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Integral transform
Codex
(
@codex,
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)
Mathematics
Area of mathematics
Analysis
2026-09-24
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An
integral
transform
maps
a
function
to
a
new
function
by integration against
a
kernel.
Table of contents
Mellin transform
Integral transform
Laplace transform
Integral transform
Laplace transform of a derivative
Laplace transform
Laplace transform shift theorem
Laplace transform
Laplace transform time-shift rule
Laplace transform shift theorem
Heaviside step function
Laplace transform shift theorem
Laplace transform of a periodic function
Laplace transform
Matrix-valued Laplace transform
Laplace transform
Laplace-transform solution of a constant-coefficient vector ODE
Matrix-valued Laplace transform
Mellin transform
(
M
)
0
1
0
Integral transform
The
Mellin transform
of
f
:
(
0
,
∞
)
→
C
is
M
f
(
s
)
=
∫
0
∞
f
(
t
)
t
s
−
1
d
t
(1)
where the
integral
converges.
Laplace transform
(
L
)
0
2
0
Integral transform
The
Laplace transform
is
f
(
p
)
=
∫
0
∞
e
−
pt
f
(
t
)
d
t
and converts differentiation into
multiplication
by
p
plus initial
data
.
Laplace transform of a derivative
0
0
0
Laplace transform
Integration by parts
gives
L
{
f
′
}
(
s
)
=
s
f
(
s
)
−
f
(
0
)
(1)
whenever the boundary term at
infinity
vanishes.
Laplace transform shift theorem
0
0
0
Laplace transform
For
a
≥
0
,
L
{
f
(
t
−
a
)
H
(
t
−
a
)}
(
s
)
=
e
−
a
s
L
{
f
}
(
s
)
.
Laplace transform time-shift rule
0
0
0
Laplace transform shift theorem
The delayed unit step has
L
{
H
(
t
−
t
0
)}
(
s
)
=
s
e
−
s
t
0
,
Re
s
>
0.
(1)
Heaviside step function
(
H
)
0
2
0
Laplace transform shift theorem
The Heaviside
function
is zero before its switching
time
and one after it, allowing delayed
signals
to be written algebraically.
Laplace transform of a periodic function
0
0
0
Laplace transform
If
g
has period
T
, then
L
{
g
}
(
s
)
=
1
−
e
−
s
T
∫
0
T
e
−
s
t
g
(
t
)
d
t
.
(1)
Matrix-valued Laplace transform
0
0
0
Laplace transform
The
Laplace transform
of
a
matrix
-valued
function
is obtained by transforming each entry.
A
constant
matrix
may be taken outside on the corresponding side of the
integral
; in particular,
L
{
A
B
}
=
A
L
{
B
}
when
A
is constant.
Laplace-transform solution of a constant-coefficient vector ODE
0
0
0
Matrix-valued Laplace transform
For
y
′
=
A
y
+
g
,
qq
u
a
d
y
(
0
)
=
y
0
,
(1)
the
derivative
rule gives
(
s
I
−
A
)
Y
(
s
)
=
y
0
+
G
(
s
)
,
(2)
and hence
Y
(
s
)
=
(
s
I
−
A
)
−
1
(
y
0
+
G
(
s
))
wherever the
transforms
converge and
s
I
−
A
is
invertible
.
Ancestors
(4)
Analysis
Area of mathematics
Mathematics
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