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Definitions, examples, and the linearity theorem for inverse laplace transforms. It covers how to find the inverse laplace transform of given functions using tables and examples. The document also explains the process of finding inverse laplace transforms of complex functions through partial fraction expansion.
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Chapter 7. Laplace Transforms. Section 7.4 Inverse Laplace Transform.
Definition 1. Given a function F (s), if there is a function f (t) that is continuous on [0, ∞) and satisfies L{f }(s) = F (s), then we say that f (t) is the inverse Laplace transform of F (s) and employ the notation f (t) = L−^1 {F }(t).
Table of inverse Laplace transform
F (s) f (t) = L−^1 {F }(t) 1 s ,^ s >^0 1 s − a,^ s > a^ e
at (n − 1)! sn^ ,^ s >^0 t
n− (^1) , n = 1, 2 , ... b s^2 + b^2
, s > 0 sin bt s s^2 + b^2 ,^ s >^0 cos^ bt (n − 1)! (s − a)n^ ,^ s > a^ e
attn− (^1) , n = 1, 2 , ...
b (s − a)^2 + b^2
, s > a eat^ sin bt s − a (s − a)^2 + b^2
, s > a eat^ cos bt
Example 1. Determine the inverse Laplace transform of the given function. (a) F (s) = (^) s^23. SOLUTION. L−^1
s^3
s^3
= t^2
(b) F (s) = (^) s (^22) +. SOLUTION. L−^1
s^2 +
s^2 +2^2
= sin 2t.
(c) F (s) = (^) s (^2) +2s+1s+.
SOLUTION. L−^1
{ (^) s+ s^2 +2s+
s+ (s+1)^2 +
s+ (s+1)^2 +3^2
= e−t^ cos 3t.
Theorem 1. (linearity of the inverse transform) Assume that L−^1 {F }, L−^1 {F 1 }, and L−^1 {F 2 } exist and are continuous on [0, ∞) and c is any constant. Then
L−^1 {F 1 + F 2 } = L−^1 {F 1 } + L−^1 {F 2 } L−^1 {cF } = cL−^1 {F }.
Example 2. Determine L−^1
3 (2s+5)^3 +^
2 s+ s^2 +4s+13 +^
3 s^2 +4s+
3 (2s+5)^3 +^
2 s+ s^2 +4s+13 +^
3 s^2 +4s+
(2s + 5)^3
2 s + 16 s^2 + 4s + 13
s^2 + 4s + 8
23 (s + 52 )^3
s + 8 (s + 2)^2 + 9
(s + 2)^2 + 4
(s + 52 )^3
(s + 2) + 6 (s + 2)^2 + 3^2
(s + 2)^2 + 2^2
(s + 52 )^3
s + 2 (s + 2)^2 + 3^2
(s + 2)^2 + 3^2
(s + 2)^2 + 2^2
e−^ 25 t t^2 + 2e−^2 t^ cos 3t + 4e−^2 t^ sin 3t +
e−^2 t^ sin 2t =
e−^
(^52) t t^2 + e−^2 t(2 cos 3t + 4 sin 3t +
sin 2t)
Example 3. Determine L−^1 {F }, where (a) F (s) = (^) (s−s1)(^2 −s^26 +2)(s−^47 s+5) , SOLUTION. We begin by finding the partial fraction expantion for F (s). The denominator consists of three linear factors, so the expantion has the form
s^2 − 26 s − 47 (s − 1)(s + 2)(s + 5)
s − 1
s + 2
s + 5
where numbers A, B, and C to be determined.
s^2 − 26 s − 47 (s − 1)(s + 2)(s + 5)
s − 1
s + 2
s + 5
A(s + 2)(s + 5) + B(s − 1)(s + 5) + C(s − 1)(s + 2) (s − 1)(s + 2)(s + 5)
So, we have that
s^2 − 26 s − 47 = A(s + 2)(s + 5) + B(s − 1)(s + 5) + C(s − 1)(s + 2).
We can find A, B, and C plugging s = 1, s = −2, and s = −5 into last equality.
s = 1 : 1 − 26 − 47 = A(1 + 2)(1 + 5), s = −2 : 4 − 26(−2) − 47 = B(− 2 − 1)(−2 + 5), s = −5 : 25 − 26(−5) − 47 = C(− 5 − 1)(−5 + 2).
So, A = −4, B = −1, C = 6. Thus,
s^2 − 26 s − 47 (s − 1)(s + 2)(s + 5)
s − 1
s + 2
s + 5