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LAPLACE TRANSFORM
TABLES

MATHEMATICS CENTRE

©2000
DEFINITION
The Laplace transform f ( s ) of a function f(t) is defined by:

f (s) =

∞

∫e

− st

f (t ) dt

0

TRANSFORMS OF STANDARD FUNCTIONS

f(t)

f (s)

1

1
s

e−αt

1
s+α

t
1 −T
e
T

1
1+ sT

1− e −α t

α
s (s + α )

te− α t

1

(s + α )2

e −α t − e − β t

β −α
( s + α )(s + β

t

1
s2

tn

n!
sn +1

e −α t t n

n!

(s + α )n +1
ω
s + ω2

sin ωt

2

s
s + ω2

cosωt

2

2

)
f(t)

f (s)

e −α t sin ω t

ω

(s + α )2 + ω 2

e −α t cos ω t

s+α

(s + α )2 + ω 2
ω2
s s2 +ω

1− cosωt

1
2ω

3

(sin ω

(

t − ω t cos ω t )

(s

t
sin ω t
2ω

(s

α


e − α t  cos ω t − sin ω t 
ω



1
2

)

s
2

)

2 2

+ω

)

2 2

+ω
s

(s + α )

2

+ω

2

s sin φ + ω cos φ
s2 +ω 2

sin (ω t + φ )
e −α t +

2

α
sin ω t − cos ω t
ω

α

2

+ω

2

( s + α )(s 2 + ω

sin 2 ωt

(

2ω

2

s s 2 + 4ω
cos2 ωt

s 2 + 2ω

(

s s 2 + 4ω

β
s −β2

sinh βt

2

cosh βt

s
s −β2
2

3

2

2

)

2
2

)

)
f(t)

f (s)

e −α t sinh β t

β

( s + α )2 − β
s +α

e −α t cosh β t

( s + α )2 − β

t sinh β t

(s

t cosh β t

2β

3

(β

t cosh β

t − sinh β

2β
2

s

−β

t)

(s

2

−β

−β

)

2 2

δ(t)

1

Unit step :

H(t)

1
s

Ramp:

tH(t)

1
s2

Delayed Unit Impulse: δ(t-T)

e-sT

Delayed Unit Step:

H(t-T)

e − sT
s

Rectangular Pulse:

H(t)-H(t-T)

1− e − sT
s

4

)

2 2

Transforms of Special Functions
Unit impulse :

)

2

1
2

2

2 2

s2 + β

(s
1

2
TRANSFORM THEOREMS
f(t)

f (s)

e-αt f(t)

f (s + α )

f(t-T)H(t-T)

e − sT f ( s )

f(kt)

1 s
f 
k k 

Damping:
Delay:
Time scale:

Integral:

∫

t

0

1
f ( s)
s

f (t ) dt

Differentiation
sf ( s ) − f ( 0)

d
f (t )
dt
d2
f (t )
dt 2
dn
f (t )
dt n
Initial Value:

s 2 f ( s) − sf ( 0) − f '( 0)
s n f ( s) − sn −1 f ( 0) − sn −2 f '( 0) −... − f n −1 ( 0)

lim { f (t )} = lim {s f ( s) }
t →0
s →∞

Final Value:

lim { f (t )} = lim {s f ( s) }
t →∞
s →0

Periodic Functions:

If f(t) has period T then:

f ( s) =

1
1 − e − sT

T

∫ f (t )e

− st

dt

0

further, if g(t) is defined as the first cycle of f(t), followed by zero, then f ( s ) =

g ( s)
1 − e − sT

Square Wave:
f (t ) = 1
f (t ) = 0

0< t <
T
<t <T
2

T

2





f (s) =

1  eα T − e−α T
1 +
2s  e α T + e −α T

π 

ω 

π
2π 
<t <
ω
ω


f (t ) = sin ω t

0<t<

Half-Wave Rectified Sine:
f (t ) = 0

Full-Wave Rectified Sine:


 , where


f (t ) = sin ω t

f ( s) =

5

ω

f (s) =

1 + e − sπ / ω

s 2 + ω 2 1 − e − sπ /ω

α =

s
4

ω
1
⋅
2
s + ω 1 − e − sπ / ω
2
Saw-Tooth Wave:

t
f (t ) = 0 < t < T
T

6

1
e − sT
f (s) = 2 −
s T s 1 − e − sT

(

)

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Laplace1

  • 2. DEFINITION The Laplace transform f ( s ) of a function f(t) is defined by: f (s) = ∞ ∫e − st f (t ) dt 0 TRANSFORMS OF STANDARD FUNCTIONS f(t) f (s) 1 1 s e−αt 1 s+α t 1 −T e T 1 1+ sT 1− e −α t α s (s + α ) te− α t 1 (s + α )2 e −α t − e − β t β −α ( s + α )(s + β t 1 s2 tn n! sn +1 e −α t t n n! (s + α )n +1 ω s + ω2 sin ωt 2 s s + ω2 cosωt 2 2 )
  • 3. f(t) f (s) e −α t sin ω t ω (s + α )2 + ω 2 e −α t cos ω t s+α (s + α )2 + ω 2 ω2 s s2 +ω 1− cosωt 1 2ω 3 (sin ω ( t − ω t cos ω t ) (s t sin ω t 2ω (s α   e − α t  cos ω t − sin ω t  ω   1 2 ) s 2 ) 2 2 +ω ) 2 2 +ω s (s + α ) 2 +ω 2 s sin φ + ω cos φ s2 +ω 2 sin (ω t + φ ) e −α t + 2 α sin ω t − cos ω t ω α 2 +ω 2 ( s + α )(s 2 + ω sin 2 ωt ( 2ω 2 s s 2 + 4ω cos2 ωt s 2 + 2ω ( s s 2 + 4ω β s −β2 sinh βt 2 cosh βt s s −β2 2 3 2 2 ) 2 2 ) )
  • 4. f(t) f (s) e −α t sinh β t β ( s + α )2 − β s +α e −α t cosh β t ( s + α )2 − β t sinh β t (s t cosh β t 2β 3 (β t cosh β t − sinh β 2β 2 s −β t) (s 2 −β −β ) 2 2 δ(t) 1 Unit step : H(t) 1 s Ramp: tH(t) 1 s2 Delayed Unit Impulse: δ(t-T) e-sT Delayed Unit Step: H(t-T) e − sT s Rectangular Pulse: H(t)-H(t-T) 1− e − sT s 4 ) 2 2 Transforms of Special Functions Unit impulse : ) 2 1 2 2 2 2 s2 + β (s 1 2
  • 5. TRANSFORM THEOREMS f(t) f (s) e-αt f(t) f (s + α ) f(t-T)H(t-T) e − sT f ( s ) f(kt) 1 s f  k k  Damping: Delay: Time scale: Integral: ∫ t 0 1 f ( s) s f (t ) dt Differentiation sf ( s ) − f ( 0) d f (t ) dt d2 f (t ) dt 2 dn f (t ) dt n Initial Value: s 2 f ( s) − sf ( 0) − f '( 0) s n f ( s) − sn −1 f ( 0) − sn −2 f '( 0) −... − f n −1 ( 0) lim { f (t )} = lim {s f ( s) } t →0 s →∞ Final Value: lim { f (t )} = lim {s f ( s) } t →∞ s →0 Periodic Functions: If f(t) has period T then: f ( s) = 1 1 − e − sT T ∫ f (t )e − st dt 0 further, if g(t) is defined as the first cycle of f(t), followed by zero, then f ( s ) = g ( s) 1 − e − sT Square Wave: f (t ) = 1 f (t ) = 0 0< t < T <t <T 2 T  2     f (s) = 1  eα T − e−α T 1 + 2s  e α T + e −α T π   ω   π 2π  <t < ω ω  f (t ) = sin ω t 0<t< Half-Wave Rectified Sine: f (t ) = 0 Full-Wave Rectified Sine:   , where  f (t ) = sin ω t f ( s) = 5 ω f (s) = 1 + e − sπ / ω s 2 + ω 2 1 − e − sπ /ω α = s 4 ω 1 ⋅ 2 s + ω 1 − e − sπ / ω 2
  • 6. Saw-Tooth Wave: t f (t ) = 0 < t < T T 6 1 e − sT f (s) = 2 − s T s 1 − e − sT ( )