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Properties of Laplace Transform
Name
Md. Mehedi Hasan
Student ID
Presented to
Laplace Transform Properties
 Definition of the Laplace transform
 A few simple transforms
 Rules
 Demonstrations
Definition
 The Laplace transform is.
 Common notation:
    
 s
dtett st
F
ffL
0

 



    
    st
st
Gg
Ff


L
L    
   st
st
Gg
Ff


   




0
fF dtets st
       



0
vuvu dttttt
Definition
 Notation:
 Variables in italics t, s
 Functions in time space f, g
 Functions in frequency space F, G
 Specific limits
   
   t
t
t
t
flim0f
flim0f
0
0








Example Transforms
 We will look at the Laplace transforms of:
 The impulse function d(t)
 The unit step function u(t)
 The ramp function t
 Sine and cosine
 Exponential Function
 Time differentiation
Impulse Function
 The easiest transform is that of the impulse function:
    
1
δδ
0
0







s
st
e
dtettL
  1δ  t
Unit Step Function
 Next is the unit step function
    
s
e
s
e
s
dte
dtett
s
st
st
st
1
1
0
1
uuL
0
0
0
0























 






11
00
u
t
t
t  
s
t
1
u 
Ramp Function
 The ramp function
  
2
0
0
00
0
111
1
0
1
1
1
u
s
e
ss
dte
s
dte
s
e
s
t
dttett
st
st
stst
st





































L
  2
1
u
s
tt 
t
t
ddf
f


st
st
e
s
te




1
g
ddg
The Sine Function
 Sine requires two integration by parts:
      
   
 
   
 
    tt
ss
dtet
ss
dtet
ss
stet
s
dtet
s
dtet
s
stet
s
dtettt
st
st
st
st
st
usin
11
sin
11
sin
11
cos
1
cos
1
0
cos
1
sin
1
sinusin
22
0
22
0
2
0
0
00
0
L
L




























The Sine Function
 Consequently:
         
      
    
1
1
usinL
1usinL1
usinL
11
usinL
2
2
22




s
tt
tts
tt
ss
tt
   
1
1
usin 2


s
tt
The Cosine Function
 As does cosine:
      
   
 
   
 
    tt
ss
dtet
ss
dtet
ss
stet
ss
dtet
ss
dtet
s
stet
s
dtettt
st
st
st
st
st
ucosL
11
cos
1
0
1
cos
11
sin
11
sin
11
sin
1
cos
1
cosucosL
2
0
22
0
2
0
0
00
0




































The Cosine Function
 Consequently:
         
      
    
1
ucos
ucos1
ucos
11
ucos
2
2
2




s
s
tt
stts
tt
ss
tt
L
L
LL
   
1
ucos 2


s
s
tt
Integration of Exponential Functions
 We now have the following commutative diagram
 
ass
s
e at



11
L
 








 
assa
e
a
at
111
1L
1
 ass 
1










t
a
de
0
L 
The Convolution
 Define the convolution to be
 Then
      
    

dt
dtt








gf
gfgf
      
       ss
j
tt
sst
GF
2
1
gf
GFgf



Integration
 As a special case of the convolution
         
   
s
s
s
s
sttsd
t
F1
F
uff
0











LL 
Summary
 We have seen these Laplace transforms:
 
 
 
  1
2
!
u
1
u
1
u
1δ





n
n
s
n
tt
s
tt
s
t
t
 
   
   
1
ucos
1
1
usin
1
1
u
2
2






s
s
tt
s
tt
s
tet
Summary
 In this topic:
 We defined the Laplace transform
 Looked at specific transforms
 Derived some properties
 Applied properties
References
 Spiegel, Laplace Transforms, McGraw-Hill, Inc., 1965.
 Wikipedia, http://en.wikipedia.org/wiki/Laplace_Transform
Thank You

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Properties of laplace transform

  • 1. Properties of Laplace Transform Name Md. Mehedi Hasan Student ID Presented to
  • 2. Laplace Transform Properties  Definition of the Laplace transform  A few simple transforms  Rules  Demonstrations
  • 3. Definition  The Laplace transform is.  Common notation:       s dtett st F ffL 0                st st Gg Ff   L L        st st Gg Ff           0 fF dtets st            0 vuvu dttttt
  • 4. Definition  Notation:  Variables in italics t, s  Functions in time space f, g  Functions in frequency space F, G  Specific limits        t t t t flim0f flim0f 0 0        
  • 5. Example Transforms  We will look at the Laplace transforms of:  The impulse function d(t)  The unit step function u(t)  The ramp function t  Sine and cosine  Exponential Function  Time differentiation
  • 6. Impulse Function  The easiest transform is that of the impulse function:      1 δδ 0 0        s st e dtettL   1δ  t
  • 7. Unit Step Function  Next is the unit step function      s e s e s dte dtett s st st st 1 1 0 1 uuL 0 0 0 0                                11 00 u t t t   s t 1 u 
  • 8. Ramp Function  The ramp function    2 0 0 00 0 111 1 0 1 1 1 u s e ss dte s dte s e s t dttett st st stst st                                      L   2 1 u s tt  t t ddf f   st st e s te     1 g ddg
  • 9. The Sine Function  Sine requires two integration by parts:                        tt ss dtet ss dtet ss stet s dtet s dtet s stet s dtettt st st st st st usin 11 sin 11 sin 11 cos 1 cos 1 0 cos 1 sin 1 sinusin 22 0 22 0 2 0 0 00 0 L L                            
  • 10. The Sine Function  Consequently:                       1 1 usinL 1usinL1 usinL 11 usinL 2 2 22     s tt tts tt ss tt     1 1 usin 2   s tt
  • 11. The Cosine Function  As does cosine:                        tt ss dtet ss dtet ss stet ss dtet ss dtet s stet s dtettt st st st st st ucosL 11 cos 1 0 1 cos 11 sin 11 sin 11 sin 1 cos 1 cosucosL 2 0 22 0 2 0 0 00 0                                    
  • 12. The Cosine Function  Consequently:                       1 ucos ucos1 ucos 11 ucos 2 2 2     s s tt stts tt ss tt L L LL     1 ucos 2   s s tt
  • 13. Integration of Exponential Functions  We now have the following commutative diagram   ass s e at    11 L             assa e a at 111 1L 1  ass  1           t a de 0 L 
  • 14. The Convolution  Define the convolution to be  Then              dt dtt         gf gfgf               ss j tt sst GF 2 1 gf GFgf   
  • 15. Integration  As a special case of the convolution               s s s s sttsd t F1 F uff 0            LL 
  • 16. Summary  We have seen these Laplace transforms:         1 2 ! u 1 u 1 u 1δ      n n s n tt s tt s t t           1 ucos 1 1 usin 1 1 u 2 2       s s tt s tt s tet
  • 17. Summary  In this topic:  We defined the Laplace transform  Looked at specific transforms  Derived some properties  Applied properties
  • 18. References  Spiegel, Laplace Transforms, McGraw-Hill, Inc., 1965.  Wikipedia, http://en.wikipedia.org/wiki/Laplace_Transform