The Laplace Transform of step functions (Sect. 6.3)

The Laplace Transform of step functions (Sect. 6.3). I Overview and notation. I The definition of a step function. I Piecewise discontinuous fun...
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The Laplace Transform of step functions (Sect. 6.3).

I

Overview and notation.

I

The definition of a step function.

I

Piecewise discontinuous functions.

I

The Laplace Transform of discontinuous functions.

I

Properties of the Laplace Transform.

Overview and notation. Overview: The Laplace Transform method can be used to solve constant coefficients differential equations with discontinuous source functions.

Notation: If L[f (t)] = F (s), then we denote L−1 [F (s)] = f (t).

Remark: One can show that for a particular type of functions f , that includes all functions we work with in this Section, the notation above is well-defined.

Example   1 From the Laplace Transform table we know that L e at = . s − a h 1 i −1 Then also holds that L C = e at . s −a

The Laplace Transform of step functions (Sect. 6.3).

I

Overview and notation.

I

The definition of a step function.

I

Piecewise discontinuous functions.

I

The Laplace Transform of discontinuous functions.

I

Properties of the Laplace Transform.

The definition of a step function. Definition A function u is called a step function at t = 0 iff holds ( 0 for t < 0, u(t) = 1 for t > 0.

Example Graph the step function values u(t) above, and the translations u(t − c) and u(t + c) with c > 0. Solution: u(t)

u(t − c)

1

1

0

t

u(t + c)

0

1

c

t

−c

0

t

C

The definition of a step function. Remark: Given any function values f (t) and c > 0, then f (t − c) is a right translation of f and f (t + c) is a left translation of f .

Example at

f(t)

a(t−c)

f(t)= e

f(t)

1

1

0

f(t)

0

t

at

f(t)

f(t)= u(t)e

1

0

f(t)= e

c

t

a(t−c)

f(t)= u(t−c) e

1

t

0

c

t

The Laplace Transform of step functions (Sect. 6.3).

I

Overview and notation.

I

The definition of a step function.

I

Piecewise discontinuous functions.

I

The Laplace Transform of discontinuous functions.

I

Properties of the Laplace Transform.

Piecewise discontinuous functions. Example Graph of the function b(t) = u(t − a) − u(t − b), with 0 < a < b. Solution: The bump function b can be graphed as follows:

u(t −a)

u(t −b)

1

1

0

a

b

0

t

a

b

t

b(t)

1

0

a

b

t

C

Piecewise discontinuous functions. Example   Graph of the function f (t) = e at u(t − 1) − u(t − 2) . Solution: y

f(t)=e

at

[ u ( t −1 ) − u ( t −2 ) ] e

1

at

[ u ( t −1 ) − u ( t −2 ) ]

1

2

t

Notation: The function values u(t − c) are denoted in the textbook as uc (t).

The Laplace Transform of step functions (Sect. 6.3).

I

Overview and notation.

I

The definition of a step function.

I

Piecewise discontinuous functions.

I

The Laplace Transform of discontinuous functions.

I

Properties of the Laplace Transform.

The Laplace Transform of discontinuous functions. Theorem Given any real number c, the following equation holds, L[u(t − c)] =

e −cs , s

s > 0.

Proof: Z



L[u(t − c)] =

e

−st

Z u(t − c) dt =

N→∞

e −st dt,

c

0

L[u(t − c)] = lim −



 e −cs 1 −Ns e − e −cs = , s s

e −cs We conclude that L[u(t − c)] = . s

s > 0.

The Laplace Transform of discontinuous functions. Example Compute L[3u(t − 2)]. e −2s L[3u(t − 2)] = 3 L[u(t − 2)] = 3 . s

Solution:

3e −2s We conclude: L[3u(t − 2)] = . s

C

Example −1

Compute L

Solution:

h e 3s i s

−1

L

.

h e 3s i s −1

We conclude: L

−1

=L

h e 3s i s

h e −(−3)s i s

= u(t − (−3)).

= u(t + 3).

The Laplace Transform of step functions (Sect. 6.3).

I

Overview and notation.

I

The definition of a step function.

I

Piecewise discontinuous functions.

I

The Laplace Transform of discontinuous functions.

I

Properties of the Laplace Transform.

C

Properties of the Laplace Transform. Theorem (Translations) If F (s) = L[f (t)] exists for s > a > 0 and c > 0, then holds L[u(t − c)f (t − c)] = e −cs F (s),

s > a.

Furthermore, L[e ct f (t)] = F (s − c),

s > a + c.

Remark: I I

   L translation (uf ) = (exp) L[f ] .    L (exp) (f ) = translation L[f ] .

Equivalent notation: I

L[u(t − c)f (t − c)] = e −cs L[f (t)],

I

L[e ct f (t)] = L[f ](s − c).

Properties of the Laplace Transform. Example   Compute L u(t − 2) sin(a(t − 2)) . a , L[u(t − c)f (t − c)] = e −cs L[f (t)]. 2 2 s +a   a . L u(t − 2) sin(a(t − 2)) = e −2s L[sin(at)] = e −2s 2 s + a2   a We conclude: L u(t − 2) sin(a(t − 2)) = e −2s 2 . C s + a2

Solution: L[sin(at)] =

Example   Compute L e 3t sin(at) . Solution: Recall: L[e ct f (t)] = L[f ](s − c).   a We conclude: L e 3t sin(at) = , with s > 3. (s − 3)2 + a2

C

Properties of the Laplace Transform. Example ( Find the Laplace transform of f (t) =

0,

t < 1,

(t 2 − 2t + 2), t > 1.

Solution: Using step function notation, f (t) = u(t − 1)(t 2 − 2t + 2). Completing the square we obtain, t 2 − 2t + 2 = (t 2 − 2t + 1) − 1 + 2 = (t − 1)2 + 1. f(t)

This is a parabola t 2 translated to the right by 1 and up by one. This is a discontinuous function.

1

0

1

t

Properties of the Laplace Transform. Example ( Find the Laplace transform of f (t) =

0,

t < 1,

(t 2 − 2t + 2), t > 1.   Solution: Recall: f (t) = u(t − 1) (t − 1)2 + 1 . This is equivalent to f (t) = u(t − 1) (t − 1)2 + u(t − 1). Since L[t 2 ] = 2/s 3 , and L[u(t − c)g (t − c)] = e −cs L[g (t)], then L[f (t)] = L[u(t − 1) (t − 1)2 ] + L[u(t − 1)] = e −s  e −s We conclude: L[f (t)] = 3 2 + s 2 . s

2 −s 1 + e . s3 s C

Properties of the Laplace Transform. Remark: The inverse of the formulas in the Theorem above are:   L−1 e −cs F (s) = u(t − c) f (t − c),   L−1 F (s − c) = e ct f (t).

Example h e −4s i Find L . s2 + 9 h −4s i 1 h 3 i −1 e −1 −4s Solution: L = L e . s2 + 9 3 s2 + 9 h a i −1 = sin(at). Then, we conclude that Recall: L s 2 + a2 h −4s i 1  −1 e L = u(t − 4) sin 3(t − 4) . s2 + 9 3 −1

C

Properties of the Laplace Transform. Example (s − 2) i Find L . (s − 2)2 + 9 h s i   −1 −1 = cos(at), Solution: L L F (s − c) = e ct f (t). 2 2 s +a h (s − 2) i −1 = e 2t cos(3t). We conclude: L 2 (s − 2) + 9 −1

h

Example −1

Find L

h 2e −3s i s2 − 4

.

a i Solution: Recall: L = sinh(at) s 2 − a2   and L−1 e −cs F (s) = u(t − c) f (t − c). −1

h

C

Properties of the Laplace Transform. Example −1

Find L

h 2e −3s i s2 − 4

.

Solution: Recall: h a i −1 = sinh(at), L s 2 − a2 −1

L

−1

We conclude: L

  L−1 e −cs F (s) = u(t − c) f (t − c).

h 2e −3s i s2 − 4

h 2e −3s i s2 − 4

−1

=L

h

e

−3s

2 i . s2 − 4

 = u(t − 3) sinh 2(t − 3) .

Properties of the Laplace Transform. Example −1

Find L

h

e −2s i . s2 + s − 2

Solution: Find the roots of the denominator: ( √   s+ = 1, 1 s± = −1 ± 1 + 8 ⇒ 2 s− = −2. Therefore, s 2 + s − 2 = (s − 1) (s + 2). Use partial fractions to simplify the rational function: b 1 a 1 = + , = (s − 1) (s + 2) s2 + s − 2 (s − 1) (s + 2) 1 (a + b) s + (2a − b) = a(s + 2) + b(s − 1) = . s2 + s − 2 (s − 1) (s + 2)

C

Properties of the Laplace Transform. Example e −2s i . Find L s2 + s − 2 (a + b) s + (2a − b) 1 = Solution: Recall: 2 s +s −2 (s − 1) (s + 2) 1 1 a + b = 0, 2a − b = 1, ⇒ a = , b = − . 3 3 h e −2s i 1 h 1 i 1 −1 h −2s 1 i −1 −1 −2s = L − L . L e e s2 + s − 2 3 s −1 3 s +2 h 1 i   −1 Recall: L = e at , L−1 e −cs F (s) = u(t − c) f (t − c), s −a h e −2s i 1 1 −1 (t−2) L = u(t − 2) e − u(t − 2) e −2(t−2) . 2 s +s −2 3 3 h e −2s i 1 h i −1 (t−2) −2(t−2) = u(t − 2) e −e Hence: L . C s2 + s − 2 3 −1

h