Coil in the AC circuit
|
|
- Dana Hancock
- 6 years ago
- Views:
Transcription
1 Coil in the AC circuit LEP Related topics Inductance, Kirchhoff s laws, parallel connection, series connection, a. c. impedance, phase displacement, vector diagram Principle The impedance and phase displacement of a coil in an A.C. circuit are observed as functions of frequency and inductance. Parallel and series circuits are studied. Material 1 Coil, 300 turns Coil, 600 turns Resistor plug-in box 50 ohm Resistor plug-in box 100 ohm Resistor plug-in box 200 ohm Connection box Difference amplifier Digital function generator Oscilloscope, 30 MHz, 2 channels Screened cable, BNC, l = 750 mm Connecting cord, l = 100 mm, red Connecting cord, l = 100 mm, blue Connecting cord, l = 500 mm, red Connecting cord, l = 500 mm, blue Fig. 1: Experimental set-up with coil and resistor in series. P PHYWE Systeme GmbH & Co. KG All rights reserved 1
2 TEP Coil in the AC circuit Tasks 1. Measure the impedance of one of the coils as a function of frequency. 2. Determine the inductance of the coils. 3. Measure the phase displacement between terminal voltage and total current as a function of the frequency in the circuit. 4. Determine the total impedance of coils connected in parallel and in series. Set-up The experimental set-up is shown in Fig. 1. Since normal voltmeters and ammeters generally measure only rms (root mean square) values and take no account of phase relationships, it is preferable to use an oscilloscope to study the dynamics of current and voltage in such circuits. The experiment will be carried out with sinusoidal voltages. The rms values are obtained when the peak-to-peak values U p p measured on the oscilloscope are divided by 2 2. In accordance with relation (1), the total current I in the circuit can be deduced by measuring the voltage U across the resistor with resistance R. Fig. 2: Circuit for simultaneous display of voltage across the coil and total current. I = U R (1) The circuit shown in Fig. 2 permits the simultaneous display of the total current and the coil voltage. The phase displacement between the terminal voltage and the total current can be measured using a similar circuit, but with channel B measuring the terminal voltage instead of the voltage across the coil (see Fig. 3). When connecting coils in parallel or series the coils need to be sufficiently far apart, since their magnetic fields influence each other. Procedure In order to achieve high reading accuracy on the oscilloscope, high gain settings should be selected. After selecting the gain setting the Y-position of the two base-lines (GND) have to be adjusted until they Fig. 3: Circuit for simultaneous display of terminal coincide. The peak-to-peak amplitude of the frequency generator s signal should not be higher than voltage and total current. 5 V and should have no offset. The digital frequency generator s antenna output has to be connected with the ground socket of the difference amplifier. For detailed descriptions of the operation of the oscilloscope and the digital function generator please refer to the manuals. 2 PHYWE Systeme GmbH & Co. KG All rights reserved P
3 Coil in the AC circuit LEP Task 1 and 2: To determine the impedance of a coil as a function of the frequency the coil is connected in series with various resistors of known value (see Fig. 2). For each resistor the frequency is varied until there is the same potential difference across the coil as across the resistor. The resistance and impedance values are then equal and equation (2) is valid. R Ω = ωl = X L (2) From this relation the inductance of a coil can be deduced, if the impedance at one frequency is known. Task 3: Set up the circuit as shown in Fig. 3 to display both terminal voltage and total current of the circuit. There are two major ways to measure the frequency-dependent phase shift between total current and terminal voltage. If, by means of the time-base control of the oscilloscope, one half-wave of the current is brought to the full screen width (10 cm) possibly with variable sweep rate the phase displacement of the voltage can be read off directly in cm (18 / cm). Another way to determine the phase shift is to read the interval between the terminal voltage and the voltage across the resistor (corresponding to the total current) directly from the oscilloscope and calculate the time gap as well as the resulting phase angle. Attention: If the second procedure is chosen, the variable sweep rate must not be used as it distorts the timeframe up to a factor of 2.5 which makes an accurate calculation of the time gap impossible. Task 4: In order to determine the total inductance of the coils in parallel and series, include the coils appropriately into the circuit and determine the frequency for R = X L = 100 Ω. The inductance can then be calculated analog to task 2. Theory If a coil of inductance L and an ohmic resistor of resistance R are connected in a circuit, the sum of the potential differences across the coil and the resistor is equal to the terminal voltage U t which gives relation (3). U t = I R + L di (3) dt This corresponds to Kirchhoff s second law, which states, that the directed sum of all electrical potential differences in a closed circuit is zero. Care must be taken regarding the direction of the potential differences. The terminal voltage has the reversed direction of the voltage across the coil and the resistor. Relation (4) gives the formula of Kirchhoff s voltage law for the studied circuits, where U Ω = I R is the voltage across the resistor and U L = L di the voltage across the coil. dt U L + U Ω U t = 0 (4) Such resistors R have been selected so that the coils d. c. resistances of 0.8 Ω (n=300) and 2.5 Ω (n=600) can be disregarded as R L (d. c. ) R. If the alternating voltage U t has the frequency ω = 2πν and the waveform U t = U 0 cos ωt, (5) inserting (5) into equation (3) gives the following solution for the current I: P PHYWE Systeme GmbH & Co. KG All rights reserved 3
4 TEP Coil in the AC circuit I = I 0 cos(ωt φ) (6) There φ is the phase angle and the phase displacement is given by tan φ = ωl R (7) with the peak current U I 0 = 0. (8) R 2 +(ωl) 2 As is seen from relation (4) the total current follows the terminal voltage. If there are more than one coil in the circuit, the total inductivity can be calculated with equations (9) for series and (10) for parallel connection, if the coils are magnetically uncoupled. L tot = L i (9) L tot = 1 L i (10) Results and Evaluation In the following the evaluation of the obtained values is described with the help of example values. Your results may vary from those presented here. Task 1: Measure the impedance of one of the coils as a function of frequency. From equation (2) the linear relation between frequency of the signal and impedance of the coil is obvious. Linear regression of the measured values (see Fig. 4) gives relation (11) with the correlation coefficient R = X L (ν) Ω = 13.8 ν 0.9 (11) khz For the coil with n=600 should also be found a linear relation. 4 PHYWE Systeme GmbH & Co. KG All rights reserved P
5 Coil in the AC circuit LEP Fig. 4: Impedance values for various frequencies. Equation (11) gives the relation of the linear fit. Task 2: Determine the inductance of the coils. Considering relations (2) and (11) for the first coil leads to equation (12) which gives the inductance of the coil with L 1 = 2.19 mh. X L = 2πν L = ν L = π = 2.19 mh (12) The analog calculation for the second coil results into L 2 = 10.4 mh. Task 3: Measure the phase displacement between the terminal voltage and total current as a function of the frequency in the circuit. As mentioned above there are two ways to determine the phase angle and the phase displacement respectively. The first way allows to read off the phase angle directly from the oscilloscope s display. Then the phase displacement can easily be calculated. According to equation (7) the phase displacement should show linear dependence with respect to the frequency as is shown in Fig. 5. The alternative method requires some calculation, as only the time shift dt is obtained. Obviously the ratio between time shift and one full period T is the same as between the phase angle and one full circle: dt T = φ 360 The period of the oscillation is nothing more than the reciprocal of the frequency. Thus the phase angle can be calculated with relation (13): P PHYWE Systeme GmbH & Co. KG All rights reserved 5
6 TEP Coil in the AC circuit Fig. 5: Frequency-dependent phase angle (blue) and phase displacement (black) between current and voltage in the circuit. φ = 360 ν dt (13) Note: Special attention should be given to the units of the various measurands. Task 4: Determine the total inductance of coils connected in parallel and in series. For series (s) and parallel (p) connection with R = 100 Ω we find the frequencies of 1.34 khz and 8.62 khz respectively. Calculation analog to equation (12) results into L s = mh and L p = 1.85 mh. One can easily verify that the found total inductances follow equations (9) and (10). 6 PHYWE Systeme GmbH & Co. KG All rights reserved P
Electricity. Coil in the AC circuit /11. Electrodynamics. What you need:
Electrodynamics Electricity Coil in the AC circuit -01/11 What you can learn about Inductance Kirchhoff s laws Maxwell s equations AC impedance Phase displacement Principle: The coil is connected in a
More informationCoil in the AC circuit with Cobra3
Coil in the AC circuit with Cobra3 TEP Related topics Inductance, Kirchhoff s laws, Maxwell s equations, a.c. impedance, phase displacement. Principle and task The coil is connected in a circuit with a
More informationLEP RLC Circuit
RLC Circuit LEP Related topics Kirchhoff s laws, series and parallel tuned circuit, resistance, capacitance, inductance, phase displacement, Q-factor, band-width, loss resistance, damping Principle The
More informationRLC-circuits TEP. f res. = 1 2 π L C.
RLC-circuits TEP Keywords Damped and forced oscillations, Kirchhoff s laws, series and parallel tuned circuit, resistance, capacitance, inductance, reactance, impedance, phase displacement, Q-factor, band-width
More informationInductance of solenoids with Cobra3
Inductance of solenoids with Cobra3 TEP Related topics Law of inductance, Lenz s law, self-inductance, solenoids, transformer, oscillatory circuit, resonance, damped oscillation, logarithmic decrement,
More informationElectromagnetic Oscillations and Currents. March 23, 2014 Chapter 30 1
Electromagnetic Oscillations and Currents March 23, 2014 Chapter 30 1 Driven LC Circuit! The voltage V can be thought of as the projection of the vertical axis of the phasor V m representing the time-varying
More informationRLC-circuits with Cobra4 Xpert-Link TEP. 1 2 π L C. f res=
Related topics Damped and forced oscillations, Kirchhoff s laws, series and parallel tuned circuit, resistance, capacitance, inductance, reactance, impedance, phase displacement, Q-factor, band-width Principle
More informationMagnetic field inside a conductor
Magnetic field inside a conductor TEP Principle A current is passed through an electrolyte producing a magnetic field. This magnetic field inside the conductor is measured as function of position and current
More informationTEP. RLC Circuit with Cobra3
RLC Circuit with Cobra3 TEP Related topics Tuned circuit, series-tuned circuit, parallel-tuned circuit, resistance, capacitance, inductance, capacitor, coil, phase displacement, Q-factor, band-width,impedance,
More informationKirchhoff s laws, induction law, Maxwell equations, current, voltage, resistance, parallel connection, series connection, potentiometer
Kirchhoff s laws with Cobra4 TEP Related Topics Kirchhoff s laws, induction law, Maxwell equations, current, voltage, resistance, parallel connection, series connection, potentiometer Principle First Kirchhoff
More informationInductance of solenoids
Inductance of solenoids LEP -01 Related topics Law of inductance, Lenz s law, self-inductance, solenoids, transformer, oscillatory circuit, resonance, damped oscillation, logarithmic decrement, Q factor.
More informationChapter 31 Alternating Current
Chapter 31 Alternating Current In this chapter we will learn how resistors, inductors, and capacitors behave in circuits with sinusoidally vary voltages and currents. We will define the relationship between
More informationAC Circuits INTRODUCTION DISCUSSION OF PRINCIPLES. Resistance in an AC Circuit
AC Circuits INTRODUCTION The study of alternating current 1 (AC) in physics is very important as it has practical applications in our daily lives. As the name implies, the current and voltage change directions
More informationChapter 6: Alternating Current. An alternating current is an current that reverses its direction at regular intervals.
Chapter 6: Alternating Current An alternating current is an current that reverses its direction at regular intervals. Overview Alternating Current Phasor Diagram Sinusoidal Waveform A.C. Through a Resistor
More informationExperiment 1 Alternating Current with Coil and Ohmic Resistors
Experiment Alternating Current with Coil and Ohmic esistors - Objects of the experiment - Determining the total impedance and the phase shift in a series connection of a coil and a resistor. - Determining
More informationGoals. Introduction. To understand the use of root mean square (rms) voltages and currents.
Lab 10. AC Circuits Goals To show that AC voltages cannot generally be added without accounting for their phase relationships. That is, one must account for how they vary in time with respect to one another.
More informationGoals. Introduction. To understand the use of root mean square (rms) voltages and currents.
Lab 10. AC Circuits Goals To show that AC voltages cannot generally be added without accounting for their phase relationships. That is, one must account for how they vary in time with respect to one another.
More informationExercise 9: inductor-resistor-capacitor (LRC) circuits
Exercise 9: inductor-resistor-capacitor (LRC) circuits Purpose: to study the relationship of the phase and resonance on capacitor and inductor reactance in a circuit driven by an AC signal. Introduction
More informationMagnetic induction with Cobra3
Principle A magnetic field of variable frequency and varying strength is produced in a long coil. The voltages induced across thin coils which are pushed into the long coil are determined as a function
More informationExperiment 9 AC Circuits
Experiment 9 AC Circuits "Look for knowledge not in books but in things themselves." W. Gilbert (1540-1603) OBJECTIVES To study some circuit elements and a simple AC circuit. THEORY All useful circuits
More informationChapter 30 Inductance, Electromagnetic. Copyright 2009 Pearson Education, Inc.
Chapter 30 Inductance, Electromagnetic Oscillations, and AC Circuits 30-7 AC Circuits with AC Source Resistors, capacitors, and inductors have different phase relationships between current and voltage
More information13 th Asian Physics Olympiad India Experimental Competition Wednesday, 2 nd May 2012
13 th Asian Physics Olympiad India Experimental Competition Wednesday, nd May 01 Please first read the following instructions carefully: 1. The time available is ½ hours for each of the two experimental
More informationReactance and Impedance
eactance and Impedance Theory esistors, 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 value (in
More informationChapter 33. Alternating Current Circuits
Chapter 33 Alternating Current Circuits Alternating Current Circuits Electrical appliances in the house use alternating current (AC) circuits. If an AC source applies an alternating voltage to a series
More informationAlternating current circuits- Series RLC circuits
FISI30 Física Universitaria II Professor J.. ersosimo hapter 8 Alternating current circuits- Series circuits 8- Introduction A loop rotated in a magnetic field produces a sinusoidal voltage and current.
More informationEE 210: CIRCUITS AND DEVICES
EE 210: CIRCUITS AND DEVICES LAB #3: VOLTAGE AND CURRENT MEASUREMENTS This lab features a tutorial on the instrumentation that you will be using throughout the semester. More specifically, you will see
More informationExercise 2: Inductors in Series and in Parallel
Exercise 2: Inductors in Series and in Parallel EXERCISE OBJECTIVE When you have completed this exercise, you will be able to determine the total inductance of a circuit containing inductors in series
More informationresistor box inductor 3 BNC to banana + V L
Physics ab II Inductance and Circuit Page 1/5 Name: Partner: Partner: Purpose: To investigate how the voltage across an inductor changes in response to changing currents. To measure the inductance by measuring
More informationBakiss Hiyana binti Abu Bakar JKE, POLISAS BHAB
1 Bakiss Hiyana binti Abu Bakar JKE, POLISAS 1. Explain AC circuit concept and their analysis using AC circuit law. 2. Apply the knowledge of AC circuit in solving problem related to AC electrical circuit.
More informationElectron Spin Resonance v2.0
Electron Spin Resonance v2.0 Background. This experiment measures the dimensionless g-factor (g s ) of an unpaired electron using the technique of Electron Spin Resonance, also known as Electron Paramagnetic
More informationPHASES IN A SERIES LRC CIRCUIT
PHASES IN A SERIES LRC CIRCUIT Introduction: In this lab, we will use a computer interface to analyze a series circuit consisting of an inductor (L), a resistor (R), a capacitor (C), and an AC power supply.
More informationAcoustic Doppler Effect
Acoustic Doppler Effect TEP Related Topics Wave propagation, Doppler shift of frequency Principle If an emitter of sound or a detector is set into motion relative to the medium of propagation, the frequency
More informationMagnetic induction with Cobra3
Magnetic induction with Cobra3 LEP Related Topics Maxwell s equations, electrical eddy field, magnetic field of coils, coil, magnetic flux, induced voltage. Principle A magnetic field of variable frequency
More informationEXPERIMENT 4: RC, RL and RD CIRCUITs
EXPERIMENT 4: RC, RL and RD CIRCUITs Equipment List An assortment of resistor, one each of (330, 1k,1.5k, 10k,100k,1000k) Function Generator Oscilloscope 0.F Ceramic Capacitor 100H Inductor LED and 1N4001
More informationEXPERIMENT 4: RC, RL and RD CIRCUITs
EXPERIMENT 4: RC, RL and RD CIRCUITs Equipment List Resistor, one each of o 330 o 1k o 1.5k o 10k o 100k o 1000k 0.F Ceramic Capacitor 4700H Inductor LED and 1N4004 Diode. Introduction We have studied
More informationEXPERIMENT 8: LRC CIRCUITS
EXPERIMENT 8: LRC CIRCUITS Equipment List S 1 BK Precision 4011 or 4011A 5 MHz Function Generator OS BK 2120B Dual Channel Oscilloscope V 1 BK 388B Multimeter L 1 Leeds & Northrup #1532 100 mh Inductor
More informationElectromagnetic Induction - A
Electromagnetic Induction - A APPARATUS 1. Two 225-turn coils 2. Table Galvanometer 3. Rheostat 4. Iron and aluminum rods 5. Large circular loop mounted on board 6. AC ammeter 7. Variac 8. Search coil
More informationCH 1. Large coil. Small coil. red. Function generator GND CH 2. black GND
Experiment 6 Electromagnetic Induction "Concepts without factual content are empty; sense data without concepts are blind... The understanding cannot see. The senses cannot think. By their union only can
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.02 Spring 2005 Experiment 10: LR and Undriven LRC Circuits
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.0 Spring 005 Experiment 10: LR and Undriven LRC Circuits OBJECTIVES 1. To determine the inductance L and internal resistance R L of a coil,
More informationElectric Transformer. Specifically, for each coil: Since the rate of change in flux through single loop of each coil are approximately the same,
Electric Transformer Safety and Equipment Computer with PASCO 850 Universal Interface and PASCO Capstone Coils Set 3 Double Banana Cables PASCO Voltage Sensor (DIN to Banana cable with slip-on Alligator
More informationωc ωc sin(wt 90o ) (for a capacitance) (4)
Physics'241'Signal'Processing:'Lab'3' Sinusoidal esponse of, L ircuits In the previous lab, we studied the behavior of series combinations of and L circuits with input square and triangular waveforms.
More informationRLC-circuits with Cobra4 Xpert-Link
Student's Sheet RLC-circuits with Cobra4 Xpert-Link (Item No.: P2440664) Curricular Relevance Area of Expertise: Physics Subtopic: Inductance, Electromagnetic Oscillations, AC Circuits Topic: Electricity
More informationChapter 6: Alternating Current
hapter 6: Alternating urrent 6. Alternating urrent.o 6.. Define alternating current (A) An alternating current (A) is the electrical current which varies periodically with time in direction and magnitude.
More informationECE 231 Laboratory Exercise 3 Oscilloscope/Function-Generator Operation ECE 231 Laboratory Exercise 3 Oscilloscope/Function Generator Operation
ECE 231 Laboratory Exercise 3 Oscilloscope/Function Generator Operation Laboratory Group (Names) OBJECTIVES Gain experience in using an oscilloscope to measure time varying signals. Gain experience in
More informationRLC Circuit with Cobra3
RLC Circuit with Cobra3 LEP Related topics Tuned circuit, series-tuned circuit, parallel-tuned circuit, resistance, capacitance, inductance, capacitor, coil, phase displacement, Q-factor, band-width,impedance,
More informationStudy of Inductive and Capacitive Reactance and RLC Resonance
Objective Study of Inductive and Capacitive Reactance and RLC Resonance To understand how the reactance of inductors and capacitors change with frequency, and how the two can cancel each other to leave
More informationExp. #2-6 : Measurement of the Characteristics of,, and Circuits by Using an Oscilloscope
PAGE 1/14 Exp. #2-6 : Measurement of the Characteristics of,, and Circuits by Using an Oscilloscope Student ID Major Name Team No. Experiment Lecturer Student's Mentioned Items Experiment Class Date Submission
More informationPHY203: General Physics III Lab page 1 of 5 PCC-Cascade. Lab: AC Circuits
PHY203: General Physics III Lab page 1 of 5 Lab: AC Circuits OBJECTIVES: EQUIPMENT: Universal Breadboard (Archer 276-169) 2 Simpson Digital Multimeters (464) Function Generator (Global Specialties 2001)*
More informationLab 8 - INTRODUCTION TO AC CURRENTS AND VOLTAGES
08-1 Name Date Partners ab 8 - INTRODUCTION TO AC CURRENTS AND VOTAGES OBJECTIVES To understand the meanings of amplitude, frequency, phase, reactance, and impedance in AC circuits. To observe the behavior
More informationInductance of solenoids
Inductance of solenoids TEP Related Topics Law of inductance, Lenz s law, self-inductance, solenoids, transformer, coupled oscillatory circuit, resonance, damped oscillation, logarithmic decrement Principle
More informationClass XII Chapter 7 Alternating Current Physics
Question 7.1: A 100 Ω resistor is connected to a 220 V, 50 Hz ac supply. (a) What is the rms value of current in the circuit? (b) What is the net power consumed over a full cycle? Resistance of the resistor,
More informationEE2210 Laboratory Project 1 Fall 2013 Function Generator and Oscilloscope
EE2210 Laboratory Project 1 Fall 2013 Function Generator and Oscilloscope For students to become more familiar with oscilloscopes and function generators. Pre laboratory Work Read the TDS 210 Oscilloscope
More informationChapter 31. Alternating Current. PowerPoint Lectures for University Physics, 14th Edition Hugh D. Young and Roger A. Freedman Lectures by Jason Harlow
Chapter 31 Alternating Current PowerPoint Lectures for University Physics, 14th Edition Hugh D. Young and Roger A. Freedman Lectures by Jason Harlow Learning Goals for Chapter 31 Looking forward at How
More informationLab 9 - AC Filters and Resonance
Lab 9 AC Filters and Resonance L9-1 Name Date Partners Lab 9 - AC Filters and Resonance OBJECTIES To understand the design of capacitive and inductive filters. To understand resonance in circuits driven
More informationPhysics for Scientists & Engineers 2 2 = 1 LC. Review ( ) Review (2) Review (3) e! Rt. cos "t + # ( ) q = q max. Spring Semester 2005 Lecture 30 U E
Review hysics for Scientists & Engineers Spring Semester 005 Lecture 30! If we have a single loop RLC circuit, the charge in the circuit as a function of time is given by! Where q = q max e! Rt L cos "t
More informationLecture 4 - Three-phase circuits, transformer and transient analysis of RLC circuits. Figure 4.1
Lecture 4 - Three-phase circuits, transformer and transient analysis of RLC circuits Power supply to sizeable power converters are often from three-phase AC source. A balanced three-phase source consists
More informationECE215 Lecture 7 Date:
Lecture 7 Date: 29.08.2016 AC Circuits: Impedance and Admittance, Kirchoff s Laws, Phase Shifter, AC bridge Impedance and Admittance we know: we express Ohm s law in phasor form: where Z is a frequency-dependent
More informationExperiment 18: Driven RLC Circuit
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8. Spring 3 Experiment 8: Driven LC Circuit OBJECTIVES To measure the resonance frequency and the quality factor of a driven LC circuit INTODUCTION
More informationCircuit Analysis-II. Circuit Analysis-II Lecture # 2 Wednesday 28 th Mar, 18
Circuit Analysis-II Angular Measurement Angular Measurement of a Sine Wave ü As we already know that a sinusoidal voltage can be produced by an ac generator. ü As the windings on the rotor of the ac generator
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.02 Spring Experiment 11: Driven RLC Circuit
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics 8.2 Spring 24 Experiment 11: Driven LC Circuit OBJECTIVES 1. To measure the resonance frequency and the quality factor of a driven LC circuit.
More informationExperiment 9: AC circuits
Experiment 9: AC circuits Nate Saffold nas2173@columbia.edu Office Hour: Mondays, 5:30PM-6:30PM @ Pupin 1216 INTRO TO EXPERIMENTAL PHYS-LAB 1493/1494/2699 Introduction Last week (RC circuit): This week:
More informationFilters And Waveform Shaping
Physics 3330 Experiment #3 Fall 2001 Purpose Filters And Waveform Shaping The aim of this experiment is to study the frequency filtering properties of passive (R, C, and L) circuits for sine waves, and
More informationCHAPTER 6: ALTERNATING CURRENT
CHAPTER 6: ALTERNATING CURRENT PSPM II 2005/2006 NO. 12(C) 12. (c) An ac generator with rms voltage 240 V is connected to a RC circuit. The rms current in the circuit is 1.5 A and leads the voltage by
More informationAPPENDIX D DISCUSSION OF ELECTRONIC INSTRUMENTS
APPENDIX D DISCUSSION OF ELECTRONIC INSTRUMENTS DC POWER SUPPLIES We will discuss these instruments one at a time, starting with the DC power supply. The simplest DC power supplies are batteries which
More informationSINUSOIDS February 4, ELEC-281 Network Theory II Wentworth Institute of Technology. Bradford Powers Ryan Ferguson Richard Lupa Benjamin Wolf
SINUSOIDS February 4, 28 ELEC-281 Network Theory II Wentworth Institute of Technology Bradford Powers Ryan Ferguson Richard Lupa Benjamin Wolf Abstract: Sinusoidal waveforms are studied in three circuits:
More informationElectrical Engineering Fundamentals
Electrical Engineering Fundamentals EE-238 Sheet 1 Series Circuits 1- For the circuits shown below, the total resistance is specified. Find the unknown resistance and the current for each circuit. 12.6
More informationExercise 1: Series RLC Circuits
RLC Circuits AC 2 Fundamentals Exercise 1: Series RLC Circuits EXERCISE OBJECTIVE When you have completed this exercise, you will be able to analyze series RLC circuits by using calculations and measurements.
More informationDC and AC Circuits. Objective. Theory. 1. Direct Current (DC) R-C Circuit
[International Campus Lab] Objective Determine the behavior of resistors, capacitors, and inductors in DC and AC circuits. Theory ----------------------------- Reference -------------------------- Young
More informationLab 9 AC FILTERS AND RESONANCE
151 Name Date Partners ab 9 A FITES AND ESONANE OBJETIES OEIEW To understand the design of capacitive and inductive filters To understand resonance in circuits driven by A signals In a previous lab, you
More informationPHY 132 Summer 2000 LAB 9: LRC Circuit (Phases) 1
PHY 132 Summer 2000 LAB 9: LRC Circuit (Phases) 1 Introduction In this lab we will measure the phases (voltage vs current) for each component in a series LRC circuit. Theory L C V_in R Fig. 1 Generic series
More informationEECS40 RLC Lab guide
EECS40 RLC Lab guide Introduction Second-Order Circuits Second order circuits have both inductor and capacitor components, which produce one or more resonant frequencies, ω0. In general, a differential
More informationRLC Frequency Response
1. Introduction RLC Frequency Response The student will analyze the frequency response of an RLC circuit excited by a sinusoid. Amplitude and phase shift of circuit components will be analyzed at different
More informationLaboratory 2 (drawn from lab text by Alciatore)
Laboratory 2 (drawn from lab text by Alciatore) Instrument Familiarization and Basic Electrical Relations Required Components: 2 1k resistors 2 1M resistors 1 2k resistor Objectives This exercise is designed
More informationExperiment 1: Instrument Familiarization (8/28/06)
Electrical Measurement Issues Experiment 1: Instrument Familiarization (8/28/06) Electrical measurements are only as meaningful as the quality of the measurement techniques and the instrumentation applied
More informationLab 1: Basic RL and RC DC Circuits
Name- Surname: ID: Department: Lab 1: Basic RL and RC DC Circuits Objective In this exercise, the DC steady state response of simple RL and RC circuits is examined. The transient behavior of RC circuits
More informationLABORATORY 4. Palomar College ENGR210 Spring 2017 ASSIGNED: 3/21/17
LABORATORY 4 ASSIGNED: 3/21/17 OBJECTIVE: The purpose of this lab is to evaluate the transient and steady-state circuit response of first order and second order circuits. MINIMUM EQUIPMENT LIST: You will
More informationExperiment 4: Grounding and Shielding
4-1 Experiment 4: Grounding and Shielding Power System Hot (ed) Neutral (White) Hot (Black) 115V 115V 230V Ground (Green) Service Entrance Load Enclosure Figure 1 Typical residential or commercial AC power
More informationChapter 33. Alternating Current Circuits
Chapter 33 Alternating Current Circuits C HAP T E O UTLI N E 33 1 AC Sources 33 2 esistors in an AC Circuit 33 3 Inductors in an AC Circuit 33 4 Capacitors in an AC Circuit 33 5 The L Series Circuit 33
More informationUNIVERSITI MALAYSIA PERLIS
UNIVERSITI MALAYSIA PERLIS ANALOG ELECTRONICS II EMT 212 2009/2010 EXPERIMENT # 3 OP-AMP (OSCILLATORS) 1 1. OBJECTIVE: 1.1 To demonstrate the Wien bridge oscillator 1.2 To demonstrate the RC phase-shift
More informationCHAPTER 9. Sinusoidal Steady-State Analysis
CHAPTER 9 Sinusoidal Steady-State Analysis 9.1 The Sinusoidal Source A sinusoidal voltage source (independent or dependent) produces a voltage that varies sinusoidally with time. A sinusoidal current source
More informationExperiment #2 Half Wave Rectifier
PURPOSE: ELECTRONICS 224 ETR620S Experiment #2 Half Wave Rectifier This laboratory session acquaints you with the operation of a diode power supply. You will study the operation of half-wave and the effect
More informationExercise 1: Inductors
Exercise 1: Inductors EXERCISE OBJECTIVE When you have completed this exercise, you will be able to describe the effect an inductor has on dc and ac circuits by using measured values. You will verify your
More informationGroup: Names: (1) In this step you will examine the effects of AC coupling of an oscilloscope.
3.5 Laboratory Procedure / Summary Sheet Group: Names: (1) In this step you will examine the effects of AC coupling of an oscilloscope. Set the function generator to produce a 5 V pp 1kHz sinusoidal output.
More informationAC Fundamental. Simple Loop Generator: Whenever a conductor moves in a magnetic field, an emf is induced in it.
AC Fundamental Simple Loop Generator: Whenever a conductor moves in a magnetic field, an emf is induced in it. Fig.: Simple Loop Generator The amount of EMF induced into a coil cutting the magnetic lines
More informationExperiment P45: LRC Circuit (Power Amplifier, Voltage Sensor)
PASCO scientific Vol. 2 Physics Lab Manual: P45-1 Experiment P45: (Power Amplifier, Voltage Sensor) Concept Time SW Interface Macintosh file Windows file circuits 30 m 700 P45 P45_LRCC.SWS EQUIPMENT NEEDED
More informationWorksheet for Exploration 31.1: Amplitude, Frequency and Phase Shift
Worksheet for Exploration 31.1: Amplitude, Frequency and Phase Shift We characterize the voltage (or current) in AC circuits in terms of the amplitude, frequency (period) and phase. The sinusoidal voltage
More informationVALLIAMMAI ENGINEERING COLLEGE
VALLIAMMAI ENGINEERING COLLEGE SRM NAGAR, KATTANKULATHUR 603203 DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING EE8261-ELECTRIC CIRCUITS LABORATORY LABORATORY MANUAL 1 ST YEAR EEE (REGULATION 2017)
More informationExperiment 2: Transients and Oscillations in RLC Circuits
Experiment 2: Transients and Oscillations in RLC Circuits Will Chemelewski Partner: Brian Enders TA: Nielsen See laboratory book #1 pages 5-7, data taken September 1, 2009 September 7, 2009 Abstract Transient
More informationUniversity of Pittsburgh
University of Pittsburgh Experiment #11 Lab Report Inductance/Transformers Submission Date: 12/04/2017 Instructors: Dr. Minhee Yun John Erickson Yanhao Du Submitted By: Nick Haver & Alex Williams Station
More informationExercise 6 AC voltage measurements average responding voltmeters
Exercise 6 AC voltage measurements average responding voltmeters 1. Aim of the exercise The aim of the exercise is to familiarize students with the AC voltage measurements by means of rectified average
More informationFigure 4.1 Vector representation of magnetic field.
Chapter 4 Design of Vector Magnetic Field Sensor System 4.1 3-Dimensional Vector Field Representation The vector magnetic field is represented as a combination of three components along the Cartesian coordinate
More information#8A RLC Circuits: Free Oscillations
#8A RL ircuits: Free Oscillations Goals In this lab we investigate the properties of a series RL circuit. Such circuits are interesting, not only for there widespread application in electrical devices,
More informationENGINEERING COUNCIL CERTIFICATE LEVEL ENGINEERING SCIENCE C103 TUTORIAL 18 ALTERNATING CURRENT
ENGINEERING OUNIL ERTIFIATE LEVEL ENGINEERING SIENE 03 TUTORIAL 8 ALTERNATING URRENT On completion of this tutorial you should be able to do the following. Explain alternating current. Explain Root Mean
More informationAVTECH TECHNICAL BRIEF 15 (TB15) A COMPARISON OF REVERSE RECOVERY MEASUREMENT SYSTEMS
A V T E C H E L E C T R O S Y S T E M S L T D. N A N O S E C O N D W A V E F O R M E L E C T R O N I C S S I N C E 1 9 7 5 P.O. BOX 265 OGDENSBURG, NY U.S.A. 13669-0265 TEL: 888-670-8729 (USA & Canada)
More informationElectronics and Instrumentation ENGR-4300 Spring 2004 Section Experiment 5 Introduction to AC Steady State
Experiment 5 Introduction to C Steady State Purpose: This experiment addresses combinations of resistors, capacitors and inductors driven by sinusoidal voltage sources. In addition to the usual simulation
More informationAC Theory and Electronics
AC Theory and Electronics An Alternating Current (AC) or Voltage is one whose amplitude is not constant, but varies with time about some mean position (value). Some examples of AC variation are shown below:
More informationET1210: Module 5 Inductance and Resonance
Part 1 Inductors Theory: When current flows through a coil of wire, a magnetic field is created around the wire. This electromagnetic field accompanies any moving electric charge and is proportional to
More informationECE 53A: Fundamentals of Electrical Engineering I
ECE 53A: Fundamentals of Electrical Engineering I Laboratory Assignment #1: Instrument Operation, Basic Resistor Measurements and Kirchhoff s Laws Fall 2007 General Guidelines: - Record data and observations
More informationFigure 1a Three small inductors are show what inductors look like. Figure 1b Three large inductors
A Series RLC Circuit This lab will let you learn the characteristics of both amplitude and phase of a series RLC circuit. Theory nductors and Capacitors Resistors (R), inductors (L) and capacitors (C)
More informationChapter 28 Alternating Current Circuits
History teaches us that the searching spirit of man required thousands of years for the discovery of the fundamental principles of the sciences, on which the superstructure was then raised in a comparatively
More information