Environmental Engineering Reference
In-Depth Information
f
(
s
)
is called the image function of f
(
t
)
.
The Laplace transformation of f
(
t
)
with t
(
0
, + )
as defined by Eq. (B.23) is
e β t
actually the Fourier transformation of f
(
t
)
I
(
t
)
(for
β >
0). Thus we have, by
the Fourier integral,
+
e t d
+
1
2
e β t
e βτ e t d
f
(
t
)
I
(
t
)
=
f
( τ )
I
( τ )
τ
ω
π
e t
+
+
1
2
e ( β + ) τ d
d
=
f
( τ )
τ
ω
π
0
+
1
2
f
e t d
=
(
s
)
ω ,
t
>
0
,
π
where s
= β +
i
ω
. Thus
+
β + i
1
2
1
2
f
e ( + β ) t d
f
e st d s
f
(
t
)=
(
s
)
ω =
(
s
)
,
(B.24)
π
π
i
β
i
which is called the inverse Laplace transformation and denoted by
L 1 f
) .
f
(
t
)=
(
s
f
The f
(
t
)
is called the inverse image function of
(
s
)
.
f
Therefore we may find
(
s
)
by Eq. (B.23) and f
(
t
)
by Eq. (B.24) from the
f
known f
. The integral in Eq. (B.23) is a regular integral. The integral
in Eq. (B.24) is however an integral of a complex-valued function and is normally
obtained by using the residue theorem which will be given in Section B.2.3.
Example 1 . Find the Laplace transformation of the unit function I
(
t
)
or
(
s
)
(
t
)
.
Solution. By Eq. (B.23),
+
e st +
0
1
s
1
s .
e st d t
L
[
I
(
t
)] =
=
=
0
Its convergence domain is Re
(
s
) >
0. Thus
1
s ,
L
[
I
(
t
)] =
Re
(
s
) >
0
.
Example 2. Find the Laplace transformation of the exponential function e α t ,where
α
is a real constant.
Solution. When Re
(
) >
s
0, by Eq. (B.23) we have
+
+
L e α t =
1
e α t e st d t
e ( s α ) t d t
=
=
α .
s
0
0
Example 3. Find the Laplace transformation of
δ (
t
)
.
 
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