Engineering Mathematics Class #11 Laplace Transforms (Part1)

Slides:



Advertisements
Similar presentations
Ch 6.4: Differential Equations with Discontinuous Forcing Functions
Advertisements

Lecture 7: Basis Functions & Fourier Series
Integrals 5. Integration by Parts Integration by Parts Every differentiation rule has a corresponding integration rule. For instance, the Substitution.
Engineering Mathematics Class #15 Fourier Series, Integrals, and Transforms (Part 3) Sheng-Fang Huang.
Copyright © Cengage Learning. All rights reserved. 6 Inverse Functions.
Lecture 3 Laplace transform
A second order ordinary differential equation has the general form
Ch 5.2: Series Solutions Near an Ordinary Point, Part I
Ch 3.5: Nonhomogeneous Equations; Method of Undetermined Coefficients
Ch 6.3: Step Functions Some of the most interesting elementary applications of the Laplace Transform method occur in the solution of linear equations.
Ch 6.1: Definition of Laplace Transform Many practical engineering problems involve mechanical or electrical systems acted upon by discontinuous or impulsive.
TECHNIQUES OF INTEGRATION
1 Chapter 7 Transcendental Functions Inverse Functions and Their Derivatives.
Ch 6.2: Solution of Initial Value Problems
Automatic Control Laplace Transformation Dr. Aly Mousaad Aly Department of Mechanical Engineering Faculty of Engineering, Alexandria University.
Bogazici University Dept. Of ME. Laplace Transforms Very useful in the analysis and design of LTI systems. Operations of differentiation and integration.
Ch 2.1: Linear Equations; Method of Integrating Factors
Inverse Trig. Functions & Differentiation Section 5.8.
Copyright © 2005 Pearson Education, Inc. Publishing as Pearson Addison-Wesley Chapter 7 Transcendental Functions.
Sheng-Fang Huang. Introduction If r (x) = 0 (that is, r (x) = 0 for all x considered; read “r (x) is identically zero”), then (1) reduces to (2) y"
Laplace Transform BIOE 4200.
Engineering Mathematics Class #11 Part 2 Laplace Transforms (Part2)
ORDINARY DIFFERENTIAL EQUATION (ODE) LAPLACE TRANSFORM.
SECOND-ORDER DIFFERENTIAL EQUATIONS
Copyright © Cengage Learning. All rights reserved. 6 Inverse Functions.
1 On Free Mechanical Vibrations As derived in section 4.1( following Newton’s 2nd law of motion and the Hooke’s law), the D.E. for the mass-spring oscillator.
SE 207: Modeling and Simulation Introduction to Laplace Transform
6.5 Fundamental Matrices and the Exponential of a Matrix Fundamental Matrices Suppose that x 1 (t),..., x n (t) form a fundamental set of solutions for.
Engineering Mathematics Class #12 Laplace Transforms (Part3)
Copyright © Cengage Learning. All rights reserved. 7 Techniques of Integration.
Chapter 2 Laplace Transform 2.1 Introduction The Laplace transform method can be used for solving linear differential equations. Laplace transforms can.
Calculus, 8/E by Howard Anton, Irl Bivens, and Stephen Davis Copyright © 2005 by John Wiley & Sons, Inc. All rights reserved. Chapter Integration.
Sheng-Fang Huang. 1.1 Basic Concepts Modeling A model is very often an equation containing derivatives of an unknown function. Such a model is called.
ME375 Handouts - Fall 2002 MESB 374 System Modeling and Analysis Laplace Transform and Its Applications.
H.Melikyan/12001 Inverse Trigonometric Functions.
Boyce/DiPrima 9 th ed, Ch 6.2: Solution of Initial Value Problems Elementary Differential Equations and Boundary Value Problems, 9 th edition, by William.
Ch 2.1: Linear Equations; Method of Integrating Factors A linear first order ODE has the general form where f is linear in y. Examples include equations.
Math 3120 Differential Equations with Boundary Value Problems
Boundary-Value Problems in Rectangular Coordinates
Sheng-Fang Huang Fourier Series Fourier series are the basic tool for representing periodic functions. A function ƒ(x) is called a periodic function.
Section 4.7 Variation of Parameters. METHOD OF VARIATION OF PARAMETERS For a second-order linear equation in standard form y″ + Py′ + Qy = g(x). 1.Find.
Ch 6.2: Solution of Initial Value Problems The Laplace transform is named for the French mathematician Laplace, who studied this transform in The.
Math for CS Fourier Transforms
Company LOGO Laplace Transform Ch # 5 1. Company LOGO Topics 1. Get to know: Laplace Transform 2. Laplace Theory and Properties 3. Applications 2.
Class 3 Linear System Solution Using the Laplace Transform
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.
歐亞書局 P Chapter 6 Laplace Transforms. 歐亞書局 P Contents  6.1 Laplace Transform. Inverse Transform. Linearity s-Shifting 6.1 Laplace Transform. Inverse Transform.
Second Shifting Theorem
INTEGRATION & TECHNIQUES OF INTEGRATION
Laplace Transforms.
Translation Theorems and Derivatives of a Transform
Fig Solving an IVP by Laplace transforms
EKT 119 ELECTRIC CIRCUIT II
Transcendental Functions
Linear Differential Equations
Chapter Integration By Parts
Automatic Control(E.E- 412) Chapter 1 Laplace Transform Dr. Monji Mohamed Zaidi.
Represented by Dr. Shorouk Ossama
Trigonometric Identities
5.6 The Quadratic Formula and the Discriminant
4.8 The Quadratic Formula and the Discriminant
Mechatronics Engineering
B.Sc. II Year Mr. Shrimangale G.W.
Chapter 3 Section 5.
Chapter 4 THE LAPLACE TRANSFORM.
Ch 6.3: Step Functions Some of the most interesting elementary applications of the Laplace Transform method occur in the solution of linear equations.
Laplace Transforms Lecture-11 Additional chapters of mathematics
Ch 6.3: Step Functions Some of the most interesting elementary applications of the Laplace Transform method occur in the solution of linear equations.
Presentation transcript:

Engineering Mathematics Class #11 Laplace Transforms (Part1) Sheng-Fang Huang

Solving an IVP by Laplace transforms The Laplace transform method is a powerful method for solving linear ODEs and corresponding initial value problems, as well as systems of ODEs arising in engineering.

6.1 Laplace Transform. Inverse Transform. Linearity. s-Shifting ƒ(t) is a function defined for all t ≥ 0. Its Laplace transform, , is denoted by F(s), which is (1) Here we must assume that ƒ(t) is such that the integral exists (that is, has some finite value).

Inverse Transform The given function ƒ(t) in (1) is called the inverse transform of F(s) and is denoted by ; that is, (1*) Note that (1) and (1*) together imply = ƒ, and = F.

Example 1: Laplace Transform Let ƒ(t) = 1 when t ≥ 0. Find F(s). Solution. From (1) we obtain by integration The interval of integration in (1) is infinite. Such an integral is evaluated according to the rule

Example 2 Laplace Transform of the eat Let ƒ(t) = eat when t ≥ 0, where a is a constant. Find Solution.

Linearity of the Laplace Transform THEOREM 1 The Laplace transform is a linear operation; that is, for any functions ƒ(t) and g(t) whose transforms exist and any constants a and b the transform of aƒ(t) + bg(t) exists, and

Example 3 Application of Theorem 1: Hyperbolic Functions Find the transforms of cosh at and sinh at. Solution. Since coshat = 1/2(eat + e-at) and sinhat = 1/2(eat – e-at),

Example 4 Cosine and Sine Derive the formulas Solution:

By substituting Ls into the formula for Lc on the right and then by substituting Lc into the formula for Ls on the right, we obtain Solution by Transforms Using Derivatives. See next section.

Solution by Complex Methods Solution by Complex Methods. In Example 2, if we set a = iω with i = (–1)1/2, we obtain Now by Theorem 1 and eiωt = cos ωt + i sin ωt If we equate the real and imaginary parts of this and the previous equation, the result follows.

Some Functions ƒ(t) and Their Laplace Transforms

s-Shifting: Replacing s by s – a in the Transform First Shifting Theorem, s-Shifting THEOREM 2 If ƒ(t) has the transform F(s) (where s > k for some k), then eatƒ(t) has the transform F(s – a) (where s – a > k). In formulas, or, if we take the inverse on both sides,

Example 5 s-Shifting: Damped Vibrations. Completing the Square From Example 4, For instance, use these formulas to find the inverse of the transform