Lecture 13 Second-order Circuits (1) Hung-yi Lee.

Slides:



Advertisements
Similar presentations
Kevin D. Donohue, University of Kentucky1 Transient Response for Second- Order Circuits Characteristics Equations, Overdamped-, Underdamped-, and Critically.
Advertisements

Lecture - 9 Second order circuits
Previous Lectures Source free RL and RC Circuits.
Reading Assignment: Chapter 8 in Electric Circuits, 9th Ed. by Nilsson
Lecture 10 Capacitor and Inductor Hung-yi Lee. Outline Capacitor (Chapter 5.1) Inductor (Chapter 5.2) Comparison of Capacitor and Inductor Superposition.
Lecture 11 First-order Circuits (1) Hung-yi Lee. Dynamic Circuits Capacitor, Inductor (Chapter 5) Frequency Domain Time Domain (Chapter 6,7) S-Domain.
Circuits Lecture 4: Superposition
Lecture 26 Laplace Transform for Circuit Analysis Hung-yi Lee.
Lecture 12 First-order Circuits (2) Hung-yi Lee. Outline Non-constant Sources for First-Order Circuits (Chapter 5.3, 9.1)
Lecture 6 Controlled Sources (2)
E E 2315 Lecture 11 Natural Responses of Series RLC Circuits.
RLC Circuits Natural Response ECE 201 Circuit Theory I.
2nd Order Circuits Lecture 16.
Lecture 171 Higher Order Circuits. Lecture 172 Higher Order Circuits The text has a chapter on 1st order circuits and a chapter on 2nd order circuits.
ECE53A Introduction to Analog and Digital Circuits Lecture Notes Second-Order Analog Circuit and System.
Lecture 17 AC Circuit Analysis (2) Hung-yi Lee. Textbook AC Circuit Analysis as Resistive Circuits Chapter 6.3, Chapter 6.5 (out of the scope) Fourier.
Fundamentals of Electric Circuits Chapter 8
Circuits Lecture 3: Mesh Analysis 李宏毅 Hung-yi Lee.
Circuits Lecture 2: Node Analysis 李宏毅 Hung-yi Lee.
Lecture 21 Network Function and s-domain Analysis Hung-yi Lee.
Lecture 18 Power in AC Circuits Hung-yi Lee. Outline Textbook: Chapter 7.1 Computing Average Power Maximum Power Transfer for AC circuits Maximum Power.
Lecture 14 Second-order Circuits (2)
Mechanical and Electrical Vibrations. Applications.
Lecture 181 Second-Order Circuits (6.3) Prof. Phillips April 7, 2003.
Lect16EEE 2021 System Responses Dr. Holbert March 24, 2008.
Series RLC Network. Objective of Lecture Derive the equations that relate the voltages across a resistor, an inductor, and a capacitor in series as: the.
Chapter 5 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Source-Free RLC Circuit
Parallel RLC Network. Objective of Lecture Derive the equations that relate the voltages across a resistor, an inductor, and a capacitor in parallel as:
Chapter 8 Second-Order Circuits
Fundamentals of Electric Circuits Chapter 8
6. RLC CIRCUITS CIRCUITS by Ulaby & Maharbiz. Overview.
Series RLC Network. Objective of Lecture Derive the equations that relate the voltages across a resistor, an inductor, and a capacitor in series as: the.
Lecture 12 - Natural Response of Parallel RLC Circuits
Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 1 Chapter 9 The RLC Circuit.
九十七學年度第二學期 電路學(二)授課綱要
ELECTRICAL ENGINEERING: PRINCIPLES AND APPLICATIONS, Fourth Edition, by Allan R. Hambley, ©2008 Pearson Education, Inc. Lecture 14 Second Order Transient.
305221, Computer Electrical Circuit Analysis การวิเคราะห์วงจรไฟฟ้าทาง คอมพิวเตอร์ 3(2-3-6) ณรงค์ชัย มุ่งแฝงกลาง คมกริช มาเที่ยง สัปดาห์ที่ 11 Frequency.
Oscillators fall CM lecture, week 4, 24.Oct.2002, Zita, TESC Review simple harmonic oscillators Examples and energy Damped harmonic motion Phase space.
Chapter 4 Second Order Circuit (11th & 12th week)
1 Lecture #1 EGR 272 – Circuit Theory II Reading Assignment: Chapter 8 in Electric Circuits, 6th Edition by Nilsson Welcome to EGR 272 Circuit Theory II.
Lecture 5 Controlled Sources (1) Hung-yi Lee. Textbook Chapter 2.3, 3.2.
Second Order Circuits ES-3 Download:
Step Response Series RLC Network.
Alexander-Sadiku Fundamentals of Electric Circuits
Assist.Prof. Aysun Taşyapı ÇELEBİ Electronics and Communication Engineering University of Kocaeli.
1 Lecture D32 : Damped Free Vibration Spring-Dashpot-Mass System Spring Force k > 0 Dashpot c > 0 Newton’s Second Law (Define) Natural Frequency and Period.
Chapter 4 Transients. 1.Solve first-order RC or RL circuits. 2. Understand the concepts of transient response and steady-state response.
LCR circuit R V0 L I(t)=0 for t<0 V(t) C + trial solution
SECOND ORDER CIRCUIT. Revision of 1 st order circuit Second order circuit Natural response (source-free) Forced response SECOND ORDER CIRCUIT.
Week 6 Second Order Transient Response. Topics Second Order Definition Dampening Parallel LC Forced and homogeneous solutions.
Apply KCL to the top node ,we have We normalize the highest derivative by dividing by C , we get Since the highest derivative in the equation is.
1 EKT101 Electric Circuit Theory Chapter 5 First-Order and Second Circuits.
Chapter 5 Transient Analysis Tai-Cheng Lee Electrical Engineering/GIEE 1.
Y.M. Hu, Assistant Professor, Department of Applied Physics, National University of Kaohsiung Chapter 2 Linear Differential Equations of Second and Higher.
Chapter 5 First-Order and Second Circuits 1. First-Order and Second Circuits Chapter 5 5.1Natural response of RL and RC Circuit 5.2Force response of RL.
Source-Free Series RLC Circuits.
Lecture - 7 First order circuits. Outline First order circuits. The Natural Response of an RL Circuit. The Natural Response of an RC Circuit. The Step.
1 ECE 3301 General Electrical Engineering Section 30 Natural Response of a Parallel RLC Circuit.
Chapter 6 Second-Order Circuit.
Previous Lecture 29 Second-Order Circuit
EENG 2610: Circuit Analysis Class 13: Second-Order Circuits
EKT101 Electric Circuit Theory
Source-Free RLC Circuit
ECE 222 Electric Circuit Analysis II Chapter 10 Natural Response
* 07/16/96 What is Second Order?
CHAPTER 5 Transient Analysis.
Chapter 8 Second Order Circuits
C H A P T E R 5 Transient Analysis.
Apply KCL to the top node ,we have We normalize the highest derivative by dividing by C , we get Since the highest derivative in the equation is.
Presentation transcript:

Lecture 13 Second-order Circuits (1) Hung-yi Lee

Second-order Circuits A second order-circuit contains two independent energy-storage elements (capacitors and inductors). Capacitor + inductor 2 inductors2 Capacitors

Second-order Circuits Steps for solving by differential equation (Chapter 9.3, 9.4) 1. List the differential equation (Chapter 9.3) 2. Find natural response (Chapter 9.3) There is some unknown variables in the natural response. 3. Find forced response (Chapter 9.4) 4. Find initial conditions (Chapter 9.4) 5. Complete response = natural response + forced response (Chapter 9.4) Find the unknown variables in the natural response by the initial conditions

Solving by differential equation Step 1: List Differential Equation

Systematic Analysis Mesh Analysis

Systematic Analysis Mesh Analysis Find i L : Find v C :

Systematic Analysis Node Analysis

Systematic Analysis Find v C : Node Analysis Systematic Analysis v C =v Find i L :

Example 9.6 Find i 2 v1v1 v2v2 v1:v1: v2:v2:

Example 9.6 Find i 2 v1v1 v2v2 Target: Equations for v 1 and v 2 Find v 2 from the left equations Then we can find i 2

Example 9.6 Find i 2 v1v1 v2v2 Find v 2

Example 9.6 Find i 2 v1v1 v2v2 Replace with

Example 9.7 Please refer to the appendix

Summary – List Differential Equations

Solving by differential equation Step 2: Find Natural Response

Natural Response The differential equation of the second-order circuits: y(t): current or voltage of an element α = damping coefficient ω 0 = resonant frequency

Natural Response The differential equation of the second-order circuits: Focus on y N (t) in this lecture

Natural Response y N (t) looks like: Characteristic equation

Natural Response λ 1, λ 2 is Overdamped Critical damped Complex Underdamped Undamped Real

Solving by differential equation Step 2: Find Natural Response Overdamped Response

λ 1, λ 2 are both real numbers y N (t) looks like

Overdamped Response

Solving by differential equation Step 2: Find Natural Response Underdamped Response

Underdamped

Euler's formula: y N (t) should be real.

Underdamped Euler's formula: y N (t) should be real. (no real part)

Underdamped a and b will be determined by initial conditions Memorize this!

Underdamped L and θ will be determined by initial conditions

Underdamped

Solving by differential equation Step 2: Find Natural Response Undamped Response

Undamped Undamped is a special case of underdamped.

Solving by differential equation Step 2: Find Natural Response Critical Damped Response

Critical Damped Underdamped Overdamped Critical damped Not complete

Critical Damped (Problem 9.44)

Solving by differential equation Step 2: Find Natural Response Summary

Fix ω 0, decrease α (α is positive): Overdamped Critical damped Underdamped Undamped Decrease α, smaller RDecrease α, increase R

α=0 Undamped Fix ω 0, decrease α (α is positive) The position of the two roots λ 1 and λ 2.

Homework

Thank You!

Answer 9.30: v1’’ + 3 v1’ + 10 v1 = : yN=a e^(-0.5t) + b te^(-0.5t) 9.36: yN=a e^(4t) + b e(-6t) 9.38: yN=2Ae^(3t) cos (6t+θ) or yN=2e^(3t) (acos6t + bsin6t) In 33, 36 and 38, we are not able to know the values of the unknown variables.

Appendix: Example 9.7

Example 9.7 Mesh current: i 1 and i c

Example 9.7 (1): (2): (2) – (1):

Example 9.7

Appendix: Figures from Other Textbooks

Undamped

Acknowledgement 感謝 陳尚甫 (b02) 指出投影片中 Equation 的錯誤 感謝 吳東運 (b02) 指出投影片中 Equation 的錯誤