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Define the weighted Sobolev space
(G)
·
ρ
,
C
0
W
ρ
=
(4.20)
where the weighted Sobolev norm
·
ρ
is defined by
R
2
(s
2
ρ
2
2
)
d
s,
ρ
:=
|
|
+|
|
≤
≤
ϕ
∂
s
ϕ
ϕ
0
ρ
1
.
(4.21)
0
C
0
For
ϕ,φ
∈
(G)
, we define the bilinear form
2
σ
2
s
2
ρ
∂
s
ϕ∂
s
φ
d
s
+
ρσ
2
R
R
1
a
CEV
ρ
s
2
ρ
−
1
∂
s
ϕφ
d
s
(ϕ, φ)
:=
0
0
r
r
R
R
−
s∂
s
ϕφ
d
s
+
ϕφ
d
s.
(4.22)
0
0
The variational formulation of (
4.19
) is based on the triple of spaces
V
=
W
ρ
→
L
2
(G)
=
H
∗
W
ρ
=
V
∗
, and reads:
H
=
→
L
2
(J
H
1
(J
L
2
(G))
such that
Find
v
∈
;
W
ρ
)
∩
;
a
CEV
+
=
∀
∈
(∂
t
v,w)
(v, w)
0
,
w
W
ρ
,
a.e. in
J,
(4.23)
ρ
v(
0
)
=
g.
To establish well-posedness of (
4.23
), we show continuity and coercivity of the
bilinear form
a
CEV
ρ
(
·
,
·
)
on
W
ρ
.
Proposition 4.5.1
Assume r>
0.
There exist C
1
,C
2
>
0
such that for ϕ,φ
∈
W
ρ
a
CEV
ρ
|
(ϕ, φ)
|≤
C
1
ϕ
ρ
φ
ρ
,ρ
∈[
0
,
1
]\{
1
/
2
}
,
(4.24)
1
2
.
a
CEV
2
(ϕ, ϕ)
≥
C
2
ϕ
ρ
,
0
≤
ρ
≤
(4.25)
ρ
C
0
Proof
Let
ϕ
∈
(G)
. By Hardy's inequality, for
ε
=
1,
ε>
0, and any
R>
0
2
d
s
2
d
s
R
1
2
R
1
2
2
s
ε
−
2
s
ε
|
ϕ
|
≤
|
∂
s
ϕ
|
,
(4.26)
|
−
|
ε
1
0
0
we find with
ε
=
2
ρ
=
1, that
2
s
2
ρ
−
1
∂
s
ϕφ
d
s
≤
s
2
ρ
(∂
s
ϕ)
2
d
s
s
2
ρ
−
2
φ
2
d
s
R
R
1
R
1
2
0
0
0
2
≤
ϕ
ρ
|
φ
ρ
|
2
ρ
−
1
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