EE16B, Spring 2018 UC Berkeley EECS. Maharbiz and Roychowdhury. Lecture 4A: Overview Slides. State Space Representations

Size: px
Start display at page:

Download "EE16B, Spring 2018 UC Berkeley EECS. Maharbiz and Roychowdhury. Lecture 4A: Overview Slides. State Space Representations"

Transcription

1 EE16B, Spring 2018 UC Berkeley EECS Maharbiz and Roychowdhury Lecture 4A: Overview Slides State Space Representations Slide 1

2 Systems Previously: circuits Now: systems circuits + more: a broader concept Can be enormously complex multi-domain EE (control, comm., computing,...) mech., chem., optical, hierarchy of sub-systems Slide 2

3 Simpler Systems easier to understand and to work with Even small and simple systems can do interesting things Slide 3

4 A Note about Intuition vs Math Proper intuition: extremely important quickly make mental leaps to solve problems and design new things avoiding confusion that can arise from masses of detail Intuition doesn t arise magically mathematics: essential for in-depth understanding math + experience and practice intuition may be wrong! Intuition backed by Math BEST: both! sometimes hard to translate math to intuition not very useful for design - but may be useful for, eg, understanding and computation Slide 4

5 Inputs and Outputs as VECTORS (move to xournal) Slide 5

6 The Internal State (move to xournal) Internal voltages/currents (unknowns): the state also written as a vector: Slide 6

7 The System s Equations (move to xournal) can be written using the input and state vectors Slide 7

8 The Outputs (move to xournal) also expressed using the input and state vectors Slide 8

9 State+Output Eqns Together general form:, + initial condition (IC) STATE SPACE FORMULATION * * if not explicitly given, the entire state will be the output. Slide 9

10 State Space Formulation: Benefits why is it useful? any circuit can be written like this (not just this one)* however big or complicated not just circuits any system* from any domain! including multi-domain systems POWERFUL ANALYSIS METHODS Any kind of system (EE, mech., chem., optical, multi-domain,...) STATE SPACE FORMULATION - phasor analysis - linearization - stability - controllability/observability - nonlinear analyses - computational methods Deeper understanding Powerful insights and intuition * some additional generalization needed won t cover in this class Slide 10

11 Previous Lecture examples + initial condition (IC) RLC circuit pendulum Any kind of system (EE, mech., chem., optical, multi-domain,...) STATE SPACE FORMULATION Slide 11

12 Mechanical Example: Pendulum (move to xournal) The system is nonlinear (because of sin(...)) Slide 12

13 Pendulum: simplification for small q k Does this look familiar? INSIGHT: RLC ckt and damped pendulum are the same! MEMS filters! Filters Filters?? (smaller, better, cheaper) Slide 13

14 Recap of Linearity The concept of LINEARITY is extremely important it is fundamentally a systems concept input SYSTEM output 3 steps to check linearity clearly identify your inputs and outputs (this affects linearity) check superposition if and if, then check scaling, then,, and Slide 14

15 Linearity of State Space Formulations general S.S.F: If, and matrices then the system is linear matrices Proof? Slide 15

16 Are these Systems Linear? Slide 16

17 State Space F. for Discrete Time Systems What is a discrete-time system? example: compound interest (move to xournal), general form: + initial condition (IC) given STATE SPACE FORMULATION Discrete time sometimes more natural (eg, for finance, social dynamics,...) Slide 17

18 Another D.T. Example: Profs. and PhDs. (move to xournal) Linear? VECTOR D.T. STATE-SPACE FORMULATION Slide 18

EE16B, Spring 2018 UC Berkeley EECS. Maharbiz and Roychowdhury. Lectures 4B & 5A: Overview Slides. Linearization and Stability

EE16B, Spring 2018 UC Berkeley EECS. Maharbiz and Roychowdhury. Lectures 4B & 5A: Overview Slides. Linearization and Stability EE16B, Spring 2018 UC Berkeley EECS Maharbiz and Roychowdhury Lectures 4B & 5A: Overview Slides Linearization and Stability Slide 1 Linearization Approximate a nonlinear system by a linear one (unless

More information

EE16B, Spring 2018 UC Berkeley EECS. Maharbiz and Roychowdhury. Lecture 5B: Open QA Session

EE16B, Spring 2018 UC Berkeley EECS. Maharbiz and Roychowdhury. Lecture 5B: Open QA Session EE16B, Spring 2018 UC Berkeley EECS Maharbiz and Roychowdhury Lecture 5B: Open QA Session EE16B, Spring 2018, Open Q/A Session (Roychowdhury) Slide 1 Today: Open Q/A Session primarily on state space r.

More information

Designing Information Devices and Systems II Spring 2018 J. Roychowdhury and M. Maharbiz Discussion 6B

Designing Information Devices and Systems II Spring 2018 J. Roychowdhury and M. Maharbiz Discussion 6B EECS 16B Designing Information Devices and Systems II Spring 2018 J. Roychowdhury and M. Maharbiz Discussion 6B 1 Stability 1.1 Discrete time systems A discrete time system is of the form: xt + 1 A xt

More information

Module 02 Control Systems Preliminaries, Intro to State Space

Module 02 Control Systems Preliminaries, Intro to State Space Module 02 Control Systems Preliminaries, Intro to State Space Ahmad F. Taha EE 5143: Linear Systems and Control Email: ahmad.taha@utsa.edu Webpage: http://engineering.utsa.edu/ taha August 28, 2017 Ahmad

More information

EE16B Designing Information Devices and Systems II

EE16B Designing Information Devices and Systems II EE6B M. Lustig, EECS UC Berkeley EE6B Designing Information Devices and Systems II Lecture 6B Cont. stability of Linear State Models Controllability Today Last time: Derived stability conditions for disc.

More information

MATH 312 Section 7.1: Definition of a Laplace Transform

MATH 312 Section 7.1: Definition of a Laplace Transform MATH 312 Section 7.1: Definition of a Laplace Transform Prof. Jonathan Duncan Walla Walla University Spring Quarter, 2008 Outline 1 The Laplace Transform 2 The Theory of Laplace Transforms 3 Conclusions

More information

Lecture A1 : Systems and system models

Lecture A1 : Systems and system models Lecture A1 : Systems and system models Jan Swevers July 2006 Aim of this lecture : Understand the process of system modelling (different steps). Define the class of systems that will be considered in this

More information

Linearization problem. The simplest example

Linearization problem. The simplest example Linear Systems Lecture 3 1 problem Consider a non-linear time-invariant system of the form ( ẋ(t f x(t u(t y(t g ( x(t u(t (1 such that x R n u R m y R p and Slide 1 A: f(xu f(xu g(xu and g(xu exist and

More information

AUTOMATIC CONTROL. Andrea M. Zanchettin, PhD Spring Semester, Introduction to Automatic Control & Linear systems (time domain)

AUTOMATIC CONTROL. Andrea M. Zanchettin, PhD Spring Semester, Introduction to Automatic Control & Linear systems (time domain) 1 AUTOMATIC CONTROL Andrea M. Zanchettin, PhD Spring Semester, 2018 Introduction to Automatic Control & Linear systems (time domain) 2 What is automatic control? From Wikipedia Control theory is an interdisciplinary

More information

Frequency Response Prof. Ali M. Niknejad Prof. Rikky Muller

Frequency Response Prof. Ali M. Niknejad Prof. Rikky Muller EECS 105 Spring 2017, Module 4 Frequency Response Prof. Ali M. Niknejad Department of EECS Announcements l HW9 due on Friday 2 Review: CD with Current Mirror 3 Review: CD with Current Mirror 4 Review:

More information

Physics 351 Wednesday, January 14, 2015

Physics 351 Wednesday, January 14, 2015 Physics 351 Wednesday, January 14, 2015 Read Chapter 1 for today. Two-thirds of you answered the Chapter 1 questions so far. Read Chapters 2+3 for Friday. Skim Chapter 4 for next Wednesday (1/21). Homework

More information

Numerical Methods for Inverse Kinematics

Numerical Methods for Inverse Kinematics Numerical Methods for Inverse Kinematics Niels Joubert, UC Berkeley, CS184 2008-11-25 Inverse Kinematics is used to pose models by specifying endpoints of segments rather than individual joint angles.

More information

EE16B Designing Information Devices and Systems II

EE16B Designing Information Devices and Systems II EE16B Designing Information Devices and Systems II Lecture 5A Control- state space representation Announcements Last time: Bode plots Resonance systes and Q HW 4 extended to Friday No hw this week. Study

More information

EE C245 ME C218 Introduction to MEMS Design Fall 2007

EE C245 ME C218 Introduction to MEMS Design Fall 2007 EE C245 ME C218 Introduction to MEMS Design Fall 2007 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley Berkeley, CA 94720 Lecture 17: Energy

More information

EE 40: Introduction to Microelectronic Circuits Spring 2008: Midterm 2

EE 40: Introduction to Microelectronic Circuits Spring 2008: Midterm 2 EE 4: Introduction to Microelectronic Circuits Spring 8: Midterm Venkat Anantharam 3/9/8 Total Time Allotted : min Total Points:. This is a closed book exam. However, you are allowed to bring two pages

More information

Difference Equations

Difference Equations 6.08, Spring Semester, 007 Lecture 5 Notes MASSACHVSETTS INSTITVTE OF TECHNOLOGY Department of Electrical Engineering and Computer Science 6.08 Introduction to EECS I Spring Semester, 007 Lecture 5 Notes

More information

Communication Engineering Prof. Surendra Prasad Department of Electrical Engineering Indian Institute of Technology, Delhi

Communication Engineering Prof. Surendra Prasad Department of Electrical Engineering Indian Institute of Technology, Delhi Communication Engineering Prof. Surendra Prasad Department of Electrical Engineering Indian Institute of Technology, Delhi Lecture - 3 Brief Review of Signals and Systems My subject for today s discussion

More information

Feedback Control part 2

Feedback Control part 2 Overview Feedback Control part EGR 36 April 19, 017 Concepts from EGR 0 Open- and closed-loop control Everything before chapter 7 are open-loop systems Transient response Design criteria Translate criteria

More information

Systems Analysis and Control

Systems Analysis and Control Systems Analysis and Control Matthew M. Peet Arizona State University Lecture 6: Generalized and Controller Design Overview In this Lecture, you will learn: Generalized? What about changing OTHER parameters

More information

Math (P)Review Part I:

Math (P)Review Part I: Lecture 1: Math (P)Review Part I: Linear Algebra Computer Graphics CMU 15-462/15-662, Fall 2017 Homework 0.0 (Due Monday!) Exercises will be a bit harder / more rigorous than what you will do for the rest

More information

EE C245 - ME C218 Introduction to MEMS Design Fall Today s Lecture

EE C245 - ME C218 Introduction to MEMS Design Fall Today s Lecture EE C45 - ME C8 Introduction to MEMS Design Fall 3 Roger Howe and Thara Srinivasan Lecture 9 Energy Methods II Today s Lecture Mechanical structures under driven harmonic motion develop analytical techniques

More information

Contents. Contents. Matrices. Contents. Objectives. Matrices

Contents. Contents. Matrices. Contents. Objectives. Matrices 9/8/7 Physics for Majors Class 8 Matrices and Lorentz s Space-time Four- Last Class Test Review Scalars and vectors Three-vectors and four-vectors The energy-momentum four-vector Rotations about the z

More information

Modern Algebra Prof. Manindra Agrawal Department of Computer Science and Engineering Indian Institute of Technology, Kanpur

Modern Algebra Prof. Manindra Agrawal Department of Computer Science and Engineering Indian Institute of Technology, Kanpur Modern Algebra Prof. Manindra Agrawal Department of Computer Science and Engineering Indian Institute of Technology, Kanpur Lecture 02 Groups: Subgroups and homomorphism (Refer Slide Time: 00:13) We looked

More information

Electromagnetic Waves

Electromagnetic Waves Electromagnetic Waves Our discussion on dynamic electromagnetic field is incomplete. I H E An AC current induces a magnetic field, which is also AC and thus induces an AC electric field. H dl Edl J ds

More information

Designing Information Devices and Systems II Spring 2018 J. Roychowdhury and M. Maharbiz Homework 5

Designing Information Devices and Systems II Spring 2018 J. Roychowdhury and M. Maharbiz Homework 5 EECS 16B Designing Information Devices and Systems II Spring 2018 J. Roychowdhury and M. Maharbiz Homework 5 This homework is due on Thursday, March 8, 2018, at 11:59AM (NOON). Self-grades are due on Monday,

More information

EE 330 Lecture 25. Amplifier Biasing (precursor) Two-Port Amplifier Model

EE 330 Lecture 25. Amplifier Biasing (precursor) Two-Port Amplifier Model EE 330 Lecture 25 Amplifier Biasing (precursor) Two-Port Amplifier Model Review from Last Lecture Exam Schedule Exam 2 Friday March 24 Review from Last Lecture Graphical Analysis and Interpretation 2 OX

More information

#29: Logarithm review May 16, 2009

#29: Logarithm review May 16, 2009 #29: Logarithm review May 16, 2009 This week we re going to spend some time reviewing. I say re- view since you ve probably seen them before in theory, but if my experience is any guide, it s quite likely

More information

Computational Methods CMSC/AMSC/MAPL 460. Fourier transform

Computational Methods CMSC/AMSC/MAPL 460. Fourier transform Computational Methods CMSC/AMSC/MAPL 460 Fourier transform Ramani Duraiswami, Dept. of Computer Science Several slides from Prof. Healy s course at UMD Fourier Methods Fourier analysis ( harmonic analysis

More information

Designing Information Devices and Systems I Spring 2018 Lecture Notes Note Introduction to Linear Algebra the EECS Way

Designing Information Devices and Systems I Spring 2018 Lecture Notes Note Introduction to Linear Algebra the EECS Way EECS 16A Designing Information Devices and Systems I Spring 018 Lecture Notes Note 1 1.1 Introduction to Linear Algebra the EECS Way In this note, we will teach the basics of linear algebra and relate

More information

The Hamiltonian and the Schrödinger equation Consider time evolution from t to t + ɛ. As before, we expand in powers of ɛ; we have. H(t) + O(ɛ 2 ).

The Hamiltonian and the Schrödinger equation Consider time evolution from t to t + ɛ. As before, we expand in powers of ɛ; we have. H(t) + O(ɛ 2 ). Lecture 12 Relevant sections in text: 2.1 The Hamiltonian and the Schrödinger equation Consider time evolution from t to t + ɛ. As before, we expand in powers of ɛ; we have U(t + ɛ, t) = I + ɛ ( īh ) H(t)

More information

Math Lecture 3 Notes

Math Lecture 3 Notes Math 1010 - Lecture 3 Notes Dylan Zwick Fall 2009 1 Operations with Real Numbers In our last lecture we covered some basic operations with real numbers like addition, subtraction and multiplication. This

More information

Course roadmap. ME451: Control Systems. Example of Laplace transform. Lecture 2 Laplace transform. Laplace transform

Course roadmap. ME451: Control Systems. Example of Laplace transform. Lecture 2 Laplace transform. Laplace transform ME45: Control Systems Lecture 2 Prof. Jongeun Choi Department of Mechanical Engineering Michigan State University Modeling Transfer function Models for systems electrical mechanical electromechanical Block

More information

Physics 132 3/31/17. March 31, 2017 Physics 132 Prof. E. F. Redish Theme Music: Benny Goodman. Swing, Swing, Swing. Cartoon: Bill Watterson

Physics 132 3/31/17. March 31, 2017 Physics 132 Prof. E. F. Redish Theme Music: Benny Goodman. Swing, Swing, Swing. Cartoon: Bill Watterson March 31, 2017 Physics 132 Prof. E. F. Redish Theme Music: Benny Goodman Swing, Swing, Swing Cartoon: Bill Watterson Calvin & Hobbes 1 Outline The makeup exam Recap: the math of the harmonic oscillator

More information

I Laplace transform. I Transfer function. I Conversion between systems in time-, frequency-domain, and transfer

I Laplace transform. I Transfer function. I Conversion between systems in time-, frequency-domain, and transfer EE C128 / ME C134 Feedback Control Systems Lecture Chapter 2 Modeling in the Frequency Domain Alexandre Bayen Department of Electrical Engineering & Computer Science University of California Berkeley Lecture

More information

Systems of Ordinary Differential Equations

Systems of Ordinary Differential Equations Systems of Ordinary Differential Equations MATH 365 Ordinary Differential Equations J Robert Buchanan Department of Mathematics Fall 2018 Objectives Many physical problems involve a number of separate

More information

Series, Parallel, and other Resistance

Series, Parallel, and other Resistance EELE 2310 Analysis Lecture 3 Equivalent s Series, Parallel, Delta-to-Wye, Voltage Divider and Current Divider Rules Dr Hala El-Khozondar Series, Parallel, and other Resistance Equivalent s ١ Overview Series,

More information

Math 333 Qualitative Results: Forced Harmonic Oscillators

Math 333 Qualitative Results: Forced Harmonic Oscillators Math 333 Qualitative Results: Forced Harmonic Oscillators Forced Harmonic Oscillators. Recall our derivation of the second-order linear homogeneous differential equation with constant coefficients: my

More information

West Windsor-Plainsboro Regional School District Math Resource Center Grade 8

West Windsor-Plainsboro Regional School District Math Resource Center Grade 8 West Windsor-Plainsboro Regional School District Math Resource Center Grade 8 Content Area: Mathematics Course & Grade Level: Math 8 Unit 1 - Foundations of Algebra Summary and Rationale This unit involves

More information

Section 1.5. Solution Sets of Linear Systems

Section 1.5. Solution Sets of Linear Systems Section 1.5 Solution Sets of Linear Systems Plan For Today Today we will learn to describe and draw the solution set of an arbitrary system of linear equations Ax = b, using spans. Ax = b Recall: the solution

More information

Chapter 6. Second order differential equations

Chapter 6. Second order differential equations Chapter 6. Second order differential equations A second order differential equation is of the form y = f(t, y, y ) where y = y(t). We shall often think of t as parametrizing time, y position. In this case

More information

Notes on Green s Theorem Northwestern, Spring 2013

Notes on Green s Theorem Northwestern, Spring 2013 Notes on Green s Theorem Northwestern, Spring 2013 The purpose of these notes is to outline some interesting uses of Green s Theorem in situations where it doesn t seem like Green s Theorem should be applicable.

More information

Modeling and Experimentation: Compound Pendulum

Modeling and Experimentation: Compound Pendulum Modeling and Experimentation: Compound Pendulum Prof. R.G. Longoria Department of Mechanical Engineering The University of Texas at Austin Fall 2014 Overview This lab focuses on developing a mathematical

More information

Dylan Zwick. Fall Ax=b. EAx=Eb. UxrrrEb

Dylan Zwick. Fall Ax=b. EAx=Eb. UxrrrEb Math 2270 - Lecture 0: LU Factorization Dylan Zwick Fall 202 This lecture covers section 2.6 of the textbook. The Matrices L and U In elimination what we do is we take a system of equations and convert

More information

Physics 351 Wednesday, January 10, 2018

Physics 351 Wednesday, January 10, 2018 Physics 351 Wednesday, January 10, 2018 Chapers 1 5 mostly review freshman physics, so we ll go through them very quickly in the first few days of class. Read Chapters 1+2 for Friday. Read Chapter 3 (momentum

More information

Control Systems I. Lecture 2: Modeling and Linearization. Suggested Readings: Åström & Murray Ch Jacopo Tani

Control Systems I. Lecture 2: Modeling and Linearization. Suggested Readings: Åström & Murray Ch Jacopo Tani Control Systems I Lecture 2: Modeling and Linearization Suggested Readings: Åström & Murray Ch. 2-3 Jacopo Tani Institute for Dynamic Systems and Control D-MAVT ETH Zürich September 28, 2018 J. Tani, E.

More information

Laplace Transform Part 1: Introduction (I&N Chap 13)

Laplace Transform Part 1: Introduction (I&N Chap 13) Laplace Transform Part 1: Introduction (I&N Chap 13) Definition of the L.T. L.T. of Singularity Functions L.T. Pairs Properties of the L.T. Inverse L.T. Convolution IVT(initial value theorem) & FVT (final

More information

EECE 301 Signals & Systems

EECE 301 Signals & Systems EECE 30 Signals & Systems Prof. Mark Fowler Note Set #22 D-T Systems: DT Systems & Difference Equations / D-T System Models So far we ve seen how to use the FT to analyze circuits Use phasors and standard

More information

Work sheet / Things to know. Chapter 3

Work sheet / Things to know. Chapter 3 MATH 251 Work sheet / Things to know 1. Second order linear differential equation Standard form: Chapter 3 What makes it homogeneous? We will, for the most part, work with equations with constant coefficients

More information

Chapter 4: Techniques of Circuit Analysis

Chapter 4: Techniques of Circuit Analysis Chapter 4: Techniques of Circuit Analysis This chapter gies us many useful tools for soling and simplifying circuits. We saw a few simple tools in the last chapter (reduction of circuits ia series and

More information

4/27 Friday. I have all the old homework if you need to collect them.

4/27 Friday. I have all the old homework if you need to collect them. 4/27 Friday Last HW: do not need to turn it. Solution will be posted on the web. I have all the old homework if you need to collect them. Final exam: 7-9pm, Monday, 4/30 at Lambert Fieldhouse F101 Calculator

More information

Chapter 13 Lecture. Essential University Physics Richard Wolfson 2 nd Edition. Oscillatory Motion Pearson Education, Inc.

Chapter 13 Lecture. Essential University Physics Richard Wolfson 2 nd Edition. Oscillatory Motion Pearson Education, Inc. Chapter 13 Lecture Essential University Physics Richard Wolfson nd Edition Oscillatory Motion Slide 13-1 In this lecture you ll learn To describe the conditions under which oscillatory motion occurs To

More information

4.4 Using partial fractions

4.4 Using partial fractions CHAPTER 4. INTEGRATION 43 Eample 4.9. Compute ln d. (Classic A-Level question!) ln d ln d ln d (ln ) + C. Eample 4.0. Find I sin d. I sin d sin p d p sin. 4.4 Using partial fractions Sometimes we want

More information

Designing Information Devices and Systems I Spring 2018 Lecture Notes Note 11

Designing Information Devices and Systems I Spring 2018 Lecture Notes Note 11 EECS 16A Designing Information Devices and Systems I Spring 2018 Lecture Notes Note 11 11.1 Context Our ultimate goal is to design systems that solve people s problems. To do so, it s critical to understand

More information

Designing Information Devices and Systems I Fall 2018 Lecture Notes Note Introduction to Linear Algebra the EECS Way

Designing Information Devices and Systems I Fall 2018 Lecture Notes Note Introduction to Linear Algebra the EECS Way EECS 16A Designing Information Devices and Systems I Fall 018 Lecture Notes Note 1 1.1 Introduction to Linear Algebra the EECS Way In this note, we will teach the basics of linear algebra and relate it

More information

Resonant MEMS, Eigenvalues, and Numerical Pondering

Resonant MEMS, Eigenvalues, and Numerical Pondering Resonant MEMS, Eigenvalues, and Numerical Pondering David Bindel UC Berkeley, CS Division Resonant MEMS, Eigenvalues,and Numerical Pondering p.1/27 Introduction I always pass on good advice. It is the

More information

Designing Information Devices and Systems II Spring 2016 Anant Sahai and Michel Maharbiz Midterm 2

Designing Information Devices and Systems II Spring 2016 Anant Sahai and Michel Maharbiz Midterm 2 EECS 16B Designing Information Devices and Systems II Spring 2016 Anant Sahai and Michel Maharbiz Midterm 2 Exam location: 145 Dwinelle (SIDs ending in 1 and 5) PRINT your student ID: PRINT AND SIGN your

More information

EE C245 ME C218 Introduction to MEMS Design Fall 2007

EE C245 ME C218 Introduction to MEMS Design Fall 2007 EE C245 ME C218 Introduction to MEMS Design Fall 2007 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley Berkeley, CA 94720 Lecture 15: Beam

More information

ECE 340 Lecture 6 : Intrinsic and Extrinsic Material I Class Outline:

ECE 340 Lecture 6 : Intrinsic and Extrinsic Material I Class Outline: ECE 340 Lecture 6 : Intrinsic and Extrinsic Material I Class Outline: Effective Mass Intrinsic Material Extrinsic Material Things you should know when you leave Key Questions What is the physical meaning

More information

Math 416, Spring 2010 Gram-Schmidt, the QR-factorization, Orthogonal Matrices March 4, 2010 GRAM-SCHMIDT, THE QR-FACTORIZATION, ORTHOGONAL MATRICES

Math 416, Spring 2010 Gram-Schmidt, the QR-factorization, Orthogonal Matrices March 4, 2010 GRAM-SCHMIDT, THE QR-FACTORIZATION, ORTHOGONAL MATRICES Math 46, Spring 00 Gram-Schmidt, the QR-factorization, Orthogonal Matrices March 4, 00 GRAM-SCHMIDT, THE QR-FACTORIZATION, ORTHOGONAL MATRICES Recap Yesterday we talked about several new, important concepts

More information

R. W. Erickson. Department of Electrical, Computer, and Energy Engineering University of Colorado, Boulder

R. W. Erickson. Department of Electrical, Computer, and Energy Engineering University of Colorado, Boulder . W. Erickson Department of Electrical, Computer, and Energy Engineering University of Colorado, Boulder 8.1.7. The low-q approximation Given a second-order denominator polynomial, of the form G(s)= 1

More information

Engineering Mechanics Prof. U. S. Dixit Department of Mechanical Engineering Indian Institute of Technology, Guwahati Introduction to vibration

Engineering Mechanics Prof. U. S. Dixit Department of Mechanical Engineering Indian Institute of Technology, Guwahati Introduction to vibration Engineering Mechanics Prof. U. S. Dixit Department of Mechanical Engineering Indian Institute of Technology, Guwahati Introduction to vibration Module 15 Lecture 38 Vibration of Rigid Bodies Part-1 Today,

More information

Predicting the future with Newton s Second Law

Predicting the future with Newton s Second Law Predicting the future with Newton s Second Law To represent the motion of an object (ignoring rotations for now), we need three functions x(t), y(t), and z(t), which describe the spatial coordinates of

More information

EE123 Digital Signal Processing

EE123 Digital Signal Processing Announcements EE Digital Signal Processing otes posted HW due Friday SDR give away Today! Read Ch 9 $$$ give me your names Lecture based on slides by JM Kahn M Lustig, EECS UC Berkeley M Lustig, EECS UC

More information

Networks and Systems Prof. V. G. K. Murti Department of Electrical Engineering Indian Institute of Technology, Madras

Networks and Systems Prof. V. G. K. Murti Department of Electrical Engineering Indian Institute of Technology, Madras Networks and Systems Prof. V. G. K. Murti Department of Electrical Engineering Indian Institute of Technology, Madras Lecture - 34 Network Theorems (1) Superposition Theorem Substitution Theorem The next

More information

Review: control, feedback, etc. Today s topic: state-space models of systems; linearization

Review: control, feedback, etc. Today s topic: state-space models of systems; linearization Plan of the Lecture Review: control, feedback, etc Today s topic: state-space models of systems; linearization Goal: a general framework that encompasses all examples of interest Once we have mastered

More information

TAYLOR POLYNOMIALS DARYL DEFORD

TAYLOR POLYNOMIALS DARYL DEFORD TAYLOR POLYNOMIALS DARYL DEFORD 1. Introduction We have seen in class that Taylor polynomials provide us with a valuable tool for approximating many different types of functions. However, in order to really

More information

Vibrations and waves: revision. Martin Dove Queen Mary University of London

Vibrations and waves: revision. Martin Dove Queen Mary University of London Vibrations and waves: revision Martin Dove Queen Mary University of London Form of the examination Part A = 50%, 10 short questions, no options Part B = 50%, Answer questions from a choice of 4 Total exam

More information

AC analysis. EE 201 AC analysis 1

AC analysis. EE 201 AC analysis 1 AC analysis Now we turn to circuits with sinusoidal sources. Earlier, we had a brief look at sinusoids, but now we will add in capacitors and inductors, making the story much more interesting. What are

More information

Modeling and Experimentation: Mass-Spring-Damper System Dynamics

Modeling and Experimentation: Mass-Spring-Damper System Dynamics Modeling and Experimentation: Mass-Spring-Damper System Dynamics Prof. R.G. Longoria Department of Mechanical Engineering The University of Texas at Austin July 20, 2014 Overview 1 This lab is meant to

More information

Phys 102 Lecture 12 Currents & magnetic fields

Phys 102 Lecture 12 Currents & magnetic fields Phys 102 Lecture 12 Currents & magnetic fields 1 Today we will... Learn how magnetic fields are created by currents Use specific examples Long straight wire Current loop Solenoid Apply these concepts Electromagnets

More information

3: Gauss s Law July 7, 2008

3: Gauss s Law July 7, 2008 3: Gauss s Law July 7, 2008 3.1 Electric Flux In order to understand electric flux, it is helpful to take field lines very seriously. Think of them almost as real things that stream out from positive charges

More information

Table of contents. d 2 y dx 2, As the equation is linear, these quantities can only be involved in the following manner:

Table of contents. d 2 y dx 2, As the equation is linear, these quantities can only be involved in the following manner: M ath 0 1 E S 1 W inter 0 1 0 Last Updated: January, 01 0 Solving Second Order Linear ODEs Disclaimer: This lecture note tries to provide an alternative approach to the material in Sections 4. 4. 7 and

More information

Main topics for the First Midterm Exam

Main topics for the First Midterm Exam Main topics for the First Midterm Exam The final will cover Sections.-.0, 2.-2.5, and 4.. This is roughly the material from first three homeworks and three quizzes, in addition to the lecture on Monday,

More information

Simon Fraser University School of Engineering Science ENSC Linear Systems Spring Instructor Jim Cavers ASB

Simon Fraser University School of Engineering Science ENSC Linear Systems Spring Instructor Jim Cavers ASB Simon Fraser University School of Engineering Science ENSC 380-3 Linear Systems Spring 2000 This course covers the modeling and analysis of continuous and discrete signals and systems using linear techniques.

More information

Partial Fractions. Combining fractions over a common denominator is a familiar operation from algebra: 2 x 3 + 3

Partial Fractions. Combining fractions over a common denominator is a familiar operation from algebra: 2 x 3 + 3 Partial Fractions Combining fractions over a common denominator is a familiar operation from algebra: x 3 + 3 x + x + 3x 7 () x 3 3x + x 3 From the standpoint of integration, the left side of Equation

More information

Differential Equations and Linear Algebra Exercises. Department of Mathematics, Heriot-Watt University, Edinburgh EH14 4AS

Differential Equations and Linear Algebra Exercises. Department of Mathematics, Heriot-Watt University, Edinburgh EH14 4AS Differential Equations and Linear Algebra Exercises Department of Mathematics, Heriot-Watt University, Edinburgh EH14 4AS CHAPTER 1 Linear second order ODEs Exercises 1.1. (*) 1 The following differential

More information

Complex number review

Complex number review Midterm Review Problems Physics 8B Fall 009 Complex number review AC circuits are usually handled with one of two techniques: phasors and complex numbers. We ll be using the complex number approach, so

More information

Slide Set 3. for ENEL 353 Fall Steve Norman, PhD, PEng. Electrical & Computer Engineering Schulich School of Engineering University of Calgary

Slide Set 3. for ENEL 353 Fall Steve Norman, PhD, PEng. Electrical & Computer Engineering Schulich School of Engineering University of Calgary Slide Set 3 for ENEL 353 Fall 2016 Steve Norman, PhD, PEng Electrical & Computer Engineering Schulich School of Engineering University of Calgary Fall Term, 2016 SN s ENEL 353 Fall 2016 Slide Set 3 slide

More information

CS 343: Artificial Intelligence

CS 343: Artificial Intelligence CS 343: Artificial Intelligence Bayes Nets Prof. Scott Niekum The University of Texas at Austin [These slides based on those of Dan Klein and Pieter Abbeel for CS188 Intro to AI at UC Berkeley. All CS188

More information

MITOCW watch?v=b1ekhyc9tto

MITOCW watch?v=b1ekhyc9tto MITOCW watch?v=b1ekhyc9tto The following content is provided under a Creative Commons license. Your support will help MIT OpenCourseWare continue to offer high-quality quality educational resources for

More information

Lecture 6: Differential Equations Describing Vibrations

Lecture 6: Differential Equations Describing Vibrations Lecture 6: Differential Equations Describing Vibrations In Chapter 3 of the Benson textbook, we will look at how various types of musical instruments produce sound, focusing on issues like how the construction

More information

Chapter 15. Probability Rules! Copyright 2012, 2008, 2005 Pearson Education, Inc.

Chapter 15. Probability Rules! Copyright 2012, 2008, 2005 Pearson Education, Inc. Chapter 15 Probability Rules! Copyright 2012, 2008, 2005 Pearson Education, Inc. The General Addition Rule When two events A and B are disjoint, we can use the addition rule for disjoint events from Chapter

More information

MA1131 Lecture 15 (2 & 3/12/2010) 77. dx dx v + udv dx. (uv) = v du dx dx + dx dx dx

MA1131 Lecture 15 (2 & 3/12/2010) 77. dx dx v + udv dx. (uv) = v du dx dx + dx dx dx MA3 Lecture 5 ( & 3//00) 77 0.3. Integration by parts If we integrate both sides of the proct rule we get d (uv) dx = dx or uv = d (uv) = dx dx v + udv dx v dx dx + v dx dx + u dv dx dx u dv dx dx This

More information

Dynamics of Ocean Structures Prof. Dr. Srinivasan Chandrasekaran Department of Ocean Engineering Indian Institute of Technology, Madras

Dynamics of Ocean Structures Prof. Dr. Srinivasan Chandrasekaran Department of Ocean Engineering Indian Institute of Technology, Madras Dynamics of Ocean Structures Prof. Dr. Srinivasan Chandrasekaran Department of Ocean Engineering Indian Institute of Technology, Madras Module - 01 Lecture - 09 Characteristics of Single Degree - of -

More information

Designing Information Devices and Systems II Spring 2017 Murat Arcak and Michel Maharbiz Homework 9

Designing Information Devices and Systems II Spring 2017 Murat Arcak and Michel Maharbiz Homework 9 EECS 16B Designing Information Devices and Systems II Spring 2017 Murat Arcak and Michel Maharbiz Homework 9 This homework is due April 5, 2017, at 17:00. 1. Midterm 2 - Question 1 Redo the midterm! 2.

More information

Physics 225 Relativity and Math Applications. Fall Unit 7 The 4-vectors of Dynamics

Physics 225 Relativity and Math Applications. Fall Unit 7 The 4-vectors of Dynamics Physics 225 Relativity and Math Applications Fall 2011 Unit 7 The 4-vectors of Dynamics N.C.R. Makins University of Illinois at Urbana-Champaign 2010 Physics 225 7.2 7.2 Physics 225 7.3 Unit 7: The 4-vectors

More information

EKF, UKF. Pieter Abbeel UC Berkeley EECS. Many slides adapted from Thrun, Burgard and Fox, Probabilistic Robotics

EKF, UKF. Pieter Abbeel UC Berkeley EECS. Many slides adapted from Thrun, Burgard and Fox, Probabilistic Robotics EKF, UKF Pieter Abbeel UC Berkeley EECS Many slides adapted from Thrun, Burgard and Fox, Probabilistic Robotics Kalman Filter Kalman Filter = special case of a Bayes filter with dynamics model and sensory

More information

Lecture 12. Upcoming labs: Final Exam on 12/21/2015 (Monday)10:30-12:30

Lecture 12. Upcoming labs: Final Exam on 12/21/2015 (Monday)10:30-12:30 289 Upcoming labs: Lecture 12 Lab 20: Internal model control (finish up) Lab 22: Force or Torque control experiments [Integrative] (2-3 sessions) Final Exam on 12/21/2015 (Monday)10:30-12:30 Today: Recap

More information

EKF, UKF. Pieter Abbeel UC Berkeley EECS. Many slides adapted from Thrun, Burgard and Fox, Probabilistic Robotics

EKF, UKF. Pieter Abbeel UC Berkeley EECS. Many slides adapted from Thrun, Burgard and Fox, Probabilistic Robotics EKF, UKF Pieter Abbeel UC Berkeley EECS Many slides adapted from Thrun, Burgard and Fox, Probabilistic Robotics Kalman Filter Kalman Filter = special case of a Bayes filter with dynamics model and sensory

More information

Dynamics and Time Integration. Computer Graphics CMU /15-662, Fall 2016

Dynamics and Time Integration. Computer Graphics CMU /15-662, Fall 2016 Dynamics and Time Integration Computer Graphics CMU 15-462/15-662, Fall 2016 Last Quiz: IK (and demo) Last few classes Keyframing and motion capture - Q: what can one NOT do with these techniques? The

More information

Mathematical Induction. EECS 203: Discrete Mathematics Lecture 11 Spring

Mathematical Induction. EECS 203: Discrete Mathematics Lecture 11 Spring Mathematical Induction EECS 203: Discrete Mathematics Lecture 11 Spring 2016 1 Climbing the Ladder We want to show that n 1 P(n) is true. Think of the positive integers as a ladder. 1, 2, 3, 4, 5, 6,...

More information

CS 188: Artificial Intelligence Spring Announcements

CS 188: Artificial Intelligence Spring Announcements CS 188: Artificial Intelligence Spring 2011 Lecture 14: Bayes Nets II Independence 3/9/2011 Pieter Abbeel UC Berkeley Many slides over the course adapted from Dan Klein, Stuart Russell, Andrew Moore Announcements

More information

LHSE Presents. Temperature

LHSE Presents. Temperature LHSE Presents Introduction to Chemistry Temperature Conversions Previous lecture Math for Chemistry Temperature Heat Temperature 3 Temperature scales (F o, C o, K) Equations for converting between scale

More information

Math 266: Phase Plane Portrait

Math 266: Phase Plane Portrait Math 266: Phase Plane Portrait Long Jin Purdue, Spring 2018 Review: Phase line for an autonomous equation For a single autonomous equation y = f (y) we used a phase line to illustrate the equilibrium solutions

More information

The Harmonic Oscillator

The Harmonic Oscillator The Harmonic Oscillator Math 4: Ordinary Differential Equations Chris Meyer May 3, 008 Introduction The harmonic oscillator is a common model used in physics because of the wide range of problems it can

More information

Parallel VLSI CAD Algorithms. Lecture 1 Introduction Zhuo Feng

Parallel VLSI CAD Algorithms. Lecture 1 Introduction Zhuo Feng Parallel VLSI CAD Algorithms Lecture 1 Introduction Zhuo Feng 1.1 Prof. Zhuo Feng Office: EERC 513 Phone: 487-3116 Email: zhuofeng@mtu.edu Class Website http://www.ece.mtu.edu/~zhuofeng/ee5900spring2012.html

More information

Propositional Logic: Semantics and an Example

Propositional Logic: Semantics and an Example Propositional Logic: Semantics and an Example CPSC 322 Logic 2 Textbook 5.2 Propositional Logic: Semantics and an Example CPSC 322 Logic 2, Slide 1 Lecture Overview 1 Recap: Syntax 2 Propositional Definite

More information

In this lecture, we will consider how to analyse an electrical circuit by applying KVL and KCL. As a result, we can predict the voltages and currents

In this lecture, we will consider how to analyse an electrical circuit by applying KVL and KCL. As a result, we can predict the voltages and currents In this lecture, we will consider how to analyse an electrical circuit by applying KVL and KCL. As a result, we can predict the voltages and currents around an electrical circuit. This is a short lecture,

More information

Lecture 13: H(s) Poles-Zeros & BIBO Stability. (a) What are poles and zeros? Answer: HS math and calculus review.

Lecture 13: H(s) Poles-Zeros & BIBO Stability. (a) What are poles and zeros? Answer: HS math and calculus review. 1. Introduction Lecture 13: H(s) Poles-Zeros & BIBO Stability (a) What are poles and zeros? Answer: HS math and calculus review. (b) What are nice inputs? Answer: nice inputs are bounded inputs; if you

More information

Advanced Structural Analysis Prof. Devdas Menon Department of Civil Engineering Indian Institute of Technology, Madras

Advanced Structural Analysis Prof. Devdas Menon Department of Civil Engineering Indian Institute of Technology, Madras Advanced Structural Analysis Prof. Devdas Menon Department of Civil Engineering Indian Institute of Technology, Madras Module No. # 5.4 Lecture No. # 30 Matrix Analysis of Beams and Grids (Refer Slide

More information