When the switch closes, the battery current A. Increases. B. Stays the same. C. Decreases. Slide 31-82 QuickCheck 31.12 When the switch closes, the battery current A. Increases. B. Stays the same. C. Decreases. Equivalent resistance decreases. Potential difference is unchanged. Slide 31-83 QuickCheck 31.13 The three bulbs are identical and the two batteries are identical. Compare the brightnesses of the bulbs. A. A > B > C. B. A > C > B. C. A > B = C. D. A < B = C. E. A = B = C. Slide 31-84 28

QuickCheck 31.13 The three bulbs are identical and the two batteries are identical. Compare the brightnesses of the bulbs. A. A > B > C. B. A > C > B. C. A > B = C. D. A < B = C. E. A = B = C. Slide 31-85 QuickCheck 31.14 The three bulbs are identical and the two batteries are identical. Compare the brightnesses of the bulbs. A. A > B > C. B. A > C > B. C. A > B = C. D. A < B = C. E. A = B = C. Slide 31-86 QuickCheck 31.14 The three bulbs are identical and the two batteries are identical. Compare the brightnesses of the bulbs. A. A > B > C. B. A > C > B. C. A > B = C. D. A < B = C. E. A = B = C. Slide 31-87 29

QuickCheck 31.15 The lightbulbs are identical. Initially both bulbs are glowing. What happens when the switch is closed? A. Nothing. B. A stays the same; B gets dimmer. C. A gets brighter; B stays the same. D. Both get dimmer. E. A gets brighter; B goes out. Slide 31-88 QuickCheck 31.15 The lightbulbs are identical. Initially both bulbs are glowing. What happens when the switch is closed? A. Nothing. B. A stays the same; B gets dimmer. C. A gets brighter; B stays the same. D. Both get dimmer. E. A gets brighter; B goes out. Short circuit. Zero resistance path. Slide 31-89 Voltmeters Figure (a) shows a simple circuit with a resistor and a real battery. We can measure the potential difference across the resistor by connecting a voltmeter in parallel across the resistor. The resistance of the voltmeter must be very high. The internal resistance is: Slide 31-90 30

QuickCheck 31.16 What does the voltmeter read? A. 6 V. B. 3 V. C. 2 V. D. Some other value. E. Nothing because this will fry the meter. Slide 31-91 QuickCheck 31.16 What does the voltmeter read? A. 6 V. B. 3 V. C. 2 V. D. Some other value. E. Nothing because this will fry the meter. Slide 31-92 QuickCheck 31.17 What does the ammeter read? A. 6 A. B. 3 A. C. 2 A. D. Some other value. E. Nothing because this will fry the meter. Slide 31-93 31

QuickCheck 31.17 What does the ammeter read? A. 6 A. B. 3 A. C. 2 A. D. Some other value. E. Nothing because this will fry the meter. Slide 31-94 Problem-Solving Strategy: Resistor Circuits Slide 31-95 Problem-Solving Strategy: Resistor Circuits Slide 31-96 32

Getting Grounded The earth itself is a conductor. If we connect one point of a circuit to the earth by an ideal wire, we can agree to call potential of this point to be that of the earth: V earth = 0 V. The wire connecting the circuit to the earth is not part of a complete circuit, so there is no current in this wire! A circuit connected to the earth in this way is said to be grounded, and the wire is called the ground wire. The circular prong of a three-prong plug is a connection to ground. Slide 31-97 A Circuit That Is Grounded The figure shows a circuit with a 10 V battery and two resistors in series. The symbol beneath the circuit is the ground symbol. The potential at the ground is V = 0. Grounding the circuit allows us to have specific values for potential at each point in the circuit, rather than just potential differences. Slide 31-98 Example 31.12 A Grounded Circuit Slide 31-99 33

Example 31.12 A Grounded Circuit Slide 31-100 Example 31.12 A Grounded Circuit Slide 31-101 Example 31.12 A Grounded Circuit Slide 31-102 34

Example 31.12 A Grounded Circuit Slide 31-103 RC Circuits The figure shows a charged capacitor, a switch, and a resistor. At t = 0, the switch closes and the capacitor begins to discharge through the resistor. A circuit such as this, with resistors and capacitors, is called an RC circuit. We wish to determine how the current through the resistor will vary as a function of time after the switch is closed. Slide 31-104 RC Circuits The figure shows an RC circuit, some time after the switch was closed. Kirchhoff s loop law applied to this circuit clockwise is: Q and I in this equation are the instantaneous values of the capacitor charge and the resistor current. The resistor current is the rate at which charge is removed from the capacitor: Slide 31-105 35

RC Circuits Knowing that I = dq/dt, the loop law for a simple closed RC circuit is: Rearranging and integrating: where the time constant τ is: Slide 31-106 RC Circuits Slide 31-107 QuickCheck 31.18 Which capacitor discharges more quickly after the switch is closed? A. Capacitor A. B. Capacitor B. C. They discharge at the same rate. D. Can t say without knowing the initial amount of charge. Slide 31-108 36

QuickCheck 31.18 Which capacitor discharges more quickly after the switch is closed? Smaller time constantτ = RC A. Capacitor A. B. Capacitor B. C. They discharge at the same rate. D. Can t say without knowing the initial amount of charge. Slide 31-109 RC Circuits The charge on the capacitor of an RC circuit is: where Q 0 is the charge at t = 0, and τ = RC is the time constant. The capacitor voltage is directly proportional to the charge, so: Where V 0 is the voltage at t = 0. The current also can be found to decay exponentially: Slide 31-110 RC Circuits Slide 31-111 37

QuickCheck 31.19 The capacitor is initially unchanged. Immediately after the switch closes, the capacitor voltage is A. 0 V. B. Somewhere between 0 V and 6 V. C. 6 V. D. Undefined. Slide 31-112 QuickCheck 31.19 The capacitor is initially unchanged. Immediately after the switch closes, the capacitor voltage is A. 0 V. B. Somewhere between 0 V and 6 V. C. 6 V. D. Undefined. Slide 31-113 Charging a Capacitor Figure (a) shows a circuit that charges a capacitor. The capacitor charge at time t is: where τ = RC. This upside-down decay is shown in figure (b). Slide 31-114 38

QuickCheck 31.20 The red curve shows how the capacitor charges after the switch is closed at t = 0. Which curve shows the capacitor charging if the value of the resistor is reduced? Slide 31-115 QuickCheck 31.20 The red curve shows how the capacitor charges after the switch is closed at t = 0. Which curve shows the capacitor charging if the value of the resistor is reduced? Smaller time constant. Same ultimate amount of charge. Slide 31-116 Chapter 31 Summary Slides Slide 31-117 39

General Strategy Slide 31-118 General Strategy Slide 31-119 General Strategy Slide 31-120 40

Important Concepts Slide 31-121 Important Concepts Slide 31-122 Important Concepts Slide 31-123 41