Laplace Transform: Derivatives, Integrals, and Solving Linear Differential Equations, Assignments of Electrical and Electronics Engineering

The laplace transform properties for derivatives and integrals of time functions, as well as the application of the partial-fraction technique to solve linear differential equations. It includes proofs, examples, and solutions.

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Boise State University
Department of Electrical and Computer Engineering
ECE 360 System Modeling and Control
The Laplace Transform II
Reading Assignment: Read Secs. 2.4-2.5.
Lecture Objectives:
1. To derive the Laplace transforms of the derivative and integral of a time function.
2. To apply the partial-fraction technique in the solution of linear differential equations.
Property 5: Derivative of a Time Function
L {f(t)}=Z
0
f(t)est dt =F(s)
L©f0(t)ª=L½df
dt ¾=sF (s)f(0)
Proof:
L©f0(t)ª=L½df
dt ¾=Z
0
df
dt est dt
=Z
0
est df
= [f(t)est]
0Z
0
f(t)d(est)
= [f()esf(0)es0] + sZ
0
f(t)est dt
=sF (s)f(0)
Higher Derivatives of a Time Function:
L©f00(t)ª=L½d
dt £f0(t)¤¾=sL©f0(t)ªf0(0)
=s[sF (s)f(0)] f0(0)
=s2F(s)sf(0)f0(0)
L©f000(t)ª=L½d
dt £f00(t)¤¾=sL©f00(t)ªf00 (0)
=s[s2F(s)sf(0)f0(0)] f00(0)
=s3F(s)s2f(0)sf0(0)f00(0)
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Boise State University Department of Electrical and Computer Engineering ECE 360 – System Modeling and Control

The Laplace Transform II

Reading Assignment: Read Secs. 2.4-2.5.

Lecture Objectives:

  1. To derive the Laplace transforms of the derivative and integral of a time function.
  2. To apply the partial-fraction technique in the solution of linear differential equations.

Property 5: Derivative of a Time Function

L {f (t)} =

∫ (^) ∞

0

f (t)e−st^ dt = F (s)

L

{ f ′(t)

} = L

{ (^) df dt

} = sF (s) − f (0−)

Proof:

L

{ f ′(t)

} = L

{ (^) df dt

}

∫ (^) ∞ 0 −

df dt

e−st^ dt

=

∫ (^) ∞

0 −

e−st^ df

= [f (t)e−st]∞ 0 − −

∫ (^) ∞

0 −

f (t) d(e−st)

= [f (∞)e−s∞^ − f (0−)e−s^0 −] + s

∫ (^) ∞ 0 −

f (t)e−st^ dt = sF (s) − f (0−)

Higher Derivatives of a Time Function:

L

{ f ′′(t)

} = L

{ (^) d dt

[ f ′(t)

]} = sL

{ f ′(t)

} − f ′(0−) = s[sF (s) − f (0−)] − f ′(0−) = s^2 F (s) − sf (0−) − f ′(0−) L

{ f ′′′(t)

} = L

{ (^) d dt

[ f ′′(t)

]} = sL

{ f ′′(t)

} − f ′′(0−)

= s[s^2 F (s) − sf (0−) − f ′(0−)] − f ′′(0−) = s^3 F (s) − s^2 f (0−) − sf ′(0−) − f ′′(0−)

Property 6: Integral of a Time Function

L {f (t)} =

∫ (^) ∞

0

f (t)e−st^ dt = F (s)

L

{∫ (^) ∞

0

f (t)

}

F (s) s

Proof:

F (s) = L {f (t)} = L

{ (^) d dt

∫ (^) t

0

f (t) dt

} = sL

{∫ (^) t

0

f (t) dt

} −

∫ (^0)

0

f (t) dt

Examples:

0 1 2 t 0 1 2 t 0 1 2 t

1

2 2

1

2

u(t) tu(t) 0.5t 2 u(t)

1

f (t) = u(t) f (t) = tu(t) f (t) = 1 2

t^2 u(t)

F (s) = 1 s

F (s) = 1 /s s

s^2

F (s) = 1 /s

2 s

s^3

Solution of Linear Differential Equations:

Example 2: Solve

dx dt

  • 2x = e−^2 t, x(0) = 5

Solution: Let X(s) = L {x(t)}.

sX(s) − x(0) + 2X(s) =

s + 2 (s + 2)X(s) = 5 +

s + 2 =^

5 s + 11 s + 2 X(s) =

5 s + 11 (s + 2)^2 =^

A

s + 2 +^

B

(s + 2)^2 =^

A(s + 2) + B (s + 2)^2 X(s) = 5 s^ + 11 (s + 2)^2

= As^ + (2A^ +^ B) (s + 2)^2

{ A = 5 2 A + B = 11 =⇒

{ A = 5 B = 1

X(s) = 5 s + 2

(s + 2)^2 x(t) = 5 e−^2 t^ + te−^2 t, t ≥ 0 x(0) = 5 + 0 = 5

Alternate Method for Partial-Fraction Expansion:

X(s) = 5 s^ + 11 (s + 2)^2

= A

s + 2

+ B

(s + 2)^2 B =

[ (s + 2)^2 X(s)

]

[^ s=−^2 =^ [5s^ + 11]s=−^2 =^1 (s + 2)^2 X(s)

] s=0 =^ [A(s^ + 2) +^ B]s= [5s + 11]s=0 = [A(s + 2) + B]s= 11 = 2 A + 1 =⇒ A = 5 X(s) = 5 s^ + 6 (s + 2)^2

s + 2

(s + 2)^2

Solution of Linear Differential Equations:

Example 3: Solve

d^2 x dt^2 + 4^

dx dt + 13x^ =^6 e

−t, x(0) = 0 , x′(0) = 0

Solution: Let X(s) = L {x(t)}.

s^2 X(s) − sx(0) − x′(0) + 4[sX(s) − x(0)] + 13X(s) = 6 s + 1 (s^2 + 4s + 13)X(s) = 6 s + 1

X(s) = 6 (s + 1)(s^2 + 4s + 13)

= A

s + 1

  • Bs^ +^ C (s + 2)^2 + 3^2

= A(s

(^2) + 4s + 13) + (Bs + C)(s + 1) (s + 1)[(s + 2)^2 + 3^2 ]

=

(A + B)s^2 + (4A + B + C)s + (13A + C) (s + 1)[(s + 2)^2 + 3^2 ]

  

A + B = 0

4 A + B + C = 0

13 A + C = 6

  

A = 0. 6

B = − 0. 6

C = − 1. 8

X(s) = 0.^6 s + 1

− 0.^6 s^ + 1.^8 [(s + 2)^2 + 3^2 ] X(s) = 0.^6 s + 1

− 0 .6(s^ + 2) + 0.^2 ×^3 [(s + 2)^2 + 3^2 ] x(t) = 0. 6 e−t^ − 0. 6 e−^2 t^ cos 3t − 0. 2 e−^2 t^ sin 3t, t ≥ 0 x(0) = 0. 6 − 0 .6 + 0 = 0