Laplace Transform
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Revision as of 18:26, 11 January 2010 by
Colby.fullerton
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Standard Form:
F
(
s
)
=
L
{
f
(
t
)
}
=
∫
0
∞
e
−
s
t
f
(
t
)
d
t
{\displaystyle F(s)={\mathcal {L}}\left\{f(t)\right\}=\int _{0}^{\infty }e^{-st}f(t)\,dt}
Sample Functions:
F
(
s
)
=
L
{
1
}
=
∫
0
∞
e
−
s
t
d
t
=
{\displaystyle F(s)={\mathcal {L}}\left\{1\right\}=\int _{0}^{\infty }e^{-st}\,dt=}
1
s
{\displaystyle {\frac {1}{s}}}
F
(
s
)
=
L
{
t
n
}
=
∫
0
∞
e
−
s
t
t
n
d
t
=
{\displaystyle F(s)={\mathcal {L}}\left\{t^{n}\right\}=\int _{0}^{\infty }e^{-st}t^{n}\,dt=}
n
!
s
n
+
1
{\displaystyle {\frac {n!}{s^{n+1}}}}
F
(
s
)
=
L
{
e
a
t
}
=
∫
0
∞
e
−
s
t
e
a
t
d
t
=
{\displaystyle F(s)={\mathcal {L}}\left\{e^{at}\right\}=\int _{0}^{\infty }e^{-st}e^{at}\,dt=}
1
s
−
a
{\displaystyle {\frac {1}{s-a}}}
F
(
s
)
=
L
{
s
i
n
(
ω
t
)
}
=
∫
0
∞
e
−
s
t
s
i
n
(
ω
t
)
d
t
=
{\displaystyle F(s)={\mathcal {L}}\left\{sin(\omega t)\right\}=\int _{0}^{\infty }e^{-st}sin(\omega t)\,dt=}
ω
s
2
+
ω
2
{\displaystyle {\frac {\omega }{s^{2}+\omega ^{2}}}}
F
(
s
)
=
L
{
c
o
s
(
ω
t
)
}
=
∫
0
∞
e
−
s
t
c
o
s
(
ω
t
)
d
t
=
{\displaystyle F(s)={\mathcal {L}}\left\{cos(\omega t)\right\}=\int _{0}^{\infty }e^{-st}cos(\omega t)\,dt=}
s
s
2
+
ω
2
{\displaystyle {\frac {s}{s^{2}+\omega ^{2}}}}
F
(
s
)
=
L
{
t
n
g
(
t
)
}
=
∫
0
∞
e
−
s
t
t
n
g
(
t
)
d
t
=
{\displaystyle F(s)={\mathcal {L}}\left\{t^{n}g(t)\right\}=\int _{0}^{\infty }e^{-st}t^{n}g(t)\,dt=}
(
−
1
)
n
d
n
G
(
s
)
d
s
n
for
n
= 1,2,...
{\displaystyle {\frac {(-1)^{n}d^{n}G(s)}{ds^{n}}}{\mbox{ for}}~n\ {\mbox{= 1,2,...}}}
F
(
s
)
=
L
{
t
s
i
n
(
ω
t
)
}
=
∫
0
∞
e
−
s
t
t
s
i
n
(
ω
t
)
d
t
=
{\displaystyle F(s)={\mathcal {L}}\left\{tsin(\omega t)\right\}=\int _{0}^{\infty }e^{-st}tsin(\omega t)\,dt=}
2
ω
s
(
s
2
+
ω
2
)
2
{\displaystyle {\frac {2\omega s}{(s^{2}+\omega ^{2})^{2}}}}
F
(
s
)
=
L
{
t
c
o
s
(
ω
t
)
}
=
∫
0
∞
e
−
s
t
t
c
o
s
(
ω
t
)
d
t
=
{\displaystyle F(s)={\mathcal {L}}\left\{tcos(\omega t)\right\}=\int _{0}^{\infty }e^{-st}tcos(\omega t)\,dt=}
s
2
−
ω
2
(
s
2
+
ω
2
)
2
{\displaystyle {\frac {s^{2}-\omega ^{2}}{(s^{2}+\omega ^{2})^{2}}}}
F
(
s
)
=
L
{
g
(
t
)
}
=
∫
0
∞
e
−
s
t
g
(
t
)
d
t
=
{\displaystyle F(s)={\mathcal {L}}\left\{g(t)\right\}=\int _{0}^{\infty }e^{-st}g(t)\,dt=}
1
a
G
(
s
a
)
{\displaystyle {\frac {1}{a}}G\left({\frac {s}{a}}\right)}
F
(
s
)
=
L
{
e
a
t
g
(
t
)
}
=
∫
0
∞
e
−
s
t
e
a
t
g
(
t
)
d
t
=
G
(
s
−
a
)
{\displaystyle F(s)={\mathcal {L}}\left\{e^{at}g(t)\right\}=\int _{0}^{\infty }e^{-st}e^{at}g(t)\,dt=G(s-a)}
F
(
s
)
=
L
{
e
a
t
t
n
}
=
∫
0
∞
e
−
s
t
e
a
t
t
n
d
t
=
{\displaystyle F(s)={\mathcal {L}}\left\{e^{at}t^{n}\right\}=\int _{0}^{\infty }e^{-st}e^{at}t^{n}\,dt=}
n
!
(
s
−
a
)
n
+
1
for
n
= 1,2,...
{\displaystyle {\frac {n!}{(s-a)^{n+1}}}{\mbox{ for}}~n\ {\mbox{= 1,2,...}}}
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