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    Mathematics 2P0MATH29641

    2010-11

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    Who ?

    2nd Year students, School of ElectricalEngineering

    Question: who in the room studies:

    1. Electrical & Electronic Engineering?

    2. Electronic Systems Engineering?

    3. Mechatronic Engineering?

    4. Communication Systems Engineering?5. Computer Systems Engineering?

    6. Other?

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    When and Where ?

    Monday 4 pm (lectures, in Renold D7)

    Wednesday 12 noon (tutorials, week 2onwards, alternating with 2Q1, in Renold

    F14)

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    What ?

    Laplace Transforms (4 lectures) :- Definition,

    Transforms of Simple Functions, Inverse

    Transforms. Transforms of first and second

    derivatives. Solution of Ordinary differentialequations by Laplace Transforms.

    Applications to RLC Circuits.

    Vector Calculus (7 lectures) :- Definition of

    div, grad and curl. Identities, examples,

    applications.

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    Contact: Dr Oliver Dorn

    Alan Turing, room 1.110

    Tel 0161 306 3217 [email protected]

    Regular office hours: Wed 15:30-16:30, AT1.110

    mailto:[email protected]:[email protected]
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    Web-pages

    www.maths.manchester.ac.uk/service/

    www.maths.manchester.ac.uk/service/MATH

    Also can be entered through Blackboard.

    http://www.maths.manchester.ac.uk/service/http://www.maths.manchester.ac.uk/service/MATH29641/http://www.maths.manchester.ac.uk/service/MATH29641/http://www.maths.manchester.ac.uk/service/
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    Are there any Questions

    before we start ?

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    1. Laplace Transforms

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    Laplace Transforms

    Four Lectures, Monday 4 pm, weeks 1-4

    Tutorials on Wednesdays, 12 noon, weeks 2 and 4

    Where to read more details?

    E Kreyszig, Advanced Engineering Mathematics,

    Wiley : Sect 5 (Laplace Transforms),

    KA Stroud, Engineering Mathematics, Palgrave :Programme 26 (Laplace Transforms)

    HELM Resources, Section 20

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    1.0 Background: Integral transforms

    =2

    1

    )(),()( tt

    dttfstKsTf

    Integral transforms play an important role in Engineering

    Mathematics. They have the general form:

    They transform functions of a specific type into functions of

    another type. Many Engineering problems can be solvedeasier by first applying suitable integral transforms, then

    solving the problem in the transformed form, and then

    transform the result back to the original problem.

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    Original problem

    Problem in

    transformed form

    Solution of original

    problem

    Solution of transformed

    problem

    Integral

    transform

    Difficult to solve

    Backward

    integral

    transform

    Easier to solve

    1.0. Background: Integral transforms

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    2/),(istestK =

    stestK =),(

    Examples for important integral transforms are:

    Fourier Transform

    Laplace Transform

    Hilbert Transform

    (and many more)

    tsstK

    = 11),(

    1.0. Background: Integral transforms

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    We will discuss in this module only the

    Laplace Transform, which has important

    applications in Electrical Engineering (the

    others have as well, but you will discuss them,if necessary, when their applications arise).

    We will in particular focus on its application

    to solving Ordinary Differential Equations

    (ODEs).

    1.0. Background: Integral transforms

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    Example: In the design of RLC circuits, certain

    ODEs appear which can be solved by the

    Laplace Transform technique. We will discuss some examples later.

    1.0. Background: Integral transforms

    ?

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    Original problem:

    solve ODE

    ODE in transformed

    form = ALGEBRAIC

    PROBLEM

    Solution of ODE

    Solution of ALGEBRAIC

    PROBLEM

    Laplace

    transform

    Solve ODE directly:

    often difficult !

    Inverse Laplace

    transform

    Solve this easier

    algebraic problem

    1.0. Background: Integral transforms

    So, the goal is to establish the following diagram:

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    1.1 Introduction to Laplace

    Transforms

    Pierre-Simon

    Laplace

    1749 1827

    French

    mathematician.

    1 1 I t d ti t L l T f

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    For any function f(t), the Laplace

    Transform is defined as

    1.1 Introduction to Laplace Transforms

    ( )0

    ( )s tf t e f t dt =

    So, how exactly is the Laplace Transformdefined?

    1 1 I t d ti t L l T f

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    As this is a definite integral between limits on t,

    the final result will NOT depend on t.

    It will, however depend on s.

    For this reason, [f(t)] is often written as

    1.1 Introduction to Laplace Transforms

    ( ) 0 ( )s t

    f t e f t dt

    =

    ( )f s

    1 1 I t d ti t L l T f

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    Example 1.1.1

    If f(t) = t, find the Laplace Transform

    ( ) [ ] ( )f t t f s= =

    1.1 Introduction to Laplace Transforms

    Well, in this case, this appears to be a simple

    integration. Do you remember how to do it ?

    =0

    ][ dttet st

    1 1 I t d ti t L l T f

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    ( ) [ ]a t

    f t e=

    Example 1.1.2

    If , find the Laplace Transform

    Hence, for example with , find

    1.1 Introduction to Laplace Transforms

    ( ) a tf t e=

    =0

    44 ][ dteee sttt

    4=a

    1 1 Introduction to Laplace Transforms

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    Laplace Transforms : An Illustration

    Consider the function f(t) = t e-st

    fordifferent values of s (s = 1, 2, 5).

    1.1 Introduction to Laplace Transforms

    1 1 Introduction to Laplace Transforms

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    is given by the area under the curve for the

    appropriate value of s.

    1.1 Introduction to Laplace Transforms

    [ ] 0s t

    t t e dt

    =

    1 1 Introduction to Laplace Transforms

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    s = 1 : Largish area under curve

    1.1 Introduction to Laplace Transforms

    1 1 Introduction to Laplace Transforms

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    s = 2 : Smaller area under curve

    1.1 Introduction to Laplace Transforms

    1 1 Introduction to Laplace Transforms

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    s = 5 : Even smaller area under curve

    1.1 Introduction to Laplace Transforms

    1 1 Introduction to Laplace Transforms

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    The Laplace Transform (area under curve)

    depends on s. In fact, it is equal to 1/s2

    1.1 Introduction to Laplace Transforms

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    1.2 Laplace Transforms by Table

    1 2 Laplace Transforms by Table

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    The direct integration approach of section1.1 will give the Laplace Transform of

    many functions. Once carried out, these

    Laplace Transforms can be written in a

    table.

    Try to verify a few of them yourself (we will

    also try some in the Tutorials)!

    More:

    Maths formula Tables (page 13),

    HELM 20.2 (page 5)

    1.2 Laplace Transforms by Table

    1 2 Laplace Transforms by Table

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    1.2 Laplace Transforms by Table

    1 2 Laplace Transforms by Table

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    1.2 Laplace Transforms by Table

    1 2 Laplace Transforms by Table

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    1.2 Laplace Transforms by Table

    1.2 Laplace Transforms by Table

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    1.2 Laplace Transforms by Table

    1.2 Laplace Transforms by Table

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    1.2 Laplace Transforms by Table

    1.2 Laplace Transforms by Table

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    Example 1.2.1

    Use the tables to find

    i)

    ii)

    4t

    1.2 Laplace Transforms by Table

    [ ]sin5t

    1.2 Laplace Transforms by Table

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    Note that the Laplace Transform is a linear

    process i.e.

    and

    [ ] [ ] [ ]( ) ( ) ( ) ( )f t g t f t g t+ = +

    p y

    [ ] [ ]( ) ( )k f t k f t =

    Do we always have to calculate the Laplace

    transform of a function by integration?

    1.2 Laplace Transforms by Table

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    More generally

    These linearity properties can be used in the sameway as for derivatives and integrals.

    They help us to calculate Laplace transforms forsome of the more complicated expressions by justusing the elementary components which we find inthe standard Laplace transform tables and combiningthem linearly.

    p y

    [ ] [ ] [ ]1 2 1 2( ) ( ) ( ) ( )k f t k g t k f t k g t + = +

    1.2 Laplace Transforms by Table

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    Example 1.2.2

    Use the tables and linearity properties to

    find

    p y

    5 24 sin 3 7t te t e +

    Basic

    Trig/Hyp

    Polytrig

    Heavy

    Exptrig

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    Next Monday:

    Inverse Laplace Transform

    The Laplace Transform of

    Derivatives and Integrals

    Convolutions and the Laplace

    Transform