EEM 3117 Laplace Transformation Dr. Sezai Taskin Department of - - PowerPoint PPT Presentation

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EEM 3117 Laplace Transformation Dr. Sezai Taskin Department of - - PowerPoint PPT Presentation

Automatic Control EEM 3117 Laplace Transformation Dr. Sezai Taskin Department of Electrical&Electronics Engineering Faculty of Engineering, Manisa Celal Bayar University Laplace Transformation The Laplace transform of a function f ( t ),


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Automatic Control EEM 3117

Laplace Transformation

  • Dr. Sezai Taskin

Department of Electrical&Electronics Engineering Faculty of Engineering, Manisa Celal Bayar University

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Laplace Transformation

The Laplace transform of a function f(t), defined for all real numbers t ≥ 0, is the function F(s), defined by: L F(s)

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[ ( )] ( ) ( )

st

f t F s f t e dt

 

   L

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Why s-domain?

  • We can transform an ordinary differential

equation into an algebraic equation which is easy to solve.

  • It is also easy to analyze and design

interconnected (series, feedback etc.) systems.

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Unit step function

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1 ( ) ( ) t f t u t t       

[1] 1 1

st st

e dt e s s s s

   

             

L

  • 1

[1] s  L

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Exponential function

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( ) ( )

( ) [ ] ( ) 1 ( ) ( ) 1

at at at st s a t s a t

f t e e e e dt e dt e s a s a s a s a

       

                   

 

L

1 [ ]

at

e s a   L

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Frequency shift

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1 [1] s  L

1 [ 1]

at

e s a    L

[ ( )] ( )

at

e f t F s a   L

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Sine and cosine functions

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2 2

[cos ] s t s     L

2 2

[sin ] t s      L

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Impulse function

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( ) f t  

[ ( )] ( ) 1

st st t

t t e dt e  

    

  

L

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Unit ramp

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( ) ( ) t t f t u t t       

udv uv vdu  

 

(integration by parts)

2

[ ] 1

st st st st

t e t dt e t e e t d dt s s s s

       

             

  

L

1

! [ ]

n n

n t s   L

similarly

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Differentiated function

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[ ( )] ( ) f t F s  L

( ) ( ) (0) df t sF s f dt         L

1 2 ( 1)

( ) ( ) (0) (0)..... (0)

n n n n n n

d f t s F s s f dt s f f

  

           L

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Integrated function

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( ) ( )

t

F s f t dt s       

L

2nd shifting theorem

 

( ) ( )

as

f t a e F s

  L

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Solution of differential equations using Laplace Transformation

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Differential Equation Transformed Equation Transformed Solution Solution

Laplace Transformation Algebraic Manipulation Inverse Laplace Particular Integral Complementary function

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Example

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2 2 2

2 5 5 ( ) (0) 2 ( ) 5 ( ) ( 2) 5 ( ) 5 2 2.5(1 )

t t t t t

dx x dt sx s x x s s x s s s x t e dt e e

  

               

Transformed Solution Transformed Equation

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Convolution integral

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1 2 1 2

( ) ( ). ( ) ( ) ( ) ( ) F s F s F s f t f t f t     Ex:

2 2 1 2 2( ) 2 2 2

1 1 1 ( ) 3 2 ( 1) ( 2) ( ) ( ) ( ) ( 1)

t t t t t t t t t t t

F s s s s s f t e e f f t d e e d e e d e e e e

  

    

        

                 

  