Lecture 12 Chapter 28 RC Circuits Course website:

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

Chapter 28. Direct Current Circuits

ConcepTest PowerPoints

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

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

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

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

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.

Chapter 26 Direct-Current Circuits

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

Chapter 7 Direct-Current Circuits

Physics Tutorial - Currents and Circuits

Circuits Practice Websheet 18.1

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

Chapter 28. Direct Current Circuits

Chapter 26 Direct-Current Circuits

ConcepTest PowerPoints

MasteringPhysics: Assignment Print View. Problem 30.50

Lecture 11. Power in Electric Circuits, Kirchhoff s Rules

PRACTICE EXAM 1 for Midterm 2

Physics 102: Lecture 7 RC Circuits

Circuits. PHY2054: Chapter 18 1

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

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

Lecture 13 Chapter 29 Magnetism Course website:

AP Physics C. Electric Circuits III.C

RC Circuits (32.9) Neil Alberding (SFU Physics) Physics 121: Optics, Electricity & Magnetism Spring / 1

Electric Charge and Electric field

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

Circuits Gustav Robert Kirchhoff 12 March October 1887

Direct-Current Circuits. Physics 231 Lecture 6-1

POWER B. Terms: EMF, terminal voltage, internal resistance, load resistance. How to add up resistors in series and parallel: light bulb problems.

Chapter 26 Examples : DC Circuits Key concepts:

physics for you February 11 Page 68

Electrical Circuits (2)

Your Comments. THIS IS SOOOO HARD. I get the concept and mathematical expression. But I do not get links among everything.

Chapter 28: DC and RC Circuits Kirchhoff s Rules

Laboratory 7: Charging and Discharging a Capacitor Prelab


PHYSICS 171. Experiment 3. Kirchhoff's Laws. Three resistors (Nominally: 1 Kilohm, 2 Kilohm, 3 Kilohm).

PRACTICE EXAM 2 for Midterm 2

Tactics Box 23.1 Using Kirchhoff's Loop Law

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

Application of Physics II for. Final Exam

Problem Solving 8: Circuits

Outline. Week 5: Circuits. Course Notes: 3.5. Goals: Use linear algebra to determine voltage drops and branch currents.

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

Experiment 4. RC Circuits. Observe and qualitatively describe the charging and discharging (decay) of the voltage on a capacitor.

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

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

Version 001 CIRCUITS holland (1290) 1

Chapter 28 Direct Current Circuits

Review. Multiple Choice Identify the letter of the choice that best completes the statement or answers the question.

PES 1120 Spring 2014, Spendier Lecture 35/Page 1

Physics 6B Summer 2007 Final

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

= e = e 3 = = 4.98%

DC Circuits. Electromotive Force Resistor Circuits. Kirchoff s Rules. RC Circuits. Connections in parallel and series. Complex circuits made easy

Chapter 28 Solutions

PHYS 1444 Section 003 Lecture #12

Capacitance. A capacitor consists of two conductors that are close but not touching. A capacitor has the ability to store electric charge.

PHYS 1444 Section 02 Review #2

Direct-Current Circuits

Electromagnetism II. (a) enav Na enav Cl (b) enav Na + enav Cl (c) enav Na (d) enav Cl (e) zero

Exam 2: Tuesday, March 21, 5:00-6:00 PM

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

3/17/2009 PHYS202 SPRING Lecture notes Electric Circuits

A positive value is obtained, so the current is counterclockwise around the circuit.

Lecture 16 - Circuit Problems

Student ID Number. Part I. Lecture Multiple Choice (43 points total)

Chapter 19 Lecture Notes

Physics 2112 Unit 11

Inductance, RL Circuits, LC Circuits, RLC Circuits

Lecture 27: FRI 20 MAR

Chapter 21 Electric Current and Direct- Current Circuits

Electric Currents. Resistors (Chapters 27-28)

Series and Parallel. How we wire the world

PHYS 1102 EXAM - II. SECTION: (Circle one) 001 (TH 9:30 AM to 10:45AM) 002 (TH 3:30 PM to 4:45 PM) You have 1 hr 45 minutes to complete the test

2005 AP PHYSICS C: ELECTRICITY AND MAGNETISM FREE-RESPONSE QUESTIONS

Sinusoidal Response of RLC Circuits

Lecture 39. PHYC 161 Fall 2016

In this unit, we will examine the movement of electrons, which we call CURRENT ELECTRICITY.

Inductors. Hydraulic analogy Duality with capacitor Charging and discharging. Lecture 12: Inductors

Inductance, Inductors, RL Circuits & RC Circuits, LC, and RLC Circuits

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

P441 Analytical Mechanics - I. RLC Circuits. c Alex R. Dzierba. In this note we discuss electrical oscillating circuits: undamped, damped and driven.

Physics 212 Midterm 2 Form A

Chapter 20 Electric 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

a. Clockwise. b. Counterclockwise. c. Out of the board. d. Into the board. e. There will be no current induced in the wire

Parallel Circuits. Chapter

Induction and Inductance

Parallel Resistors (32.6)

Parallel Resistors (32.6)

Lab 10: DC RC circuits

First Order RC and RL Transient Circuits

Question 1. Question 2. Question 3

General Physics (PHYC 252) Exam 4

Phys 102 Lecture 9 RC circuits

Transcription:

Lecture 12 Chapter 28 RC Circuits Course website: http://faculty.uml.edu/andriy_danylov/teaching/physicsii

Today we are going to discuss: Chapter 28: Section 28.9 RC circuits

Steady current Time-varying current In the preceding sections we dealt with circuits in which the circuits elements were resistors and in which the currents did not vary with time. Here we introduce the capacitor as a circuit element, which will lead us to the study of time-varying currents.

RC circuit (Charging a Capacitor) Now, we know Kirchhoff s rules and let s apply them to study an RC circuit

The capacitor charge at time t is: Charging a Capacitor The figure shows an RC circuit, some time after the switch was closed. We need to analyze it:,,? Let s look at the circuit at some arbitrary moment of time t and apply Kirchhoff s loop rule: + + 0 0 There are two variables I(t),Q(t), which are dependent: (The resistor current is the rate at which charge is added to the capacitor) / 0 It is not hard to solve, but we just present the solution (see the solution at the end of this presentation) 0 denote RC (the time constant) and (full charge of the capacitor) 1 1

Resistor Current and Capacitor Voltage Let s calculate the resistor current: RC This current looks like The Land Run of 1893 (the Oklahoma Territory) shown in the movie Far and Away (https://www.youtube.com/watch?v=jfrvog-edfc) No current. Electrons waiting for a switch to be closed. 1 Race begins. Electrons are on the way to their lands. The first photo of a traveling electron

ConcepTest RC circuit 1 In the circuit shown, the capacitor is originally uncharged. Describe the behavior of the lightbulb from the instant switch S is closed until a long time later. A) No light. B) First, it is bright, then dim. C) First, it is dim, then bright. D) Steady bright. When the switch is first closed, the current is high and the bulb burns brightly. As the capacitor charges, The voltage across the capacitor increases causing the current to be reduced, and the bulb dims.

RC circuit (discharging) We want to analyze the RC circuit:,,? At t = 0, the switch closes and the charged capacitor begins to discharge through the resistor.

RC circuit (discharging) 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 0, The resistor current is the rate at which charge is removed from the capacitor: ln 0 denote time constant as: where Q 0 is the charge at t = 0 The charge on the capacitor of an RC circuit

RC circuit (discharging) Let s plot it:

RC circuit (discharging) Let s calculate the resistor current: I 0 is the initial current The current undergoes the same exponential decay Let s calculate the voltage of the capacitor: 2.7 0.37 / / the voltage across the capacitor Now we know everything about the circuit [Q(t), I(t), and ΔV(t)]

ConcepTest RC circuit 1 Which capacitor discharges more quickly after the switch is closed? time constant = RC = 12 µs = 15 µs So the capacitor A discharges faster than B A) Capacitor A. B) Capacitor B. C) They discharge at the same rate. D) Can t say without knowing the initial amount of charge.

ConcepTest RC circuit 3 What is the time constant for the discharge of the capacitor shown in the figure? A) 5 s B) 4 s C) 2 s D) 1 s E) The capacitor does not discharge because the resistors cancel each other += time constant by definition = R eq C How about this? = R eq C=4Ωx1F=4 seconds = R eq C eq

I used an RC circuit in my paper. My application Charging a Capacitor Discharging a Capacitor

Derivation (charging a capacitor)

Thank you See you next time

ConcepTest RC circuit 2 Figure shows the voltage as a function of time of a capacitor as it is discharged (separately) through three different resistors. Rank in order, from largest to smallest, the A) R 1 < R 2 < R 3 B) R 1 < R 3 < R 2. C) R 2 < R 3 < R 1. D) Not enough information. values of the resistances R 1, R 2, and R 3. time constant by definition = RC From the figure we can see that: <...

ConcepTest An ammeter A is connected between points a and b in the circuit below, in which the four resistors are identical. The current through the ammeter is: Wheatstone Bridge A) l B) l/2 C) l/3 D) l/4 E) zero Since all resistors are identical, the voltage drops are the same across the upper branch and the lower branch. Thus, the potentials at points a and b are also the same. Therefore, no current flows. V I