Environmental Engineering Reference
In-Depth Information
into
a 2 v xx
a 2 w xx
v tt
=
+
w tt
,
(
0
,
l
) × (
0
, + ) ,
v
(
0
,
t
)=
v
(
l
,
t
)=
0
,
v
(
x
,
0
)= ϕ (
x
)
w
(
x
,
0
) ,
v t
(
x
,
0
)=
w t
(
x
,
0
) .
Therefore, it is of crucial importance to have a function w
satisfying the nonho-
mogeneous boundary conditions. Such kinds of auxiliary functions depend on the
type of boundary conditions. Here we list such auxiliary functions for three typical
kinds of boundary conditions
(
x
,
t
)
1. w
(
x
,
t
)=
xf 2 (
t
)+
f 1 (
t
)
for
u
(
0
,
t
)=
f 1 (
t
)
, u x (
l
,
t
)=
f 2 (
t
)
;
2. w
(
x
,
t
)=(
x
l
)
f 1 (
t
)+
f 2 (
t
)
for
u x (
0
,
t
)=
f 1 (
t
)
, u
(
l
,
t
)=
f 2 (
t
)
;
f 2
(
t
)
f 1
(
t
)
x 2
3. w
(
x
,
t
)=
+
f 1 (
t
)
x
for
u x (
0
,
t
)=
f 1 (
t
)
, u x (
l
,
t
)=
f 2 (
t
)
.
2 l
For the case of u
(
0
,
t
)=
0, u
(
l
,
t
)=
A sin
ω
t , both
sin ω
x
a
sin ω
Ax
l
w 1 (
x
,
t
)=
sin
ω
t
and w 2 (
x
,
t
)=
A
sin
ω
t
l
a
can serve as the auxiliary function of homogenization. As a 2 w xx
w tt =
0, however,
(
,
)
the function transformation using w 2
as the auxiliary function will not change
the source term of the equation and is thus more desirable. Such a transformation
can preserve the homogenenity of the original equation.
Remark 2. To understand the Green function, we must discuss the Dirac function,
or
x
t
-function can be
found in Appendix B. Here, we introduce it from the point of view of physics and
engineering.
The
δ
-function for short. A precise mathematical discussion of the
δ
δ
-function is often called the unit impulse function and is defined by
0
+
,
=
,
x
x 0
δ (
x
x 0 )=
δ (
x
x 0 )
d x
=
1
.
,
=
,
x
x 0
Its introduction comes from the desire to describe some localized phenomena. For
example, consider an infinite wire (
) with all the charges of unit quan-
tity of electricity located at point x 0 . The charge density
<
x
< +
ρ (
x
x 0 )
satisfies
0
+
,
x
=
x 0
,
ρ (
x
x 0
)=
ρ (
x
x 0
)
d x
=
1
.
,
x
=
x 0
,
 
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