Resistive-Inductive (RL) Circuits

Slides:



Advertisements
Similar presentations
Chapter 11 Inductors.
Advertisements

Complex Numbers for AC Circuits Topics Covered in Chapter : Positive and Negative Numbers 24-2: The j Operator 24-3: Definition of a Complex Number.
Chapter 12 RL Circuits.
Chapter 19 Methods of AC Analysis. 2 Dependent Sources Voltages and currents of independent sources –Not dependent upon any voltage or current elsewhere.
Electronics Inductive Reactance Copyright © Texas Education Agency, All rights reserved.
Sinusoidal Steady-State Power Calculations
Alternating Current Circuits
Parallel AC Circuits Analysis ET 242 Circuit Analysis II Electrical and Telecommunication Engineering Technology Professor Jang.
R,L, and C Elements and the Impedance Concept
Lesson 24 AC Power and Power Triangle
Copyright © 2009 Pearson Education, Inc. Lecture 10 – AC Circuits.
chapter 33 Alternating Current Circuits
AC POWER ANALYSIS Tunku Muhammad Nizar Bin Tunku Mansur
SINGLE PHASE A.C CIRCUITS
Chapter 7 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Chapter 4 Electrical Principles
AC POWER ANALYSIS Tunku Muhammad Nizar Bin Tunku Mansur
ELECTRIC CIRCUIT ANALYSIS - I
Fundamentals of Electric Circuits Chapter 11
Series and Parallel AC Circuits
Chapter 4 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Chapter 15 – Series & Parallel ac Circuits Lecture 20 by Moeen Ghiyas 19/08/
ELECTRIC CIRCUIT ANALYSIS - I
ARRDEKTA INSTITUTE OF TECHNOLOGY GUIDED BY GUIDED BY Prof. R.H.Chaudhary Prof. R.H.Chaudhary Asst.prof in electrical Asst.prof in electrical Department.
AC Circuits & Phasors. We want to understand RLC circuits driven with a sinusoidal emf. First: engineers characterize the amplitude of a sinusoidal emf.
Copyright © 2009 Pearson Education, Inc. Chapter 30 Inductance, Electromagnetic Oscillations, and AC Circuits.
RLC Circuits and Resonance
AC electric circuits 1.More difficult than DC circuits 2. Much more difficult than DC circuits 3. You can do it!
Fundamentals of Electric Circuits Chapter 11
ELECTRICAL ENGINEERING: PRINCIPLES AND APPLICATIONS, Fourth Edition, by Allan R. Hambley, ©2008 Pearson Education, Inc. Lecture 16 Phasor Circuits, AC.
1 © Unitec New Zealand DE4401 AC PHASORS BASICS. AC Resistors 2 © Unitec New Zealand.
1 Alternating Current Circuits Chapter Inductance CapacitorResistor.
Fall 2000EE201Phasors and Steady-State AC1 Phasors A concept of phasors, or rotating vectors, is used to find the AC steady-state response of linear circuits.
Enrollment no.: Abhi P. Choksi Anuj Watal Esha N. Patel Guidied by: M. K. Joshi, P.R.Modha A.D.PATEL.INSTITUTE.
Storey: Electrical & Electronic Systems © Pearson Education Limited 2004 OHT 15.1 Alternating Voltages and Currents  Introduction  Voltage and Current.
SUBELEMENT E5 ELECTRICAL PRINCIPLES [4 Exam Questions - 4 Groups] Electrical Principles1.
AC Series-Parallel Circuits Chapter 18. AC Circuits 2 Rules and laws developed for dc circuits apply equally well for ac circuits Analysis of ac circuits.
Electric Circuits.
DC & AC BRIDGES Part 2 (AC Bridge).
Copyright © 2009 Pearson Education, Inc. Chapter 33 Inductance, Electromagnetic Oscillations, and AC Circuits Part II.
1 ELECTRICAL TECHNOLOGY ET 201  Define series impedances and analyze series AC circuits using circuit techniques.
EEE107 AC Circuits 1.
1 ELECTRICAL TECHNOLOGY EET 103/4  Define and explain sine wave, frequency, amplitude, phase angle, complex number  Define, analyze and calculate impedance,
Today Course overview and information 09/16/2010 © 2010 NTUST.
Unit 8 Phasors.
1 ECE 3336 Introduction to Circuits & Electronics Set #15 Complex Power Fall 2011, TUE&TH 4-5:30 pm Dr. Wanda Wosik.
Chapter 10 Sinusoidal Steady- State Power Calculations
1  Explain and calculate average power, apparent power, reactive power  Calculate the total P, Q and S and sketch the power triangle. ELECTRICAL TECHNOLOGY.
Chapter 31 Lecture 33: Alternating Current Circuits: II HW 11 (problems): 30.58, 30.65, 30.76, 31.12, 31.26, 31.46, 31.56, Due Friday, Dec 11. Final.
Single-phase series a.c. circuits. Purely resistive a.c. circuit In a purely resistive a.c. circuit, the current I R and applied voltage V R are in phase.
Lecture 03: AC RESPONSE ( REACTANCE N IMPEDANCE ).
AC POWER ANALYSIS. 2 Content Average Power Maximum Average Power Transfer Complex Power Power Factor Correction.
AC POWER & POWER FACTOR. Lesson Objectives  Compute and define apparent, reactive, and average power for capacitors, inductors, and resistors.  Compute.
Chapter 19 Principles of Electric Circuits, Conventional Flow, 9 th ed. Floyd © 2010 Pearson Higher Education, Upper Saddle River, NJ All Rights.
Chapter 13 The Basic Elements and Phasors. Objectives Be able to add and subtract sinusoidal voltages or currents Use phasor format to add and subtract.
Chapter 10 RC Circuits.
Chapter 14 Series and Parallel AC Circuits. Objectives Become familiar with the characteristics of a series and parallel ac circuit Find the total impedance.
RC Circuits (sine wave)
Chapter 13 The Basic Elements and Phasors. Objectives Be able to add and subtract sinusoidal voltages or currents Use phasor format to add and subtract.
Chapter 12 RL Circuits.
Lesson 3: Ac Power in Single Phase Circuits
Lesson 21: AC Power and Power Triangle
Lecture 07 AC POWER & POWER FACTOR.
AC POWER & POWER FACTOR.
Chapter 17 Resonance Circuits.
Sinusoidal Excitation of Circuits
Lecture 6 (III): AC RESPONSE
Introduction to AC Bridge.
Parallel AC Circuits Analysis
Chapter 15.
Presentation transcript:

Resistive-Inductive (RL) Circuits AC Circuits I

Series RL Circuits Series circuits: A comparison (Magnitude) IT = IR1 = IR2 IT = IL1=IL2 IT = IL=IR VT =VR1+VR2 VT = j(VL1 + VL2) |VT| = sqrt(VR2 + VL2) RT = R1+R2 XT = XL1 + XL2 |ZT| = sqrt(R2 + XL2)

Series RL Circuits Series Voltages

Series RL Circuits Series Voltages (Continued) Since VL leads VR by 90°, the values of the component voltages are usually represented using phasors Phasor – a vector used to represent a value that constantly changes phase. Usually denoted in a polar form r@θ.

Series RL circuits Series Impedance Polar form Polar form Rectangular form Rectangular form

Example The component voltages shown below were measured using an ac voltmeter (HINT: rms values!!!). Calculate the source voltage for the circuit.

Example Calculate the total impedance for the circuit shown (remember Z = R +jXL , where XL=2πfL )

Phase Reference In a series RL circuit the current I and voltage across the resistor VR are considered to have 0o phase. Sometimes however (especially in the lab) the source voltage Vs is assumed to have 0o phase.

Example Calculate the circuit impedance, and current in the circuit shown below I and Vs can be represented as either: (I lags Vs or Vs leads I)

Example Determine the voltage, current and impedance values for the circuit shown below

Voltage Dividers RL Voltage Dividers In a series RL circuit where I(VR )is used as the 0o phase reference, Vs and ZT always have the same phase angle!!! where Zn = magnitude of R or XL Vn = voltage across the component

Example Determine the voltages VL and VR in the circuit below

Example Calculate ZT, VL1 VL2 and VR for the circuit shown below.

Series RL Circuit Frequency Response Frequency Response – used to describe any changes that occur in a circuit as a result of a change in operating frequency An increase in frequency causes XL to increase An increase in XL causes ZT and  to increase An increase in ZT causes IT to decrease An increase in XL causes VL to increase An increase in VL causes VR to decrease

Power Power is also a complex quantity in AC circuits

Apparent, True and Reactive Power Value Definition Resistive power (PR) The power dissipated by the resistance in an RL circuit. Also known as true power. Reactive power (PX) The value found using P = I2XL. Also known as imaginary power. The energy stored by the inductor in its electromagnetic field. PX is measured in volt-amperes-reactive (VARs) to distinguish it from true power. Apparent power (PAPP) The combination of resistive (true) power and reactive (imaginary) power. Measured in volt-amperes (VAs).

Power Factor (PF) The ratio of resistive power to apparent power

Example Calculate PR, PX and PAPP for the following circuit - (see slide 13)

Parallel RL Circuits Note that VS, IR and VR are all in phase IL is 90o out of phase with (lags) VS, IR and VR. VS = VR1 = VR2 VS = VL1 = VL2 VT = VL= VR IT =IR1+IR2 IT = j(IL1 + IL2) |IT|= sqrt(IR2 + IL2) RT = 1/[ (1/R1 )+(1/R2)] XT = 1/[(1/XL1 ) + (1/XL2 )] XT = 1/[(1/R ) + (1/jXL )]

Parallel RL Circuits Branch Currents IL lags IR , VR and VS by 90º

Parallel RL Circuits Parallel Circuit Impedance Impedance phase angle is positive since current phase angle is negative Angles of ZT and IT have the same magnitude but opposite signs Calculating Parallel-Circuit Impedance (polar form)

Parallel RL Circuits Calculating Parallel-Circuit Impedance rectangular form approach:

Parallel RL Circuits Parallel-Circuit Frequency Response The increase in frequency causes XL to increase The increase in XL causes: IL to decrease IT to increase ZT to increase The decrease in IL causes IT to decrease

Example 1 Calculate the total current for circuit (a) in both rectangular and polar forms Calculate total impedance of circuit (a) Repeat for circuit (b)

Example 2 (Rectangular) Calculate the total impedance for circuit (a) in both rectangular and polar forms Calculate total current of circuit (a) Repeat for circuit (b)

Example 2 (Polar) Calculate the total impedance for circuit (a) in both rectangular and polar forms Calculate total current of circuit (a) Repeat for circuit (b)

Series –Parallel RL Circuits First collapse the parallel RL portion into a single impedance ZP If this single impedance is in polar form, convert it to rectangular form Add any resistances/ reactances in series with ZP to get ZT. Remember you cannot add complex numbers in their polar form. Always assume that IT is the zero Phase reference!! And that VS and ZT have the same phase i.e. Same assumption as for series RL circuit

Example Calculate the Equivalent Impedance, the total current and the current in each branch of the parallel RL circuit shown below Now convert to rect and back to polar

Example Cont’d Knowing that Remember in a series circuit, IT is the phase reference and VS and ZT always have the same phase!!!

Example Cont’d Alternatively using a current divider equation Does IT = IL + IR2?

Remember!! For Series RL Circuits For Parallel RL Circuits IT and VR are the 0o phase reference VS and ZT have the same phase For Parallel RL Circuits VS is the 0o phase reference IT and ZT have the same phase magnitude but opposite signs For Series-Parallel RL Circuits Use same rules as Series RL Circuits