Lecture 131 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.

Slides:



Advertisements
Similar presentations
LAPLACE TRANSFORMS.
Advertisements

Laplace Transform (1).
1 1 Eng. Mohamed Eltaher Eng.Ahmed Ibrahim. 2 2 Exercise (1)  Solve the following set of equations using MATLAB x 1 + 2x 2 + 3x 3 + 5x 4 = 21 – 2x 1.
EEE 302 Electrical Networks II
Lecture 111 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
Lecture 161 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
Lecture 141 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
Lecture 11 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
Lecture 31 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
Lecture 21 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
Lecture 241 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
Laplace Transforms Important analytical method for solving linear ordinary differential equations. - Application to nonlinear ODEs? Must linearize first.
Lecture 121 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
Laplace Transformations
Lecture 81 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
Lecture 231 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
EEE340Lecture : Electromagnetic Boundary Conditions E 1t =E 2t, always. B 1n =B 2n, always. For PEC, the conductor side H 2 =0, E 2 =0. (7.66b)
Automatic Control Laplace Transformation Dr. Aly Mousaad Aly Department of Mechanical Engineering Faculty of Engineering, Alexandria University.
Lecture 61 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
Bogazici University Dept. Of ME. Laplace Transforms Very useful in the analysis and design of LTI systems. Operations of differentiation and integration.
Introduction to Differential Equations
Laplace Transform Applications of the Laplace transform
FOURIER TRANSFORMS.
The Laplace Transform M. J. Roberts - All Rights Reserved. Edited by Dr. Robert Akl 1.
Lecture 181 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
Lecture 211 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
Lecture 151 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
Chapter 3 1 Laplace Transforms 1. Standard notation in dynamics and control (shorthand notation) 2. Converts mathematics to algebraic operations 3. Advantageous.
Lecture 171 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001.
DEPARTMENT OF MATHEMATI CS [ YEAR OF ESTABLISHMENT – 1997 ] DEPARTMENT OF MATHEMATICS, CVRCE.
Hany Ferdinando Dept. of Electrical Eng. Petra Christian University
Types of systems in the Laplace domain. System order Most systems that we will be dealing with can be characterised as first or second order systems.
ISAT 412 -Dynamic Control of Energy Systems (Fall 2005)
EE313 Linear Systems and Signals Fall 2010 Initial conversion of content to PowerPoint by Dr. Wade C. Schwartzkopf Prof. Brian L. Evans Dept. of Electrical.
Topic-laplace transformation Presented by Harsh PATEL
ORDINARY DIFFERENTIAL EQUATION (ODE) LAPLACE TRANSFORM.
Lecture 12 - Natural Response of Parallel RLC Circuits
SE 207: Modeling and Simulation Introduction to Laplace Transform
Chapter 5: Fourier Transform.
Mathematical Models and Block Diagrams of Systems Regulation And Control Engineering.
Lecture 4: Electrical Circuits
ABE425 Engineering Measurement Systems ABE425 Engineering Measurement Systems Laplace Transform Dr. Tony E. Grift Dept. of Agricultural & Biological Engineering.
Instrumentation (AMME2700) 1 Instrumentation Dr. Xiaofeng Wu.
Alexander-Sadiku Fundamentals of Electric Circuits
case study on Laplace transform
University of Warwick: AMR Summer School 4 th -6 th July, 2016 Structural Identifiability Analysis Dr Mike Chappell, School of Engineering, University.
LAPLACE TRANSFORMS.
Lec 4. the inverse Laplace Transform
DIFFERENTIAL EQUATIONS
The Laplace transform a quick review!
Chapter 6 Laplace Transform
Chap2. Modeling in the Frequency Domain
Engineering Analysis I
EKT 119 ELECTRIC CIRCUIT II
Complex Frequency and Laplace Transform
Lecture 3: Solving Diff Eqs with the Laplace Transform
Chapter 15 Introduction to the Laplace Transform
Mechatronics Engineering
Digital Control Systems Waseem Gulsher
B.Sc. II Year Mr. Shrimangale G.W.
Fundamentals of Electric Circuits Chapter 15
EKT 119 ELECTRIC CIRCUIT II
Introduction The purpose of Laplace transformation is to solve different differential equations. There are a number of methods to solve homogeneous and.
Chapter 9 – Sinusoids and Phasors
Chapter 2. Mathematical Foundation
RAYAT SHIKSHAN SANSTHA’S S.M.JOSHI COLLEGE HADAPSAR, PUNE
Chapter 9 – Sinusoids and Phasors
Laplace Transforms Important analytical method for solving linear ordinary differential equations. - Application to nonlinear ODEs? Must linearize first.
Lectures State-Space Analysis of LTIC
Laplace Transforms Important analytical method for solving linear ordinary differential equations. - Application to nonlinear ODEs? Must linearize first.
Presentation transcript:

Lecture 131 EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001

Lecture 132 Laplace Transform Applications of the Laplace transform –solve differential equations (both ordinary and partial) –application to RLC circuit analysis Laplace transform converts differential equations in the time domain to algebraic equations in the frequency domain, thus 3 important processes: (1) transformation from the time to frequency domain (2) manipulate the algebraic equations to form a solution (3) inverse transformation from the frequency to time domain

Lecture 133 Definition of Laplace Transform Definition of the unilateral (one-sided) Laplace transform where s=  +j  is the complex frequency, and f(t)=0 for t<0 The inverse Laplace transform requires a course in complex variables analysis (e.g., MAT 461)

Lecture 134 Singularity Functions Singularity functions are either not finite or don't have finite derivatives everywhere The two singularity functions of interest here are (1) unit step function, u(t) and its construct: the gate function (2) delta or unit impulse function,  (t) and its construct: the sampling function

Lecture 135 Unit Step Function, u(t) The unit step function, u(t) –Mathematical definition –Graphical illustration 1 t 0 u(t)u(t)

Lecture 136 Extensions of the Unit Step Function A more general unit step function is u(t-a) The gate function can be constructed from u(t) –a rectangular pulse that starts at t=  and ends at t=  +T –like an on/off switch 1 t 0a 1 t 0  +T u(t-  ) - u(t-  -T)

Lecture 137 Delta or Unit Impulse Function,  (t) The delta or unit impulse function,  (t) –Mathematical definition (non-pure version) –Graphical illustration 1 t 0 (t)(t) t0t0

Lecture 138 Extensions of the Delta Function An important property of the unit impulse function is its sampling property –Mathematical definition (non-pure version) f(t)f(t) t 0t0t0 f(t)  (t-t 0 )

Lecture 139 Transform Pairs The Laplace transforms pairs in Table 13.1 are important, and the most important are repeated here.

Lecture 1310 Class Examples Extension Exercise E13.1 Extension Exercise E13.2

Lecture 1311 Laplace Transform Properties

Lecture 1312 Class Examples Extension Exercise E13.3 Extension Exercise E13.4 Extension Exercise E13.5 Extension Exercise E13.6 Extension Exercise E13.8