DC Circuits: Ch 19. Resistors in Series 6/1/2016

Similar documents
Circuits. The light bulbs in the circuits below are identical. Which configuration produces more light? (a) circuit I (b) circuit II (c) both the same

Chapter 7 Direct-Current Circuits

CHAPTER 28 ELECTRIC CIRCUITS

= (0.400 A) (4.80 V) = 1.92 W = (0.400 A) (7.20 V) = 2.88 W

Exercises on Voltage, Capacitance and Circuits. A d = ( ) π(0.05)2 = F

Chapter 7. DC Circuits

Method 1: 30x Method 2: 15

People s Physics Book

Experiment #5, Series and Parallel Circuits, Kirchhoff s Laws

PHYSICS 111 LABORATORY Experiment #3 Current, Voltage and Resistance in Series and Parallel Circuits

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

Solutions to Bulb questions

Chapter 19. Electric Circuits

Chapter 13: Electric Circuits

Direct-Current Circuits

Problem Solving 8: RC and LR Circuits

AP Physics Electricity and Magnetism #4 Electrical Circuits, Kirchoff s Rules

ES250: Electrical Science. HW7: Energy Storage Elements

Series and Parallel Circuits

Resistors in Series and Parallel

Series-Parallel Circuits. Objectives

Chapter 5. Parallel Circuits ISU EE. C.Y. Lee

EE301 Lesson 14 Reading: , , and

Electrical Fundamentals Module 3: Parallel Circuits

Experiment 4: Sensor Bridge Circuits (tbc 1/11/2007, revised 2/20/2007, 2/28/2007) I. Introduction. From Voltage Dividers to Wheatstone Bridges

Last time : energy storage elements capacitor.

Lab 3 - DC Circuits and Ohm s Law

( )( 10!12 ( 0.01) 2 2 = 624 ( ) Exam 1 Solutions. Phy 2049 Fall 2011

Eðlisfræði 2, vor 2007

Physics, Chapter 27: Direct-Current Circuits

W03 Analysis of DC Circuits. Yrd. Doç. Dr. Aytaç Gören

Kirchhoff s Laws Physics Lab IX

Homework # Physics 2 for Students of Mechanical Engineering

Light Bulbs in Parallel Circuits

Experiment 8 Series-Parallel Circuits

Student Exploration: Circuits

THE BREADBOARD; DC POWER SUPPLY; RESISTANCE OF METERS; NODE VOLTAGES AND EQUIVALENT RESISTANCE; THÉVENIN EQUIVALENT CIRCUIT

Experiment: Series and Parallel Circuits

Chapter 30 Inductance

2 A bank account for electricity II: flows and taxes

Parallel and Series Resistors, Kirchoff s Law

Tutorial 12 Solutions

Series and Parallel Resistive Circuits Physics Lab VIII

Current, Resistance and Electromotive Force. Young and Freedman Chapter 25

Lab E1: Introduction to Circuits

ELECTRICAL CIRCUITS. Electrical Circuits

Series and Parallel Circuits

Induced voltages and Inductance Faraday s Law

RC Circuits and The Oscilloscope Physics Lab X

DC Circuits (Combination of resistances)

AP1 Electricity. 1. A student wearing shoes stands on a tile floor. The students shoes do not fall into the tile floor due to

Resistors in Series and Parallel

Electric Current and Cell Membranes

i( t) L i( t) 56mH 1.1A t = τ ln 1 = ln 1 ln ms

Lecture Notes: ECS 203 Basic Electrical Engineering Semester 1/2010. Dr.Prapun Suksompong 1 June 16, 2010

CLASS TEST GRADE 11. PHYSICAL SCIENCES: PHYSICS Test 3: Electricity and magnetism

Chapter 1. Fundamental Electrical Concepts

Your Comments. This was a very confusing prelecture. Do you think you could go over thoroughly how the LC circuits work qualitatively?

CURRENT ELECTRICITY INTRODUCTION TO RESISTANCE, CAPACITANCE AND INDUCTANCE

Slide 1 / 26. Inductance by Bryan Pflueger

Rectifier circuits & DC power supplies

Fig. 1 Analogue Multimeter Fig.2 Digital Multimeter

Σ I in = Σ I out E = IR 1 + IR 2 FXA 2008 KIRCHHOFF S LAWS 1. Candidates should be able to : LAW 1 (K1)

Physics 2102 Lecture 19. Physics 2102

Maximum value. resistance. 1. Connect the Current Probe to Channel 1 and the Differential Voltage Probe to Channel 2 of the interface.

First Order Circuits. EENG223 Circuit Theory I

CURRENT ELECTRICITY - I

Series and Parallel Circuits

First Year (Electrical & Electronics Engineering)

Episode 126: Capacitance and the equation C =Q/V

7. What is the current in a circuit if 15 coulombs of electric charge move past a given point in 3 seconds? (1) 5 A (3) 18 A (2) 12 A (4) 45 A

17.4 Series and Parallel Circuits

Series and Parallel Resistive Circuits

1. The diagram below represents magnetic lines of force within a region of space.

Experiment 4 ~ Resistors in Series & Parallel

Resistors in Series and Parallel Circuits

Parallel DC circuits

Objectives. Electric Current

BSNL TTA Question Paper-Instruments and Measurement Specialization 2007

STUDY MATERIAL FOR CLASS Physics- CURRENT ELECTRICITY. The flow of electric charges in a particular direction constitutes electric current.

Objectives. Capacitors 262 CHAPTER 5 ENERGY

The Time Constant of an RC Circuit

Essential Electrical Concepts

Circuits with inductors and alternating currents. Chapter 20 #45, 46, 47, 49

Programmable Single-/Dual-/Triple- Tone Gong SAE 800

General Physics (PHY 2140)

SERIES-PARALLEL DC CIRCUITS

Kirchhoff's Current Law (KCL)

Preamble. Kirchoff Voltage Law (KVL) Series Resistors. In this section of my lectures we will be. resistor arrangements; series and

Section 3. Sensor to ADC Design Example

Introduction to Electricity & Magnetism. Dr Lisa Jardine-Wright Cavendish Laboratory

CHAPTER 30: Inductance, Electromagnetic Oscillations, and AC Circuits

45. The peak value of an alternating current in a 1500-W device is 5.4 A. What is the rms voltage across?

ELECTRIC FIELD LINES AND EQUIPOTENTIAL SURFACES

Physics 133: tutorial week 4 Ohm s law, electrical power, emf and internal resistance.

Lab 2: Resistance, Current, and Voltage

Chapter 22 Further Electronics

Experiment NO.3 Series and parallel connection

Tristan s Guide to: Solving Parallel Circuits. Version: 1.0 Written in Written By: Tristan Miller Tristan@CatherineNorth.com

Transcription:

DC Circuits: Ch 19 Voltage Starts out at highest point at + end of battery Voltage drops across lightbulbs and other sources of resistance. Voltage increases again at battery. I The following circuit uses a 1.5 V battery and has a 15 W lightbulb. a. Calculate the current in the circuit b. Calculate the voltage drop across the lightbulb. c. Sketch a graph of voltage vs. path (battery, top wire, resistor, bottom wire) + - Voltage highest Voltage zero Resistors in Series Same current (I) passes through all resistors (bulbs) All bulbs are equally bright (energy loss, not current loss) Voltage drop across each resistor (V 1,V 2, V 3 ) 1

V = V 1 + V 2 + V 3 V = IR 1 + IR 2 + IR 3 V = I(R 1 + R 2 + R 3 ) R eq = R 1 + R 2 + R 3 V = IR eq Resistors in Parallel Current splits at the junction Same Voltage across all resistors I = I 1 + I 2 + I 3 I 1 = V R 1 I = V R eq Calculate the equivalent resistance of two 200W resistors placed in: a. Series b. Parallel 1 = 1 + 1 + 1 R eq R 1 R 2 R 3 2

Calculate the equivalent resistance for the circuit below. Which combination of auto headlights will produce the brightest bulbs? Assume all bulbs have a resistance of R. For the Bulbs in Series: R eq = R + R = 2R For the Bulbs in Parallel 1 = 1 + 1 R eq R R 1 = 2 R eq R R eq = R/2 The bulbs in parallel have less resistance and will be brighter What current flows through each resistor in the following circuit? (R = 100 W) 0.120 A Calculate the current through this circuit, and the voltage drop across each resistor. V ab = (0.0174A)(400W) V ab = 6.96 V V bc = (0.0174A)(290W) V bc = 5.04 V R eq = 690 W I = 0.0174 A 3

What current flows through each of the resistors in this circuit? (Both are 100 W) What current will flow through the circuit shown? (I =0.48 A, I 1 =I 2 =0.24 A) R eq = 400 W + 290 W R eq = 690 W V = IR I = V/R I = 12.0 V/690 W I = 0.017 A or 17 ma What current is flowing through just the 500 W resistor? First we find the voltage drop across the first resistor: V = IR = (0.017 A)(400 W) V = 6.8 V The voltage through the resistors in parallel will be: 12.0 V 6.8 V = 5.2 V Calculate the equivalent resistance in the following circuit. To find the current across the 500 W resistor: V = IR I = V/R I = 5.2 V/500 W = 0.010 A = 10 ma 4

Which bulb will be the brightest in this arrangement (most current)? Bulb C (current gets split running through A and B) What happens when the switch is opened? C and B will have the same brightness (I is constant in a series circuit) What resistance would be present between points A and B? (ANS: 41/15 R) EMF and Terminal Voltage Batteries - source of emf (Electromotive Force), E (battery rating) All batteries have some internal resistance r A 12-V battery has an internal resistance of 0.1 W. If 10 Amps flow from the battery, what is the terminal voltage? V ab = E Ir V ab = terminal(useful)voltage E = battery rating r = internal resistance V ab = 11 V 5

Calculate the current in the following circuit. R eq = 6 W + 2.7 W R eq = 8.7 W 1/R eq = 1/10 W + 1/8.7 W R eq = 4.8 W Everything is now in series R eq = 4.8 W + 5.0 W + 0.50 W R eq = 10.3 W V = IR I = V/R I = 9.0 V/10.3 W I = 0.87 A Now calculate the terminal(useful)voltage. V = E Ir V = 9.0 V (0.87 A)(0.50 W) V = 8.6 V Grounded Wire is run to the ground Houses have a ground wire at main circuit box Does not affect circuit behavior normally Provides path for electricity to flow in emergency 6

Kirchhoff s Rules 1. Junction Rule - The sum of the currents entering a junction must equal the sum of currents leaving 2. Loop Rule - The sum of the changes in potential around any closed path = 0 Kirchhoff Conventions The loop current is not a current. Just a direction that you follow around the loop. Kirchhoff Conventions Kirchhoff s Rule Ex 1 I 1 = I 2 + I 3 Junction Rule 7

Loop Rule Main Loop 6V (I 1 )(4W) (I 3 )(9W) = 0 Side Loop (-I 2 )(5W) + (I 3 )(9W) = 0 I 1 = I 2 + I 3 Eqn 3 6V (I 1 )(4W) (I 3 )(9W) = 0 Eqn 2 (-I 2 )(5W) + (I 3 )(9W) = 0 Eqn 3 Solve Eqn 1 (-I 2 )(5W) + (I 3 )(9W) = 0 (I 3 )(9W) = (I 2 )(5W) I 3 = 5/9 I 2 Substitution into Eqn 2 6V (I 2 + I 3 )(4W) (I 3 )(9W) = 0 6 4I 2-4I 3-9I 3 = 0 6 4I 2-13I 3 = 0 I 3 = 5/9 I 2 (from last slide) 6 4I 2-13(5/9 I 2 ) = 0 6 = 101/9 I 2 I 2 = 0.53 A I 3 = 5/9 I 2 = 0.29 A I 1 = I 2 + I 3 = 0.53 A + 0.29 A = 0.82 A Kirchhoff s Rule Ex 2 I 1 = I 2 + I 3 8

Loop Rule Main Loop 9V (I 3 )(10W) (I 1 )(5W) = 0 Side Loop (-I 2 )(5W) + (I 3 )(10W) = 0 (-I 2 )(5W) + (I 3 )(10W) = 0 (I 2 )(5W) = (I 3 )(10W) I 2 = 2I 3 I 3 = 9/25 = 0.36 A I 2 = 2I 3 = 2(0.36 A) = 0.72 A I 1 = I 2 + I 3 = 0.36A + 072 A = 1.08 A 9V (I 3 )(10W) (I 1 )(5W) = 0 9V (I 3 )(10W) (I 2 + I 3 )(5W) = 0 9 10I 3 5I 2 5I 3 = 0 9 15I 3 5I 2 = 0 9 15I 3 5(2I 3 ) = 0 9 25I 3 = 0 I 3 = 9/25 = 0.36 A Calculate all the currents in the following circuit. A = 0.417 A B = 0.26 A C = 0.156 A Calculate the currents in the following circuit. 2 Amps, 3 Amps, -1 Amps 9

Bottom Loop (clockwise) 10V (6W)I 1 (2W)I 3 = 0 Top Loop (clockwise) -14V +(6W)I 1 10 V -(4W)I 2 = 0 Work with Bottom Loop 10V (6W)I 1 (2W)I 3 = 0 I 1 + I 2 = I 3 10 6I 1 2(I 1 + I 2 ) = 0 10 6I 1 2I 1-2I 2 = 0 10-8I 1-2I 2 = 0 10 = 8I 1 + 2I 2 5 = 4I 1 + I 2 I 2 = 5-4I 1 Working with Top Loop -14V +(6W)I 1 10 V -(4W)I 2 = 0 24 = 6I 1-4I 2 12 = 3I 1-2I 2 12 = 3I 1-2(5-4I 1 ) 22 = 11I 1 I 1 = 22/11 = 2.0 Amps I 2 = 5-4I 1 I 2 = 5 4(2) = -3.0 Amps I 1 + I 2 = I 3 I 3 = -1.0 A Calculate all the currents in the following circuit. A = 1.56A B = 0.522 A C = 1.04 A Batteries in Series If + to -, voltages add (top drawing) If + to +, voltages subtract (middle drawing = 8V, used to charge the 12V battery as in a car engine) I 1 = -0.864 A I 2 = 2.6 A I 3 = 1.73 A Extra Kirchhoff Problems Batteries in Parallel Provide large current when needed (Same voltage) 10

Calculate I (0.5 Amps) a. Calculate the equivalent resistance. (2.26 W) b. Calculate the current in the upper and lower wires. (3.98 A) c. Calculate I 1, I 2, and I 3 (0.60 A, 2.25 A, 1.13 A) d. Sketch a graph showing the voltage through the circuit starting at the battery. Capacitors in Parallel I 1 = +2.00 A I 2 = +1.50 A 1 3 = 0.50 A Voltage is constant in parallel Q = CV Q = C 1 V + C 2 V Q = C eq V C eq = C 1 + C 2 + C 3 + C 1 C 2 (like using a larger plate) I 1 = +2.00 A I 2 = +1.50 A 1 3 = 0.50 A Capacitors in Series Charge is constant in series 1 = 1 + 1 + 1 C eq C 1 C 2 C 3 Eq. Capacitance Ex. 1 Determine the equivalent capacitance for the circuit below if each capacitor is 5 mf. C 1 C 3 C 1 C 2 C 3 C 2 +Q -Q +Q -Q +Q -Q 11

Parallel first: Given the following setup: C eq = C 1 + C 2 C eq = 5mF + 5mF = 10 mf Series: 1 = 1 + 1 = 3/10 C eq 10 5 Ceq = 3.33 mf a. Calculate the charge on each capacitor (52.8 mc, 28.8 mc) Given the circuit below: a. Calculate the equivalent capacitance b. Calculate the charge across each capacitor c. Calculate the voltage on each capacitor (HINT: Combine them for part a, and then split them back up for b and c) Parallel capacitors C eq = 5 mf +1 mf = 6 mf Now both are series 1/ C eq = 1/6 + 1/3 C eq = 2 mf Q = CV = (2 mf)(12 V) = 24 mc For 3 mf capacitor Q = CV V = Q/C = 24 mc/3 mf = 8 V For Combined Parallel Capacitors (same voltage) V = Q/C = 24 mc/6 mf = 4 V For 5 mf Capacitor Q = CV = (5 mf)(4 V) = 20 mc For 1 mf Capacitor Q = CV = (1 mf)(4 V) = 4 mc 12

Given the following setup: a. Calculate the equivalent capacitance. (2.0 mf) b. Calculate the total charge that leaves the battery. (8.0 mc) c. Calculate the charge and voltage on each capacitor. (Q 1 = 8.0 mc, 2.7 V: Q 2 = Q 3 = 4.0 mc, 1.3 V) Given the following setup: a. Calculate the equivalent capacitance. (0.609 mf) b. Calculate the total charge that leaves the battery. (14.6 mc) c. Calculate the charge and voltage on each capacitor. (Q 1 = 14.6 mc, 14.6 V, Q 2 = 14.6 mc, 7.30 V, Q 3 = 6.26 mc, 2.09 V, Q 4 = 8.36 mc, 2.09 V ) a. Calculate the equivalent capacitance. (18 mf) b. Calculate the total charge that leaves the battery. (162 mc) c. Calculate the charge and voltage on each capacitor. (Q 1 = 45 mc, 9 V, Q 2 = 90 mc, 9 V, Q 3 = 27 mc, 9 V) a. Equivalent capacitance. (1.58 mf) b. Calculate the total charge that leaves the battery. (14.2 mc) c. Calculate the charge and voltage on each capacitor. (Q 1 = 14.2 mc, 2.84 V, Q 2 = 14.2 mc, 1.42 V, Q 3 = 14.2 mc, 4.73 V) a. Equivalent capacitance. (7.31 mf) b. Total charge that leaves the battery. (43.8 mc) c. Calculate the charge and voltage on each capacitor. (Q 1 = 30 mc, 6 V, Q 2 = 13.8 mc, 1.38 V, Q 3 = 13.8 mc, 4.6 V) a. Equivalent capacitance. (6.41 mf) b. Calculate the total charge that leaves the battery. (22.4 mc) c. Calculate the charge and voltage on each capacitor. (Q 1 = 22.4 mc, 2 V, Q 2 = 15 mc, 1.5 V, Q 3 = 7.5 mc, 1.5 V) 13

RC Circuits Capacitors store energy (flash in a camera) Resistors control how fast that energy is released Car lights that dim after you shut them off Camera flashes Difibralator DV c + DV r = 0 Q - IR = 0 (Divide by R) C Q - I = 0 RC (I = -dq/dt) Q + dq = 0 RC dt = time constant (time to reach 63% of full voltage) = RC A versatile relationship Charging the Capacitor (for capacitor) V = V o (1-e -t/rc ) Q = Q o (1-e -t/rc ) I = I o e -t/rc Discharging the Capacitor V = V o e -t/rc Q = Q o e -t/rc I = I o e -t/rc RC Circuits: Ex 1 What is the time constant for an RC circuit of resistance 200 kw and capacitance of 3.0 mf? = (200,000 W)(3.0 X 10-6 F) = 0.60 s (lower resistance will cause the capacitor to charge more quickly) 14

RC Circuits: Ex 2 What will happen to the bulb (resistor) in the circuit below when the switch is closed (like a car door)? Answer: Bulb will glow brightly initially, then dim as capacitor nears full charge. RC Circuits: Ex 3 An uncharged RC circuit has a 12 V battery, a 5.0 mf capacitor and a 800 kw resistor. Calculate the time constant. = RC = (5.0 X 10-6 F)(800,000 W) = 4.0 s What is the maximum charge on the capacitor? Q = CV Q = (5.0 X 10-6 F)(12 V) Q = 6 X 10-5 C or 60 mc What is the voltage and charge on the capacitor after 1 time constant (when discharging)? Calculate: a. Time constant (6 ms) b. Maximum charge on the capacitor (3.6 mc) c. Maximum current (0.60 ma) d. Time to reach 99% of maximum charge (28 ms) e. Current when charge = ½ Q max (0.300 ma) f. The charge when the current is 20% of the maximum value. (2.9 mc) V = V o e -t/rc Discharging the RC Circuit 15

An RC circuit has a charged capacitor C = 35 mf and a resistance of 120W. How much time will elapse until the voltage falls to 10 percent of its original (maximum) value? V = V o e -t/rc 0.10V o =V o e -t/rc 0.10 =e -t/rc ln(0.10) = ln(e -t/rc ) -2.3 = -t/rc 2.3 = t/rc t = 2.3RC t = (2.3)(120W)(35 X 10-6 F) t = 0.0097 s or 9.7 ms If a capacitor is discharged in an RC circuit, how many time constants will it take the voltage to drop to ¼ its maximum value? A fully charged 1.02 mf capacitor is in a circuit with a 20.0 V battery and a resistor. When discharged, the current is observed to decrease to 50% of it s initial value in 40 ms. a. Calculate the charge on the capacitor at t=0 (20.4 mc) b. Calculate the resistance R (57 W) c. Calculate the charge at t = 60 ms (7.3 mc) (t = 1.39RC) The capacitor in the drawing has been fully charged. The switch is quickly moved to position b (camera flash). a. Calculate the initial charge on the capacitor. (9 mc) b. Calculate the charge on the capacitor after 5.0 ms while discharging. (5.5 mc) c. Calculate the voltage after 5.0 ms while discharging. (5.5 V) d. Calculate the current through the resistor after 5.0 ms while discharging. (0.55 A) Meters Galvanometer Can only handle a small current Full-scale Current Sensitivity (I m ) Maximum deflection Ex: Multimeter Car speedometer 16

Measuring I and V Measuring Current Anmeter is placed in series Current is constant in series Anmeter (Series) Voltmeter (parallel) Measuring Voltage Voltmeter placed in parallel Voltage constant in parallel circuits Measuring voltage drop across a resistor DC Anmeter Uses Shunt (parallel) resistor Shunt resistor has low resistance Most of current flows through shunt, only a little through Galvanometer I R R = I G r Meters: Ex 1 What size shunt resistor should be used if a galvanometer has a full-scale sensitivity of 50 ma and a resistance of r= 30 W? You want the meter to read a 1.0 A current. Voltage same through both (V=IR) I R R = I g r Since most of the current goes through the shunt I R ~ 1 A I R R = I g r (1 A)(R) = (50 X 10-6 A)(30 W) R = 1.5 X 10-3 W or 1.5 m W Meters: Ex 2 Design an anmeter that can test a 12 A vacuum cleaner if the galvanometer has an internal resistance of 50 W and a full scale deflection of 1 ma. I R R = I g r (12 A)(R) = (1 X 10-3 A)(50 W) R = 4.2 X 10-3 W or 4.2 m W 17

DC Voltmeter Resistor in series Large R for resistor (keeps current low in Galvanometer) V = I(R + r) Meters: Ex 3 What resistor should be used in a voltmeter that can read a maximum of 15 V? The galvanometer has an internal resistance of 30W and a full scale deflection of 50 ma. V = I(R + r) 15 V = (50 X 10-6 A)(R + 30W) R + 30W = 15 V 50 X 10-6 A R + 30W = 300,000 W R ~ 300,000 W Meters: Ex 4 Design a voltmeter for a 120 V appliance with and internal galvanometer resistance of 50 W and a current sensitivity of 1 ma. (ANS: R = 120,000 W) 2. Clockwise (12 V. 50 W, (10 mf and 100 W parallel)) 4. a) 0.10 A b) Graph page 32-3 6. a) 5 V, 10 V b) Graph page 32-4 8. 1.92 W, 2.9 W 10. 3.6 X 10 6 J 14. 25 W 18. 3.2 % 20. R/4 22. 12 W 24. 24 W 26. 183 W 28. 13 V, 5 V, 0 V, -2 V 30. 2 ms 32. 6.9 ms 34. 0.87 K W 36. A> D = E > B = C 38. 1.99 m 40. 4.0 W 42. 7 W 44. 10 W and 60 V 46. 9.0 V 50.1.0 A, 2.0 A, 15 V 56.a) 8 Amps (8 V ab ) b) 9 Amps (0 V ab ) 58. a) R =0.505 W b) R eq = 0.500 W 62.Resistor(W) (V) Current (A) 4 8 2 6 8 1.3 8 8 1 24(bottom) 8 0.33 24 (right) 16 0.66 18

19

I 2 = -0.33 A I 1 = 0.54 A I 3 = 0.875 A 20

21

22