Physics 1402: Lecture 11 Today’s Agenda Announcements: –Lectures posted on: www.phys.uconn.edu/~rcote/ www.phys.uconn.edu/~rcote/ –HW assignments, solutions.

Slides:



Advertisements
Similar presentations
Circuits Electromotive Force Work, Energy and emf
Advertisements

Direct-Current Circuits
Lecture 7 Circuits Ch. 27 Cartoon -Kirchhoff's Laws Topics –Direct Current Circuits –Kirchhoff's Two Rules –Analysis of Circuits Examples –Ammeter and.
Kirchhoff's Rules Continued
Overview Discuss Test 1 Review RC Circuits
a b  R C I I R  R I I r V Lecture 10, ACT 1 Consider the circuit shown: –What is the relation between V a - V d and V a - V c ? (a) (V a -V d ) < (V.
Chapter 19 DC Circuits.
Chapter 18 Direct Current Circuits. Sources of emf The source that maintains the current in a closed circuit is called a source of emf Any devices that.
Fundamentals of Circuits: Direct Current (DC)
The Lead Acid Electric Battery + - Spongy Lead (Pb) Lead Oxide (PbO 2 ) Sulfuric Acid Solution H 2 SO 4 Sulfuric Acid Electrolyte: Oxidation at the Negative.
Chapter 19 DC Circuits. Units of Chapter 19 EMF and Terminal Voltage Resistors in Series and in Parallel Kirchhoff’s Rules EMFs in Series and in Parallel;
Physics 1402: Lecture 12 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, solutions.
1 CHAPTER-27 Circuits. 2 Ch 27-2 Pumping Charges  Charge Pump:  A emf device that maintains steady flow of charges through the resistor.  Emf device.
2/13/07184 Lecture 201 PHY 184 Spring 2007 Lecture 20 Title:
Dr. Jie ZouPHY Chapter 28 Direct Current Circuits (Cont.)
Fig 28-CO, p.858. Resistive medium Chapter 28 Direct Current Circuits 28.1 Electromotive “Force” (emf)
Copyright © 2009 Pearson Education, Inc. Lecture 7 – DC Circuits.
Lesson 6 Direct Current Circuits  Electro Motive Force  Internal Resistance  Resistors in Series and Parallel  Kirchoffs Rules.
Physics 1402: Lecture 10 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, solutions.
Lecture 2 Basic Circuit Laws
Week 04, Day 2 W10D2 DC Circuits Today’s Reading Assignment W10D2 DC Circuits & Kirchhoff’s Loop Rules Course Notes: Sections Class 09 1.
CHAPTER-2 NETWORK THEOREMS.
Chapter 28A - Direct Current Circuits
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Lecture 22: FRI 17 OCT DC circuits II Ch Physics 2113
FCI. Direct Current Circuits: 3-1 EMF 3-2 Resistance in series and parallel. 3-3 Rc circuit 3-4 Electrical instruments FCI.
Chapter 26 DC Circuits. Units of Chapter EMF and Terminal Voltage - 1, Resistors in Series and in Parallel - 3, 4, 5, 6, Kirchhoff’s.
a b  R C I I R  R I I r V Yesterday Ohm’s Law V=IR Ohm’s law isn’t a true law but a good approximation for typical electrical circuit materials Resistivity.
DC circuits, RC circuits
Circuit Basics Direct Current (DC) Circuits 1.5 V + – wire open switch closed switch 2-way switch ideal battery capacitor resistor 47  F 4.7 k  These.
Chapter 25 Electric Circuits.
P212c27: 1 Direct Current Circuits Two Basic Principles: Conservation of Charge Conservation of Energy Resistance Networks R eq I a b.
10/9/20151 General Physics (PHY 2140) Lecture 10  Electrodynamics Direct current circuits parallel and series connections Kirchhoff’s rules Chapter 18.
DC CIRCUIT PREPARED BY: Patel Nidhi Harkishnbhai Sharma Surabhi Chandra Deo BE First Semester IT ACTIVE LEARNING ASSIGNMENTS.
Chapter 19 DC Circuits. Objective of the Lecture Explain Kirchhoff’s Current and Voltage Laws. Demonstrate how these laws can be used to find currents.
Chapter 28 Direct Current Circuits. Direct Current When the current in a circuit has a constant direction, the current is called direct current Most of.
Chapter 28 Direct Current Circuits. Introduction In this chapter we will look at simple circuits powered by devices that create a constant potential difference.
Lecture 11-1 Electric Current Current = charges in motion Magnitude rate at which net positive charges move across a cross sectional surface Units: [I]
Lecture 7 Circuits Chp. 28 Cartoon -Kirchoff’s Laws Opening Demo- transmission lines Physlet Topics –Direct Current Circuits –Kirchoff’s Two Rules –Analysis.
Physics 1202: Lecture 8 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, solutions.
Fundamentals of Electric Circuits
EEE ( ) - ACTIVE LEARNING ASSIGNMENT Presented by: Divyang Vadhvana( ) Branch: Information Technology.
1 18 Overview resistor & capacitor circuits Kirchoff’s Rules voltmeters & ammeters household circuits & safety Homework: 17, 27, 31, 33, 55, 67, 71, 85.
Review Exam 4. Chapter 18 Electric Currents Resistance and Resistors The ratio of voltage to current is called the resistance: (18-2a) (18-2b)
Announcements WebAssign HW Set 5 due this Friday Problems cover material from Chapters 18 My office hours today from 2 – 3 pm or by appointment (I am away.
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
Physics 1202: Lecture 9 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, solutions.
Lecture 12: TUE 02 FEB DC circuits Ch Physics 2102 Jonathan Dowling.
Lecture 12-1 Resistors in Parallel and in Serial R1R1 R2R2 i i ε.
Chapter 27 Circuits (Basic) Electric Circuits Series Connections: Total Resistance = Sum of individual Resistances. Current the same through every load.
Chapter 19 DC Circuits. EMF and Terminal Voltage Any device that can transform a type of energy into electric energy is called a source of electromotive.
RC Circuits Physics 102 Professor Lee Carkner Lecture 16.
Direct-Current Circuits
Physics 4 – Jan 26, 2017 P3 Challenge –
Chapter 26:DC Circuits Chapter 26 Opener. These MP3 players contain circuits that are dc, at least in part. (The audio signal is ac.) The circuit diagram.
Electricity and magnetism Chapter Seven: DC Circuits
Internal Resistance in EMF
Physics 1202: Lecture 6 Today’s Agenda
General Physics (PHY 2140) Lecture 10 Electrodynamics
Circuit in DC Instruments
This Class Resistors in series: Current through is same.
Ideal vs Real Battery Ideal battery: no internal energy dissipation
WELCOME TO PHYSICS PROJECT.
Kirchoff’s Laws.
Kirchoff’s Laws.
Direct-Current Circuits
Kirchhoff’s Laws.
Kirchhoff’s Laws.
Physics 4 – Feb 8, 2018 P3 Challenge –
Direct-Current Circuits
Presentation transcript:

Physics 1402: Lecture 11 Today’s Agenda Announcements: –Lectures posted on: –HW assignments, solutions etc. Homework #4:Homework #4: –On Masterphysics : due next Friday at 8:00 AM –Go to masteringphysics.com

V R1R1 R2R2 V R1R1 R2R2 Summary Resistors in series –the current is the same in both R 1 and R 2 –the voltage drops add Resistors in parallel –the voltage drop is the same in both R 1 and R 2 –the currents add

 I1I1   R R R I2I2 I3I3

Kirchoff's First Rule "Loop Rule" or “Kirchoff’s Voltage Law (KVL)” "When any closed circuit loop is traversed, the algebraic sum of the changes in potential must equal zero." This is just a restatement of what you already know: that the potential difference is independent of path! We will follow the convention that voltage gains enter with a + sign and voltage drops enter with a - sign in this equation. RULES OF THE ROAD:  R1R1  R2R2 I Move clockwise around circuit:  R1R1 R2R2  I   IR 1  IR 2     0 0 KVL:

Kirchoff's Second Rule "Junction Rule" or “Kirchoff’s Current Law (KCL)” In deriving the formula for the equivalent resistance of 2 resistors in parallel, we applied Kirchoff's Second Rule (the junction rule). "At any junction point in a circuit where the current can divide (also called a node), the sum of the currents into the node must equal the sum of the currents out of the node." This is just a statement of the conservation of charge at any given node.

Junction Example Outside loop:Top loop:Junction:  I1I1   R R R I2I2 I3I3

Chapter 11, ACT 1 Consider the circuit shown: –What is the relation between V a -V d and V a -V c ? (a) (V a -V d ) < (V a -V c ) (b) (V a -V d ) = (V a -V c ) (c) (V a -V d ) > (V a -V c ) 2A (a) I 1 < I 2 (b) I 1 = I 2 (c) I 1 > I 2 2B – What is the relation between I 1 and I 2 ? 12 V I1I1 I2I2 a b d c 50  20  80 

Chapter 11, ACT 2 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 A) I B) I/2 C) I/4 D) I/8 E) 0

RC Circuits Consider the circuit shown: –What will happen when we close the switch ? –Add the voltage drops going around the circuit, starting at point a. IR + Q/C – V = 0 –In this case neither I nor Q are known or constant. But they are related, V a b c R C This is a simple, linear differential equation.

RC Circuits V a b c R We do a little bit of algebra and separate dq and dt. C

RC Circuits Case 1: Charging Q 1 = 0, Q 2 = Q and t 1 = 0, t 2 = t V a b c R C To get Current, I = dQ/dt Q tt I

RC Circuits c Case 2: Discharging To discharge the capacitor we have to take the battery out of the circuit a b R C To get Current, I = dQ/dt t I Q t

Chapter 11, ACT 3 c Consider the simple circuit shown here. Initially the switch is open and the capacitor is charged to a potential V O. Immediately after the switch is closed, what is the current ? a b R C A) I = V O /RB) I = 0 C) I = RCD) I = V O /R exp(-1/RC)

Chapter 11, ACT 4 Consider the circuit at right after the switch is closed i) What is the initial current I? A) 0 B) 1 A C) 2 A D) 3 A E) 4 A I 6  12  F 12 V ii) What is the current I after 2 minutes? A) 0 B) 1 A C) 2 A D) 3 A E) 4 A

If R = 3.0 kΩ, C = 6.0 nF,  1 = 10.0 V, Q = 18 nC,  2 = 6.0 V, and I = 5.0 mA, what is the potential difference V b –V a ? a. –13 V b. +28 V c. +13 V d. –28 V e. +2.0V Lecture 11, ACT 5

Electrical Instruments The Ammeter The device that measures current is called an ammeter. Ideally, an ammeter should have zero resistance so that the measured current is not altered. A  I R1R1 R2R2 + -

Electrical Instruments The Voltmeter The device that measures potential difference is called a voltmeter. An ideal voltmeter should have infinite resistance so that no current passes through it. V  R1R1 R2R2 I IvIv I2I2

Problem Solution Method: Five Steps: 1)Focus the Problem - draw a picture – what are we asking for? 2)Describe the physics -what physics ideas are applicable -what are the relevant variables known and unknown 3)Plan the solution -what are the relevant physics equations 4)Execute the plan -solve in terms of variables -solve in terms of numbers 5)Evaluate the answer -are the dimensions and units correct? -do the numbers make sense?