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Laplace Transformation II

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(1)

Laplace Transformation II

(2)

Why use Laplace Transform?

Algebraic Manipulation of ODE

Solution of ODE is hard.

Tranform in to a “domain” where it’s easier to solve

Solve in the new domain Perform “inverse” transform.

Laplace domain is a frequency domain.

Integration, Differentiation

becomes multiplication, division.

(3)

 Definition: £ [f(t)] =

£ : f(t)  F(s) , s=  +j  (complex variable) f(t) : a time function such that f(t)=0 for t<0

0

( )

st

( ) f t e dt F s

 

Laplace Transformation

Integration from 0-

[

t

] A

Ae s

L 

0

[1( )] 1

[1( )]

st

t s

t t e

s

 

L L

2 2

2 2

[ sin ] [ cos ]

A t A s A t As

s

 

 

 

  L

L

 

0

0

( ) 1

( )

t s

1

t

t t e

  

L L

2

[ ] t  1

L

(4)

Theorem 1. Linearity

Theorem 2. Superposition

Theorem 3. Translation in time.

0

( )

0

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

( )1( ) ( . )

( )1( ) ( ) ( ( )1( ) 0 0)

st

s a

a

s sa sa

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

f e d let t a

f e e d e F s f for

   

     

    

  

   

 

L

(a0)

Useful Theorems

[ af t ( )]  aF s ( ) L

1 2 1 2

[ ( ) f t  f t ( )]  F s ( )  F s ( )

L

(5)

Theorem 4. Complex differentiations

Theorem 5. Translation in the s-domain [ ( )] d ( )

tf t F s

  ds L

[1] 1

 s

L 1

2

[ 1] d ( )

t F s

ds s

   

L

2 3

2

0

0 0

2

2 2

2

1 2

[ ] [ ] [ ( )] ( )

) . ( ) ( )

( ) ( ) ( ) [ ( )]

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

st

st st

n

n n

n

d d

t t t tf t F s

ds s s ds

proof let F s f t e dt

d F s f t e dt tf t e dt tf t

ds s

d d

similarly t f t F s t f t F s

ds ds

 

          

 

  

       

   

 

L L L

L

L L

2 2

( )

[ cos ]

( )

at

s a

e t

s a

 

 

  [ e f t

at

( )]  F s a (  ) L

L

Useful Theorems

(6)

 

0

0 0

2

2

( ) ( )

) . [ ( )] ( )

( ) ( ) ( )

(0 ) ( )

( ) (0 )

, [ ( )] [ ( )] [ ( )]

( ) (0 ) '(0 ) ( ) (0 ) '(0 )

[

st

st st

n n

Df t d f t dt

d d

proof let f t f t e dt

dt dt

f t e f t e dt s

f s F s

s F s f

similarly D f t D Df t Df t

s s F s f f s F s s f f

d f dt

  

    

   

   

            

L

L L L

L

1 2

( 1)

( )] ( ) (0) '(0 )

(0 )

n n n

n

t s F s s f s f

f

      

 

Useful Theorems

Theorem 6. Real Differentiation

[ d ( )] ( ) (0 )

f t s F s f

dt    

L

(7)

Theorem 7. Real Integration

Theorem 8. Complex Integration

) 0 ( )

( )

( 1 1

0 t f t dt  D  f t  D  f

0 0 0

0 0 0

1

0 0 0

( ) ( )

1 1

( ) ( )

1 1 ( ) (0)

( ) ( )

t t

st

t

st st

t

st t

f t dt f d e dt

e f d e f t dt

s s

F s f

f d e f t dt

s s s s

 

 

 

 

 

 

 

   

   

 

 

 

L

( ) f t

t

  

 

 

L ( )

s

F s ds

Useful Theorems

1

0

( ) (0)

( )

t

F s f

f t dt

s s

 

 

 

  

L

(8)

Theorem 9. Final value Theorem

Theorem 10. Initial value Theorem

0

( ) ( )

lim lim

t s

f t sF s



0

( ) ( )

lim lim

t s

f t sF s



Useful Theorems

(9)

 

-1

-1

: ( ) ( ) : ( ) ( )

( ) ( ) 1 ( )

2

c j

st c j

f t F s F s f t

f t F s F s e ds

j

  

L L

L

1

1 0

1

1 1 0

( ) ( )

( )

m m

m m

n n

n

a s a s a

F s P s

Q s s b s b s b

  

 

   

(nm)

( c : real constant )

* Inverse Laplace Transformation by Partial Fraction Method

1

1 1 0

2

1 2 1 2

real complex conjugate, a , b : real num.

( )( ) ( )

n n

s b s

n

b s b

s c s c s d s d

   

    

1 2 1 2

2

1 2 1 2

( ) s

F s s c s c s d s d

    

     

     

Inverse Laplace Transformation

(10)

2 2 2

d ds

2

) ( ) 1

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

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

2, 1, 3, 1

2 1 ( 3) ( 2) 1

( 2)

3 3 3 ( 3)

1, 1

a b c

ex F s

s s s s s

a s s b s c s

let s than b let s than c

s s s

a s b c a c

s s s s

a b

   

    

      

     

    

        

   

    1 1

2

1

, 1, ( )

( 2) ( 2) ( 3)

c F s

s s s

    

  

2 2 3

( ) f t   e

t

 te

t

 e

t

=> Inverse Laplace Transformation

(partial fraction method)

Examples of Inverse Laplace Transformation

2 2 2 2 2

3

10 1 4

10 4 10 4

) ( )

6 25 ( 3) 4 4 ( 3) 4

( ) 10 sin 4 4

t

ex F s

s s s s

f t te

    

     

 

(11)

Solution of Differential Equation by Laplace Transformation

 

2

2

2 4 1 (0) 0 , (0) 2

L.T: ( ) (0) (0) 2 ( ) (0) 4 ( ) 1

1 2 1

( 2 4) ( ) 2

y y y y y

s Y s sy y sY s y Y s

s s s Y s s

s s

       

      

     

 

2

2 2

2 1 1 1 1 1

( )

( 2 4) 4 4 ( 1) 3

1 1 1

( ) cos 3 sin 3

4 4 4 3

t t

s s

Y s s s s s s

y t te

te

  

  

   

   

(12)

Laplace Transform Table

Nise Ch.2

(13)

Laplace Transform Theorems

Nise Ch.2
(14)

End of Laplace Transform

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