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Laplace Transformation I

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Laplace Transformation I

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Why use Laplace Transform?

Algebraic Manipulation of ODE

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 Definition:

£ [f(t)]

=

£: f(t)  F(s) , s= +j (complex variable)

f(t) : a time function such that f(t)=0 for t<0

 Inverse Laplace Transformation

L

1[ ( )]F s f t( )

0

( )

st

( )

f t e dt F s

 

Laplace Transformation

(4)

f(t) Laplace – transformable

if i) f(t) piecewise-continuous

ii) f(t) of exponential order as t approaches infinity

- bounded, exist.

- or approaches zero as t approaches infinity.

If

the : the abscissa of convergence

Existence of Laplace Transformation

lim

t

( ) 0

c

t c

e f t for

for

 

 



 

    

c

t ( ) e f t )

(t et f

(5)

2

0 ( )

0 0, T< t

e

t

for t T

f t

for t

    

   

 

0 0

lim sin

0

t t

e t t if

if

 



 

    

lim

t ct

0

t

if c

e te

if c



  

     

c

0

 

c

c

  

, , sin , .

ct ct ct

e

te

e

 t c  const , sin , sin ...

t  t t  t

example : 1)

the abscissa of convergence

2)

the abscissa of convergence

2 2

t

,

t

e te

does not possess L. T.

L[f(t)] exists.

- The signals that can be physically generated always have corresponding Laplace transforms

Existence of Laplace Transformation

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0 0

( ) t 0

for t f t Ae for t

 

  

0

( )

0

( ) 0

( )

[ ]

1 1

[ ]

1 1

[ ]

t t st

s t

s

j

Ae Ae e dt

Ae dt

A e e

s s

A e

s s

 

 

 

 

  

  

 

  

 

  

 

L

Laplace Transformation of simple function

Exponential function

A,

a

: constants

(s  j)

j

   

(7)

step function

( ) 0

0 0

f t A t

t

 

   

unit step input function

0 0

1 1

[ ( )] [ ]

[0 1 ] Re[ ] 0

st s s

f t Ae dt A e e

s s

A if s

s

   

  

  

L

Laplace Transformation of simple function

0 0

0

1( ) 1

0

1 0

1( ) 0 0

[1( )] 1

t t t t

t t t t

t

t s

 

    

 

   

L 

(8)

 Sinusoidal Functions

cos 1 ( )

2

sin 1 ( )

2

j t j t

j t j t

t e e

t e e

j

 

 

0

2 2

2 2

[ sin ] ( )

2

1 1 1

( )

2

[ cos ]

j t j t st

A t A e e e dt

j

j s j s j

A s A t As

s

 

 

 

 

 

 

 

L

L

Ramp function

Laplace Transformation of simple function

[ ]

0 st

st st

At A te dt

e e

A t dt

 

 

 

L

sin 0

( ) 0 0

A t t

f t t

  

( ) 0

0 0

At t

f t t

 

  

(9)

0 0

0

( ) 0

0 0, < t

A for t t

f t t

for t t

  

 

 

0

0 0

( ) A 1( ) A 1( )

f t t t t

t t

  

0 0

0

0

0 0

0 0

0 0

[ ( )] lim 1(1 )

(1 )

lim

( )

t s t

t s

t

f t A e

t s

d A e

dt A s

d s A

dt t s

 

   

 

  

  

  

L

Pulse function

Impulse function

0

0 0 0

0

lim 0

( )

0 0,

t

A for t t

f t t

for t t t

  

 

  

0

0

0 0

0

[ ( )] 1( ) 1( )

1 (1

t s

)

A A

f t t t t

t t

A e

t s

   

      

   

 

L L L

Laplace Transformation of simple function

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 

0

0 0 0

0

0

0 0

lim 1 0

( )

0 0,

( ) 0 ( ) ( ) ( ) 1

0 0

t

st

for t t

f t t

for t t t

t t t t e dt t dt

t   

  

 

  

 

   L

The unit-impulse function occuring at

 

0 0 0

0

0

0 0 0

0 0

( ) ( ) ( ) ( ) 1

0

t

st t s

st t

t t

t t t t t e dt t t e dt e

t t

   

 

   L  

 

  

t  t

0

Laplace Transformation of simple function

Unit impulse function ; impulse function of magnitude 1

Referensi

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