Reading assignment: All students should read the Appendix about using oscilloscopes.

Size: px
Start display at page:

Download "Reading assignment: All students should read the Appendix about using oscilloscopes."

Transcription

1 10. A ircuits* Objective: To learn how to analyze current and voltage relationships in alternating current (a.c.) circuits. You will use the method of phasors, or the vector addition of rotating vectors that represent the voltages or currents. This method does not require calculus. Reading assignment: All students should read the Appendix about using oscilloscopes. The learning objectives are the following: 1. To learn how alternating currents or voltages can be represented as the y-components of rotating vectors, or phasors. 2. To understand the amplitude and phase relationships amongst the different components (resistors, capacitors, inductors) of a.c. circuits. 3. To learn effective use of a typical oscilloscope. 4. To understand the phenomenon of resonance in series RL circuits. (This material is presented in your textbook iunder alternating current circuits.) Reading assignment Before you come to the lab study the sections on alternating current, capacitor circuits, inductors and inductor circuits, Read the following sections. (Section numbers may be slightly different depending on the edition of your textbook: heck the section titles.) Knight, Jones and Field : 26.1 Alternating urrent, capacitor circuits 26.4, inductors and inductor circuits 26.5, oscillation circuits 26.6 Serway and uille (212): 21.1 Resistors in an A ircuit, 21.2: apacitors in an A ircuit, 21.3 Inductors in an A ircuit, 21.4 The RL Series ircuit, 21.5: Power in an A ircuit, 21.6 Resonance in a Series RL ircuit Serway and Jewett (252): 33.1 A Sources, 33.2 Resistors in an A ircuit, 33.3: Inductors in an A ircuit, 33.4 apacitors in an A ircuit, 33.5 The RL Series ircuit, 33.6 Power in an A ircuit, 33.7 Resonance in a Series RL ircuit Pre-lab assignment: 1. The vector shown is rotating counter-clockwise around the circle shown with an angular frequency of 2 f. At time t 0sec, the angle is. Write a formula for the x and y components of the vector (a phasor ) at general time t. The length of the vector is I o. I x = I y = * William A Schwalm

2 The idea behind a current phasor is that either I x or I y can be used to represent an alternating current as the phasor rotates, since these components vary 2. (Phys 252 only) At the right is a schematic circuit di sinusoidally. 3. Is t 2. (Phys 252 only) At the right is a schematic circuit diagram showing a resistor, capacitor, inductor and alternating voltage source. (a) Label these with R,, L and a.c. (b) At a given instant t in time, suppose is the current flowing out of the source, as shown. Let, and be the currents flowing through R, L and at this instant. Write the equations that hold between each pair currents. Explain why. (c) Suppose the capacitor starts out with zero charge. As the current flows in the direction shown, what happens to the right and to the left capacitor plate? (Two separate answers.) (d) As we have learned, the voltage drop across the coil, that is to say across the inductor L, is proportional to the rate of change of the current.. What is the relation between the current through the resistor and the voltage drop across the resistor? Give an equation. (e) The voltage across the capacitor is related to the charge Q on either of its plates by the definition of capacitance. Thus give a formula for the voltage drop across the capacitor. 10-2

3 (f) Write an equation (one equation) relating the voltage to the three voltage drops across the three other circuit components. s t of the alternating voltage source 3. (Phys 212 and 252) In the following figure you see the source current as a function of time. The other curves represent voltages across the resistor, capacitor and inductor, in some order. Based on your answers above, identify which curve represents which voltage drop. Then explain briefly each choice. (Don t just say that current leads voltage across the grob, (whatever) because you also have to explain why that is, based on how grob works.) source current time voltage A B time A = B = = 4. Below left is a current phasor, a vector rotating counter-clockwise with angular frequency such that its vertical component (y component) gives the source current. At the right are three voltage phasors marked A, B, and. These relate to voltages. Based on your responses above, identify which of the three phasors corresponds to the voltage drop across each of R, L and? (The letters A, B, are not necessarily going to correspond to the curves in the previous question.) Explain your choices. For instance, which voltage phasor should line up with the current phasor because the voltage drop is proportional to current? I o A B A? B?? Phasor for source current Phasors for voltage drops 10-3

4 Exploring equipment: Read the Appendix on the use of oscilloscopes The hold introduces extra time delay between sweeps by missing some sweeps. Pulling the hold knob you can chop the input between H1 and H2. That means the input (not triggering) is sampled by rapidly alternating back and forth between the two inputs. This is handy for very low sweep rates and is used in place of alternate sweeps in this case. Equipment: The a.c. voltage source or signal generator (a) The same current flows at each instant through each circuit element. This means the current through the capacitor I c is the same at each instant as the current I R through the resistor. (b) The sum at each instant of the voltage drops around the circuit is zero. Thus if c is the voltage drop across the capacitor, R EMF provided at the same instant by the signal generator, then at each instant in time Resistor Resisto r apacitor apacitor apacito r Inductor The photo on the left shows the signal generator attached to a resistor and capacitor. The signal generator is in the rear and there is a resistor, capacitor and an inductor (not part of the circuit) each mounted on a Plexiglas box. The wires complete the circuit, so that during half the cycle current flows out one terminal of the signal generator, through the resistor, into the capacitor (charging the capacitor) and back into the generator. Then on the other half of the cycle it flows the other way. Therefore notice from the way the circuit is set up that. - - R = 0. (Yes) But and here s the tricky part R0 0. (No! ) (c) The maximum voltages across each circuit element do not add up. This is because these maximum voltages occur at different times during the cycle. 10-4

5 The fact that the voltages across the different kinds of circuit elements do not reach maximum at the same time (i.e. they are out of phase with one another) and thus don t add up is the reason you have to use an oscilloscope rather than a volt meter and is also the reason we will analyze the circuits using phasors. Problem 1 omparing voltages across the capacitor and the resistor in a series R circuit. The ontrol Data orporation needs you to analyze a bunch of control circuits for an aircraft. In the midst of this, your supervisor is asking your group to demonstrate, using the oscilloscope, the relationship between the voltage across a capacitor and a resistor R in a particular series R circuit. You are supposed to show this to your supervisor as a display on the oscilloscope screen by having the H1 trace show the resistor voltage drop t and the H2 trace show the voltage drop is one tricky point. t across the capacitor. You will have to figure out how to do it, although there In-class response question: The group should draw on the white board a circuit diagram for a series R circuit with a signal generator. Reproduce it here also. Then, answer the following both on the board and below: (a) Between which two points would you connect the oscilloscope input leads for H1 in order to measure Indicate on the diagram. t? R R (b) Between which points would you connect the leads of H2 in order to measure t? Now here s the tricky part. (a) You want to have the top of the oscilloscope screen represent a more positive voltage. (b) You also want to measure the voltages in the same direction relative to the instantaneous current flow (that is, both clockwise or both counter clockwise in the circuit.) However: (c) You cannot ground more than one point in a circuit or you have a short circuit. The problem comes about because one side of each input channel is already grounded. Notice the actual H1 and H2 inputs are BN connectors. The outer sleeve of a BN is a metal cylinder welded to the oscilloscope frame. This side of the input usually corresponds to the common on a voltmeter and to the negative or downward direction on the screen. Thus when the other input lead (central terminal of the BN) is more positive that the sleeve, the trace on the screen goes up, and when it is more negative than the sleeve the trace goes down. Therefore you have to connect the sleeve side (grounded side) of each input to the same point in the circuit. 10-5

6 In-class group response: Go back to your circuit diagram and figure out which point you would like to connect the grounded sides of the H1 and H2 inputs (same point). Indicate this point on the diagram. Then explain why this makes H2 measure the capacitor voltage upside down! (Dang.) Thus it seems you will have to see t on the screen. This is not you t and R assignment. Explain here and on the white board. A diagram showing both the R circuit and the oscilloscope connections will be appropriate. Ok, here is a possible solution to the problem: If you look carefully on the control panel you may find a control (often a push-pull thing) that will reverse the sign of the display for H2. Thus it will flip the H2 trace on the screen vertically. This should allow you to show what your supervisor needs to see. Try to find such a control. In-class response: Draw a picture of how you expect the two traces on the oscilloscope screen to look. Indicate clearly which trace is which. In-class response: Draw a phasor diagram showing voltage drops across the resistor and across the capacitor as phasors of length R0 and 0 respectively. Draw them at a time when the current phasor points along the x axis. Measurement plan: Describe very briefly how you will set up the circuit and create the display the supervisor wants. Recall that an R circuit has a time constant, which is the product R of resistance and capacitance. Plan to observe the voltage signals in three cases, (a) when the angular frequency 2 f applied by the source is less than 1/R, (b) when it equals 1/R and (c) when it is greater than 1/R. Record your plan here. 10-6

7 Implementation: arry out your plan. Record the results as graphs of what you actually observe in each case. Include the actual numbers on the scales taking into account the time base and voltage per division. Graph at least two cycles for each. Be sure your supervisor sees the display for at least one of the three cases. Analysis: Write a summary of what you learned. In particular, describe the phase relation between the two voltage drops. In each of three experiments, did the capacitor or the resistor voltage reach a maximum first, and was this what you expected? an you say how much (what fraction of a cycle) one voltage leads the other by? Why or why not? Also, how do the voltage maxima (the amplitudes) compare in each of the three cases? an you explain this? 10-7

8 Problem 2 Now your group is asked to perform a similar study and to provide a similar demonstration for a series RL. You are to demonstrate to your supervisor using the oscilloscope how the voltages across the R, the inductor L and the capacitor vary in a series RL circuit as a function of the applied angular frequency. (Recall the pre-lab exercises.) Further, you should compare to predictions that you make using phasor pictures. Work assignment: You need first to be able to show on the screen: (a) both the resistor voltage drop (You have to rewire between a) and b)) (b) both the inductor voltage drop (Rewire again. This time it s a little different.) t in H1 and the capacitor voltage drop R L t in H1 and the capacitor voltage drop Measure the phase angle from the current to the source voltage in the cases (a) when 1/ L, (b) when.2/ L, (c) when 5./ L. t in H2. t in H2. Finally you need to produce a nice, professional-looking graph showing the ratio of the current amplitude I o divided by the source voltage amplitude o as a function of, where 2 f. That is, make a graph of I o o versus. The supervisor wants this written up, of course, so you will hand it in as part of your report, as follows. You should be aware from your reading that the length of the voltage phasors representing voltage drops across each of the circuit elements are Of course the phasor, which are rotating vectors, do not all point in the same direction. In-class response: (a) The voltage phasor for which one of the circuit elements (R, L or ) is parallel to the current phasor at every instant in time? (b) Why? (c) Also, how are the directions of the other two voltage phasors related to the direction of the current phasor? Draw a picture of the three voltage phasors in this situation, representing phasors as arrows with proper labels, at an instant when the current phasor points directly along the positive x axis. R0 0 L0 0 0 I R, I L, I

9 In-class response: The source voltage at any instant is the y component (in some textbooks, the x components are used) of the vector sum of the voltage phasors. Referring to your drawing and to the formulas for the phasor lengths, what are the components of the total voltage phasor at the instant shown in your figure? ox = oy = In-class response: Thus what is the magnitude of the source voltage phasor as a function of frequency? (This gives the amplitude of the source voltage.) In-class response: What is the phase angle between the source voltage and the source current? (Remember, the current phasor is along the x axis at the moment, so this asks the angle between the axis and the total voltage phasor. It s easy to get its tangent.) Measurement plan: Your group should agree on a measurement plan for performing the assigned work. You will turn in the graph as part of your report. Include a brief outline of the measurement plan here, devoting at least some space to each point. Be sure in particular to tell us how you will wire the circuits in each case. Implementation: arry out your plan. Record the necessary data and ancillary observations here and on additional sheets. Before leaving lab, you should also have a rough sketch of the curve representing data from your resonance experiment. Analysis: You have worked out a prediction of what to expect in each case using phasors. Thus, for each of the points above, the analysis may consist of comparing what you would expect to see (which of course you must state, basing it on the phasors) with what you actually did see. As usual, you should comment especially on things that didn t go as expected. In particular, your analysis should include some discussion of the form of the graph you have constructed, and how this relates to the phenomenon of resonance as described in the text. What is the resonance frequency? What happens to the current there? etc. 10-9

10 onclusion: Usually the last five minutes are devoted to discussing the lab activity and how the activities related to the learning objectives. Give here a brief discussion of how the objectives were addressed, noting anything of particular interest. Include the main points of the class discussion

Electrical Resonance

Electrical Resonance Electrical Resonance (R-L-C series circuit) APPARATUS 1. R-L-C Circuit board 2. Signal generator 3. Oscilloscope Tektronix TDS1002 with two sets of leads (see Introduction to the Oscilloscope ) INTRODUCTION

More information

Inductors in AC Circuits

Inductors in AC Circuits Inductors in AC Circuits Name Section Resistors, inductors, and capacitors all have the effect of modifying the size of the current in an AC circuit and the time at which the current reaches its maximum

More information

The purposes of this experiment are to test Faraday's Law qualitatively and to test Lenz's Law.

The purposes of this experiment are to test Faraday's Law qualitatively and to test Lenz's Law. 260 17-1 I. THEORY EXPERIMENT 17 QUALITATIVE STUDY OF INDUCED EMF Along the extended central axis of a bar magnet, the magnetic field vector B r, on the side nearer the North pole, points away from this

More information

RC & RL Transient Response

RC & RL Transient Response EE 2006 University of Minnesota Duluth ab 8 1. Introduction R & R Transient Response The student will analyze series R and R circuits. A step input will excite these respective circuits, producing a transient

More information

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA UNIT 5 - ELECTRICAL AND ELECTRONIC PRINCIPLES NQF LEVEL 3 OUTCOME 4 - ALTERNATING CURRENT

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA UNIT 5 - ELECTRICAL AND ELECTRONIC PRINCIPLES NQF LEVEL 3 OUTCOME 4 - ALTERNATING CURRENT EDEXCEL NATIONAL CERTIFICATE/DIPLOMA UNIT 5 - ELECTRICAL AND ELECTRONIC PRINCIPLES NQF LEVEL 3 OUTCOME 4 - ALTERNATING CURRENT 4 Understand single-phase alternating current (ac) theory Single phase AC

More information

Lab E1: Introduction to Circuits

Lab E1: Introduction to Circuits E1.1 Lab E1: Introduction to Circuits The purpose of the this lab is to introduce you to some basic instrumentation used in electrical circuits. You will learn to use a DC power supply, a digital multimeter

More information

Using an Oscilloscope

Using an Oscilloscope Using an Oscilloscope The oscilloscope is used to measure a voltage that changes in time. It has two probes, like a voltmeter. You put these probes on either side of the thing that you want to measure

More information

Lab 3 - DC Circuits and Ohm s Law

Lab 3 - DC Circuits and Ohm s Law Lab 3 DC Circuits and Ohm s Law L3-1 Name Date Partners Lab 3 - DC Circuits and Ohm s Law OBJECTIES To learn to apply the concept of potential difference (voltage) to explain the action of a battery in

More information

Magnetic Field of a Circular Coil Lab 12

Magnetic Field of a Circular Coil Lab 12 HB 11-26-07 Magnetic Field of a Circular Coil Lab 12 1 Magnetic Field of a Circular Coil Lab 12 Equipment- coil apparatus, BK Precision 2120B oscilloscope, Fluke multimeter, Wavetek FG3C function generator,

More information

Experiment #11: LRC Circuit (Power Amplifier, Voltage Sensor)

Experiment #11: LRC Circuit (Power Amplifier, Voltage Sensor) Experiment #11: LRC Circuit (Power Amplifier, Voltage Sensor) Concept: circuits Time: 30 m SW Interface: 750 Windows file: RLC.SWS EQUIPMENT NEEDED Science Workshop Interface Power Amplifier (2) Voltage

More information

RLC Series Resonance

RLC Series Resonance RLC Series Resonance 11EM Object: The purpose of this laboratory activity is to study resonance in a resistor-inductor-capacitor (RLC) circuit by examining the current through the circuit as a function

More information

ε: Voltage output of Signal Generator (also called the Source voltage or Applied

ε: Voltage output of Signal Generator (also called the Source voltage or Applied Experiment #10: LR & RC Circuits Frequency Response EQUIPMENT NEEDED Science Workshop Interface Power Amplifier (2) Voltage Sensor graph paper (optional) (3) Patch Cords Decade resistor, capacitor, and

More information

Resistance, Ohm s Law, and the Temperature of a Light Bulb Filament

Resistance, Ohm s Law, and the Temperature of a Light Bulb Filament Resistance, Ohm s Law, and the Temperature of a Light Bulb Filament Name Partner Date Introduction Carbon resistors are the kind typically used in wiring circuits. They are made from a small cylinder of

More information

EE 1202 Experiment #4 Capacitors, Inductors, and Transient Circuits

EE 1202 Experiment #4 Capacitors, Inductors, and Transient Circuits EE 1202 Experiment #4 Capacitors, Inductors, and Transient Circuits 1. Introduction and Goal: Exploring transient behavior due to inductors and capacitors in DC circuits; gaining experience with lab instruments.

More information

Basic Electrical Technology Dr. L. Umanand Department of Electrical Engineering Indian Institute of Science, Bangalore. Lecture - 33 3 phase System 4

Basic Electrical Technology Dr. L. Umanand Department of Electrical Engineering Indian Institute of Science, Bangalore. Lecture - 33 3 phase System 4 Basic Electrical Technology Dr. L. Umanand Department of Electrical Engineering Indian Institute of Science, Bangalore Lecture - 33 3 phase System 4 Hello everybody. So, in the last class we have been

More information

BASIC ELECTRONICS AC CIRCUIT ANALYSIS. December 2011

BASIC ELECTRONICS AC CIRCUIT ANALYSIS. December 2011 AM 5-202 BASIC ELECTRONICS AC CIRCUIT ANALYSIS December 2011 DISTRIBUTION RESTRICTION: Approved for Pubic Release. Distribution is unlimited. DEPARTMENT OF THE ARMY MILITARY AUXILIARY RADIO SYSTEM FORT

More information

ANALYTICAL METHODS FOR ENGINEERS

ANALYTICAL METHODS FOR ENGINEERS UNIT 1: Unit code: QCF Level: 4 Credit value: 15 ANALYTICAL METHODS FOR ENGINEERS A/601/1401 OUTCOME - TRIGONOMETRIC METHODS TUTORIAL 1 SINUSOIDAL FUNCTION Be able to analyse and model engineering situations

More information

Alternating-Current Circuits

Alternating-Current Circuits hapter 1 Alternating-urrent ircuits 1.1 A Sources... 1-1. Simple A circuits... 1-3 1..1 Purely esistive load... 1-3 1.. Purely Inductive oad... 1-5 1..3 Purely apacitive oad... 1-7 1.3 The Series ircuit...

More information

EXPERIMENT NUMBER 8 CAPACITOR CURRENT-VOLTAGE RELATIONSHIP

EXPERIMENT NUMBER 8 CAPACITOR CURRENT-VOLTAGE RELATIONSHIP 1 EXPERIMENT NUMBER 8 CAPACITOR CURRENT-VOLTAGE RELATIONSHIP Purpose: To demonstrate the relationship between the voltage and current of a capacitor. Theory: A capacitor is a linear circuit element whose

More information

Chapter 12 Driven RLC Circuits

Chapter 12 Driven RLC Circuits hapter Driven ircuits. A Sources... -. A ircuits with a Source and One ircuit Element... -3.. Purely esistive oad... -3.. Purely Inductive oad... -6..3 Purely apacitive oad... -8.3 The Series ircuit...

More information

PHASOR DIAGRAMS HANDS-ON RELAY SCHOOL WSU PULLMAN, WA. RON ALEXANDER - BPA

PHASOR DIAGRAMS HANDS-ON RELAY SCHOOL WSU PULLMAN, WA. RON ALEXANDER - BPA PHASOR DIAGRAMS HANDS-ON RELAY SCHOOL WSU PULLMAN, WA. RON ALEXANDER - BPA What are phasors??? In normal practice, the phasor represents the rms maximum value of the positive half cycle of the sinusoid

More information

Chapter 35 Alternating Current Circuits

Chapter 35 Alternating Current Circuits hapter 35 Alternating urrent ircuits ac-ircuits Phasor Diagrams Resistors, apacitors and nductors in ac-ircuits R ac-ircuits ac-ircuit power. Resonance Transformers ac ircuits Alternating currents and

More information

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

Episode 126: Capacitance and the equation C =Q/V Episode 126: Capacitance and the equation C =Q/V Having established that there is charge on each capacitor plate, the next stage is to establish the relationship between charge and potential difference

More information

Measuring Electric Phenomena: the Ammeter and Voltmeter

Measuring Electric Phenomena: the Ammeter and Voltmeter Measuring Electric Phenomena: the Ammeter and Voltmeter 1 Objectives 1. To understand the use and operation of the Ammeter and Voltmeter in a simple direct current circuit, and 2. To verify Ohm s Law for

More information

DIODE CIRCUITS LABORATORY. Fig. 8.1a Fig 8.1b

DIODE CIRCUITS LABORATORY. Fig. 8.1a Fig 8.1b DIODE CIRCUITS LABORATORY A solid state diode consists of a junction of either dissimilar semiconductors (pn junction diode) or a metal and a semiconductor (Schottky barrier diode). Regardless of the type,

More information

AC CIRCUITS - CAPACITORS AND INDUCTORS

AC CIRCUITS - CAPACITORS AND INDUCTORS EXPRIMENT#8 AC CIRCUITS - CAPACITORS AND INDUCTORS NOTE: Two weeks are allocated for this experiment. Before performing this experiment, review the Proper Oscilloscope Use section of Experiment #7. Objective

More information

Eðlisfræði 2, vor 2007

Eðlisfræði 2, vor 2007 [ Assignment View ] [ Print ] Eðlisfræði 2, vor 2007 30. Inductance Assignment is due at 2:00am on Wednesday, March 14, 2007 Credit for problems submitted late will decrease to 0% after the deadline has

More information

Measurement of Capacitance

Measurement of Capacitance Measurement of Capacitance Pre-Lab Questions Page Name: Class: Roster Number: Instructor:. A capacitor is used to store. 2. What is the SI unit for capacitance? 3. A capacitor basically consists of two

More information

Capacitors in Circuits

Capacitors in Circuits apacitors in ircuits apacitors store energy in the electric field E field created by the stored charge In circuit apacitor may be absorbing energy Thus causes circuit current to be reduced Effectively

More information

The Time Constant of an RC Circuit

The Time Constant of an RC Circuit The Time Constant of an RC Circuit 1 Objectives 1. To determine the time constant of an RC Circuit, and 2. To determine the capacitance of an unknown capacitor. 2 Introduction What the heck is a capacitor?

More information

Three phase circuits

Three phase circuits Three phase circuits THREE PHASE CIRCUITS THREE-PHASE ADVANTAGES 1. The horsepower rating of three-phase motors and the kva rating of three-phase transformers are 150% greater than single-phase motors

More information

Force on Moving Charges in a Magnetic Field

Force on Moving Charges in a Magnetic Field [ Assignment View ] [ Eðlisfræði 2, vor 2007 27. Magnetic Field and Magnetic Forces Assignment is due at 2:00am on Wednesday, February 28, 2007 Credit for problems submitted late will decrease to 0% after

More information

The DC Motor. Physics 1051 Laboratory #5 The DC Motor

The DC Motor. Physics 1051 Laboratory #5 The DC Motor The DC Motor Physics 1051 Laboratory #5 The DC Motor Contents Part I: Objective Part II: Introduction Magnetic Force Right Hand Rule Force on a Loop Magnetic Dipole Moment Torque Part II: Predictions Force

More information

Figure 1: Multiple unsynchronized snapshots of the same sinusoidal signal.

Figure 1: Multiple unsynchronized snapshots of the same sinusoidal signal. 1 Oscilloscope Guide Introduction An oscilloscope is a device used to observe and measure time-dependent electronic signals. It is essentially an enhanced voltmeter which displays a graph of potential

More information

6. Block and Tackle* Block and tackle

6. Block and Tackle* Block and tackle 6. Block and Tackle* A block and tackle is a combination of pulleys and ropes often used for lifting. Pulleys grouped together in a single frame make up what is called a pulley block. The tackle refers

More information

12. Transformers, Impedance Matching and Maximum Power Transfer

12. Transformers, Impedance Matching and Maximum Power Transfer 1 1. Transformers, Impedance Matching and Maximum Power Transfer Introduction The transformer is a device that takes AC at one voltage and transforms it into another voltage either higher or lower than

More information

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

Circuits with inductors and alternating currents. Chapter 20 #45, 46, 47, 49 Circuits with inductors and alternating currents Chapter 20 #45, 46, 47, 49 RL circuits Ch. 20 (last section) Symbol for inductor looks like a spring. An inductor is a circuit element that has a large

More information

Experiment 8: Undriven & Driven RLC Circuits

Experiment 8: Undriven & Driven RLC Circuits Experiment 8: Undriven & Driven RLC Circuits Answer these questions on a separate sheet of paper and turn them in before the lab 1. RLC Circuits Consider the circuit at left, consisting of an AC function

More information

Transistor Amplifiers

Transistor Amplifiers Physics 3330 Experiment #7 Fall 1999 Transistor Amplifiers Purpose The aim of this experiment is to develop a bipolar transistor amplifier with a voltage gain of minus 25. The amplifier must accept input

More information

MATERIALS. Multisim screen shots sent to TA.

MATERIALS. Multisim screen shots sent to TA. Page 1/8 Revision 0 9-Jun-10 OBJECTIVES Learn new Multisim components and instruments. Conduct a Multisim transient analysis. Gain proficiency in the function generator and oscilloscope. MATERIALS Multisim

More information

ELECTRIC FIELD LINES AND EQUIPOTENTIAL SURFACES

ELECTRIC FIELD LINES AND EQUIPOTENTIAL SURFACES ELECTRIC FIELD LINES AND EQUIPOTENTIAL SURFACES The purpose of this lab session is to experimentally investigate the relation between electric field lines of force and equipotential surfaces in two dimensions.

More information

Magnetic Fields and Their Effects

Magnetic Fields and Their Effects Name Date Time to Complete h m Partner Course/ Section / Grade Magnetic Fields and Their Effects This experiment is intended to give you some hands-on experience with the effects of, and in some cases

More information

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

Experiment #5, Series and Parallel Circuits, Kirchhoff s Laws Physics 182 Summer 2013 Experiment #5 1 Experiment #5, Series and Parallel Circuits, Kirchhoff s Laws 1 Purpose Our purpose is to explore and validate Kirchhoff s laws as a way to better understanding

More information

Lab #9: AC Steady State Analysis

Lab #9: AC Steady State Analysis Theory & Introduction Lab #9: AC Steady State Analysis Goals for Lab #9 The main goal for lab 9 is to make the students familar with AC steady state analysis, db scale and the NI ELVIS frequency analyzer.

More information

Lesson 3 DIRECT AND ALTERNATING CURRENTS. Task. The skills and knowledge taught in this lesson are common to all missile repairer tasks.

Lesson 3 DIRECT AND ALTERNATING CURRENTS. Task. The skills and knowledge taught in this lesson are common to all missile repairer tasks. Lesson 3 DIRECT AND ALTERNATING CURRENTS Task. The skills and knowledge taught in this lesson are common to all missile repairer tasks. Objectives. When you have completed this lesson, you should be able

More information

EXPERIMENT NUMBER 5 BASIC OSCILLOSCOPE OPERATIONS

EXPERIMENT NUMBER 5 BASIC OSCILLOSCOPE OPERATIONS 1 EXPERIMENT NUMBER 5 BASIC OSCILLOSCOPE OPERATIONS The oscilloscope is the most versatile and most important tool in this lab and is probably the best tool an electrical engineer uses. This outline guides

More information

Candidate Number. General Certificate of Education Advanced Level Examination June 2014

Candidate Number. General Certificate of Education Advanced Level Examination June 2014 entre Number andidate Number Surname Other Names andidate Signature General ertificate of Education dvanced Level Examination June 214 Physics PHY4/1 Unit 4 Fields and Further Mechanics Section Wednesday

More information

Measuring Impedance and Frequency Response of Guitar Pickups

Measuring Impedance and Frequency Response of Guitar Pickups Measuring Impedance and Frequency Response of Guitar Pickups Peter D. Hiscocks Syscomp Electronic Design Limited phiscock@ee.ryerson.ca www.syscompdesign.com April 30, 2011 Introduction The CircuitGear

More information

E. K. A. ADVANCED PHYSICS LABORATORY PHYSICS 3081, 4051 NUCLEAR MAGNETIC RESONANCE

E. K. A. ADVANCED PHYSICS LABORATORY PHYSICS 3081, 4051 NUCLEAR MAGNETIC RESONANCE E. K. A. ADVANCED PHYSICS LABORATORY PHYSICS 3081, 4051 NUCLEAR MAGNETIC RESONANCE References for Nuclear Magnetic Resonance 1. Slichter, Principles of Magnetic Resonance, Harper and Row, 1963. chapter

More information

LAB 7 MOSFET CHARACTERISTICS AND APPLICATIONS

LAB 7 MOSFET CHARACTERISTICS AND APPLICATIONS LAB 7 MOSFET CHARACTERISTICS AND APPLICATIONS Objective In this experiment you will study the i-v characteristics of an MOS transistor. You will use the MOSFET as a variable resistor and as a switch. BACKGROUND

More information

ECEN 1400, Introduction to Analog and Digital Electronics

ECEN 1400, Introduction to Analog and Digital Electronics ECEN 1400, Introduction to Analog and Digital Electronics Lab 4: Power supply 1 INTRODUCTION This lab will span two lab periods. In this lab, you will create the power supply that transforms the AC wall

More information

Frequency Response of Filters

Frequency Response of Filters School of Engineering Department of Electrical and Computer Engineering 332:224 Principles of Electrical Engineering II Laboratory Experiment 2 Frequency Response of Filters 1 Introduction Objectives To

More information

SERIES-PARALLEL DC CIRCUITS

SERIES-PARALLEL DC CIRCUITS Name: Date: Course and Section: Instructor: EXPERIMENT 1 SERIES-PARALLEL DC CIRCUITS OBJECTIVES 1. Test the theoretical analysis of series-parallel networks through direct measurements. 2. Improve skills

More information

INTERFERENCE OF SOUND WAVES

INTERFERENCE OF SOUND WAVES 1/2016 Sound 1/8 INTERFERENCE OF SOUND WAVES PURPOSE: To measure the wavelength, frequency, and propagation speed of ultrasonic sound waves and to observe interference phenomena with ultrasonic sound waves.

More information

Ampere's Law. Introduction. times the current enclosed in that loop: Ampere's Law states that the line integral of B and dl over a closed path is 0

Ampere's Law. Introduction. times the current enclosed in that loop: Ampere's Law states that the line integral of B and dl over a closed path is 0 1 Ampere's Law Purpose: To investigate Ampere's Law by measuring how magnetic field varies over a closed path; to examine how magnetic field depends upon current. Apparatus: Solenoid and path integral

More information

Lab 1: The Digital Oscilloscope

Lab 1: The Digital Oscilloscope PHYSICS 220 Physical Electronics Lab 1: The Digital Oscilloscope Object: To become familiar with the oscilloscope, a ubiquitous instrument for observing and measuring electronic signals. Apparatus: Tektronix

More information

Homework #11 203-1-1721 Physics 2 for Students of Mechanical Engineering

Homework #11 203-1-1721 Physics 2 for Students of Mechanical Engineering Homework #11 203-1-1721 Physics 2 for Students of Mechanical Engineering 2. A circular coil has a 10.3 cm radius and consists of 34 closely wound turns of wire. An externally produced magnetic field of

More information

FREQUENCY RESPONSE OF AN AUDIO AMPLIFIER

FREQUENCY RESPONSE OF AN AUDIO AMPLIFIER 2014 Amplifier - 1 FREQUENCY RESPONSE OF AN AUDIO AMPLIFIER The objectives of this experiment are: To understand the concept of HI-FI audio equipment To generate a frequency response curve for an audio

More information

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

Your Comments. This was a very confusing prelecture. Do you think you could go over thoroughly how the LC circuits work qualitatively? Your omments I am not feeling great about this mierm...some of this stuff is really confusing still and I don't know if I can shove everything into my brain in time, especially after spring break. an you

More information

= V peak 2 = 0.707V peak

= V peak 2 = 0.707V peak BASIC ELECTRONICS - RECTIFICATION AND FILTERING PURPOSE Suppose that you wanted to build a simple DC electronic power supply, which operated off of an AC input (e.g., something you might plug into a standard

More information

Basic Op Amp Circuits

Basic Op Amp Circuits Basic Op Amp ircuits Manuel Toledo INEL 5205 Instrumentation August 3, 2008 Introduction The operational amplifier (op amp or OA for short) is perhaps the most important building block for the design of

More information

Introduction to the Smith Chart for the MSA Sam Wetterlin 10/12/09 Z +

Introduction to the Smith Chart for the MSA Sam Wetterlin 10/12/09 Z + Introduction to the Smith Chart for the MSA Sam Wetterlin 10/12/09 Quick Review of Reflection Coefficient The Smith chart is a method of graphing reflection coefficients and impedance, and is often useful

More information

Scott Hughes 7 April 2005. Massachusetts Institute of Technology Department of Physics 8.022 Spring 2005. Lecture 15: Mutual and Self Inductance.

Scott Hughes 7 April 2005. Massachusetts Institute of Technology Department of Physics 8.022 Spring 2005. Lecture 15: Mutual and Self Inductance. Scott Hughes 7 April 2005 151 Using induction Massachusetts nstitute of Technology Department of Physics 8022 Spring 2005 Lecture 15: Mutual and Self nductance nduction is a fantastic way to create EMF;

More information

Slide 1 / 26. Inductance. 2011 by Bryan Pflueger

Slide 1 / 26. Inductance. 2011 by Bryan Pflueger Slide 1 / 26 Inductance 2011 by Bryan Pflueger Slide 2 / 26 Mutual Inductance If two coils of wire are placed near each other and have a current passing through them, they will each induce an emf on one

More information

9. Momentum and Collisions in One Dimension*

9. Momentum and Collisions in One Dimension* 9. Momentum and Collisions in One Dimension* The motion of objects in collision is difficult to analyze with force concepts or conservation of energy alone. When two objects collide, Newton s third law

More information

Lock - in Amplifier and Applications

Lock - in Amplifier and Applications Lock - in Amplifier and Applications What is a Lock in Amplifier? In a nut shell, what a lock-in amplifier does is measure the amplitude V o of a sinusoidal voltage, V in (t) = V o cos(ω o t) where ω o

More information

Direction of Induced Current

Direction of Induced Current Direction of Induced Current Bar magnet moves through coil Current induced in coil A S N v Reverse pole Induced current changes sign B N S v v Coil moves past fixed bar magnet Current induced in coil as

More information

RC Circuits and The Oscilloscope Physics Lab X

RC Circuits and The Oscilloscope Physics Lab X Objective RC Circuits and The Oscilloscope Physics Lab X In this series of experiments, the time constant of an RC circuit will be measured experimentally and compared with the theoretical expression for

More information

Lab 14: 3-phase alternator.

Lab 14: 3-phase alternator. Lab 14: 3-phase alternator. Objective: to obtain the no-load saturation curve of the alternator; to determine the voltage regulation characteristic of the alternator with resistive, capacitive, and inductive

More information

Electronic WorkBench tutorial

Electronic WorkBench tutorial Electronic WorkBench tutorial Introduction Electronic WorkBench (EWB) is a simulation package for electronic circuits. It allows you to design and analyze circuits without using breadboards, real components

More information

FORCE ON A CURRENT IN A MAGNETIC FIELD

FORCE ON A CURRENT IN A MAGNETIC FIELD 7/16 Force current 1/8 FORCE ON A CURRENT IN A MAGNETIC FIELD PURPOSE: To study the force exerted on an electric current by a magnetic field. BACKGROUND: When an electric charge moves with a velocity v

More information

Unit2: Resistor/Capacitor-Filters

Unit2: Resistor/Capacitor-Filters Unit2: Resistor/Capacitor-Filters Physics335 Student October 3, 27 Physics 335-Section Professor J. Hobbs Partner: Physics335 Student2 Abstract Basic RC-filters were constructed and properties such as

More information

Bipolar Transistor Amplifiers

Bipolar Transistor Amplifiers Physics 3330 Experiment #7 Fall 2005 Bipolar Transistor Amplifiers Purpose The aim of this experiment is to construct a bipolar transistor amplifier with a voltage gain of minus 25. The amplifier must

More information

Physics 121 Sample Common Exam 3 NOTE: ANSWERS ARE ON PAGE 6. Instructions: 1. In the formula F = qvxb:

Physics 121 Sample Common Exam 3 NOTE: ANSWERS ARE ON PAGE 6. Instructions: 1. In the formula F = qvxb: Physics 121 Sample Common Exam 3 NOTE: ANSWERS ARE ON PAGE 6 Signature Name (Print): 4 Digit ID: Section: Instructions: Answer all questions 24 multiple choice questions. You may need to do some calculation.

More information

Experiment 3: Magnetic Fields of a Bar Magnet and Helmholtz Coil

Experiment 3: Magnetic Fields of a Bar Magnet and Helmholtz Coil MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.02 Spring 2006 Experiment 3: Magnetic Fields of a Bar Magnet and Helmholtz Coil OBJECTIVES 1. To learn how to visualize magnetic field lines

More information

Scaling and Biasing Analog Signals

Scaling and Biasing Analog Signals Scaling and Biasing Analog Signals November 2007 Introduction Scaling and biasing the range and offset of analog signals is a useful skill for working with a variety of electronics. Not only can it interface

More information

EXPERIMENT 7 OHM S LAW, RESISTORS IN SERIES AND PARALLEL

EXPERIMENT 7 OHM S LAW, RESISTORS IN SERIES AND PARALLEL 260 7- I. THEOY EXPEIMENT 7 OHM S LAW, ESISTOS IN SEIES AND PAALLEL The purposes of this experiment are to test Ohm's Law, to study resistors in series and parallel, and to learn the correct use of ammeters

More information

Chapter 19 Operational Amplifiers

Chapter 19 Operational Amplifiers Chapter 19 Operational Amplifiers The operational amplifier, or op-amp, is a basic building block of modern electronics. Op-amps date back to the early days of vacuum tubes, but they only became common

More information

1. Oscilloscope is basically a graph-displaying device-it draws a graph of an electrical signal.

1. Oscilloscope is basically a graph-displaying device-it draws a graph of an electrical signal. CHAPTER 3: OSCILLOSCOPE AND SIGNAL GENERATOR 3.1 Introduction to oscilloscope 1. Oscilloscope is basically a graph-displaying device-it draws a graph of an electrical signal. 2. The graph show signal change

More information

INTERFERENCE OF SOUND WAVES

INTERFERENCE OF SOUND WAVES 2011 Interference - 1 INTERFERENCE OF SOUND WAVES The objectives of this experiment are: To measure the wavelength, frequency, and propagation speed of ultrasonic sound waves. To observe interference phenomena

More information

Electromagnetic Induction: Faraday's Law

Electromagnetic Induction: Faraday's Law 1 Electromagnetic Induction: Faraday's Law OBJECTIVE: To understand how changing magnetic fields can produce electric currents. To examine Lenz's Law and the derivative form of Faraday's Law. EQUIPMENT:

More information

Chapter 7 Direct-Current Circuits

Chapter 7 Direct-Current Circuits Chapter 7 Direct-Current Circuits 7. Introduction...7-7. Electromotive Force...7-3 7.3 Resistors in Series and in Parallel...7-5 7.4 Kirchhoff s Circuit Rules...7-7 7.5 Voltage-Current Measurements...7-9

More information

Prelab Exercises: Hooke's Law and the Behavior of Springs

Prelab Exercises: Hooke's Law and the Behavior of Springs 59 Prelab Exercises: Hooke's Law and the Behavior of Springs Study the description of the experiment that follows and answer the following questions.. (3 marks) Explain why a mass suspended vertically

More information

Inductors. Resources and methods for learning about these subjects (list a few here, in preparation for your research):

Inductors. Resources and methods for learning about these subjects (list a few here, in preparation for your research): Inductors This worksheet and all related files are licensed under the Creative Commons Attribution License, version 1.0. To view a copy of this license, visit http://creativecommons.org/licenses/by/1.0/,

More information

ElectroMagnetic Induction. AP Physics B

ElectroMagnetic Induction. AP Physics B ElectroMagnetic Induction AP Physics B What is E/M Induction? Electromagnetic Induction is the process of using magnetic fields to produce voltage, and in a complete circuit, a current. Michael Faraday

More information

S-Parameters and Related Quantities Sam Wetterlin 10/20/09

S-Parameters and Related Quantities Sam Wetterlin 10/20/09 S-Parameters and Related Quantities Sam Wetterlin 10/20/09 Basic Concept of S-Parameters S-Parameters are a type of network parameter, based on the concept of scattering. The more familiar network parameters

More information

Equipment: Power Supply, DAI, Transformer (8341), Variable resistance (8311), Variable inductance (8321), Variable capacitance (8331)

Equipment: Power Supply, DAI, Transformer (8341), Variable resistance (8311), Variable inductance (8321), Variable capacitance (8331) Lab 5: Single-phase transformer operations. Objective: to examine the design of single-phase transformers; to study the voltage and current ratios of transformers; to study the voltage regulation of the

More information

People s Physics Book

People s Physics Book The Big Ideas: The name electric current is given to the phenomenon that occurs when an electric field moves down a wire at close to the speed of light. Voltage is the electrical energy density (energy

More information

EET272 Worksheet Week 9

EET272 Worksheet Week 9 EET272 Worksheet Week 9 answer questions 1-5 in preparation for discussion for the quiz on Monday. Finish the rest of the questions for discussion in class on Wednesday. Question 1 Questions AC s are becoming

More information

NUCLEAR MAGNETIC RESONANCE. Advanced Laboratory, Physics 407, University of Wisconsin Madison, Wisconsin 53706

NUCLEAR MAGNETIC RESONANCE. Advanced Laboratory, Physics 407, University of Wisconsin Madison, Wisconsin 53706 (revised 4/21/03) NUCLEAR MAGNETIC RESONANCE Advanced Laboratory, Physics 407, University of Wisconsin Madison, Wisconsin 53706 Abstract This experiment studies the Nuclear Magnetic Resonance of protons

More information

Circuit symbol. Each of the cells has a potential difference of 1.5 volts. Figure 1. Use the correct answer from the box to complete the sentence.

Circuit symbol. Each of the cells has a potential difference of 1.5 volts. Figure 1. Use the correct answer from the box to complete the sentence. Q.(a) Draw one line from each circuit symbol to its correct name. Circuit symbol Name Diode Light-dependent resistor (LDR) Lamp Light-emitting diode (LED) (3) Figure shows three circuits. The resistors

More information

Power measurement in balanced 3 phase circuits and power factor improvement. 1 Power in Single Phase Circuits. Experiment no 1

Power measurement in balanced 3 phase circuits and power factor improvement. 1 Power in Single Phase Circuits. Experiment no 1 Experiment no 1 Power measurement in balanced 3 phase circuits and power factor improvement 1 Power in Single Phase Circuits Let v = m cos(ωt) = cos(ωt) is the voltage applied to a R-L circuit and i =

More information

Induced voltages and Inductance Faraday s Law

Induced voltages and Inductance Faraday s Law Induced voltages and Inductance Faraday s Law concept #1, 4, 5, 8, 13 Problem # 1, 3, 4, 5, 6, 9, 10, 13, 15, 24, 23, 25, 31, 32a, 34, 37, 41, 43, 51, 61 Last chapter we saw that a current produces a magnetic

More information

Experiment 8 : Pulse Width Modulation

Experiment 8 : Pulse Width Modulation Name/NetID: Teammate/NetID: Experiment 8 : Pulse Width Modulation Laboratory Outline In experiment 5 we learned how to control the speed of a DC motor using a variable resistor. This week, we will learn

More information

Physics 42 Lab 4 Fall 2012 Cathode Ray Tube (CRT)

Physics 42 Lab 4 Fall 2012 Cathode Ray Tube (CRT) Physics 42 Lab 4 Fall 202 Cathode Ray Tube (CRT) PRE-LAB Read the background information in the lab below and then derive this formula for the deflection. D = LPV defl 2 SV accel () Redraw the diagram

More information

13. Diode Rectifiers, Filters, and Power Supplies

13. Diode Rectifiers, Filters, and Power Supplies 1 13. Diode Rectifiers, Filters, and Power Supplies Introduction A power supply takes Alternating Current or A.C. power from your electric utility (Con Edison) and converts the A.C. electrical current

More information

RLC Resonant Circuits

RLC Resonant Circuits C esonant Circuits Andrew McHutchon April 20, 203 Capacitors and Inductors There is a lot of inconsistency when it comes to dealing with reactances of complex components. The format followed in this document

More information

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

45. The peak value of an alternating current in a 1500-W device is 5.4 A. What is the rms voltage across? PHYS Practice Problems hapters 8- hapter 8. 45. The peak value of an alternating current in a 5-W device is 5.4 A. What is the rms voltage across? The power and current can be used to find the peak voltage,

More information

Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science. 6.002 Electronic Circuits Spring 2007

Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science. 6.002 Electronic Circuits Spring 2007 Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science 6.002 Electronic Circuits Spring 2007 Lab 4: Audio Playback System Introduction In this lab, you will construct,

More information

Positive Feedback and Oscillators

Positive Feedback and Oscillators Physics 3330 Experiment #6 Fall 1999 Positive Feedback and Oscillators Purpose In this experiment we will study how spontaneous oscillations may be caused by positive feedback. You will construct an active

More information