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Global estimates for mixed methods for second order elliptic equations
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Global error estimates in
L
2
(
Ω
)
{L^2}(\Omega )
,
L
∞
(
Ω
)
{L^\infty }(\Omega )
, and
H
−
s
(
Ω
)
{H^{ - s}}(\Omega )
,
Ω
\Omega
in
R
2
{{\mathbf {R}}^2}
or
R
3
{{\mathbf {R}}^3}
, are derived for a mixed finite element method for the Dirichlet problem for the elliptic operator
L
p
=
−
div
(
a
g
r
a
d
p
+
b
p
)
+
c
p
Lp = - \operatorname {div}(a\;{\mathbf {grad}}\;p + {\mathbf {b}}p) + cp
based on the Raviart-Thomas-Nedelec space
V
h
×
W
h
⊂
H
(
div
;
Ω
)
×
L
2
(
Ω
)
{{\mathbf {V}}_h} \times {W_h} \subset {\mathbf {H}}(\operatorname {div};\Omega ) \times {L^2}(\Omega )
. Optimal order estimates are obtained for the approximation of
p
and the associated velocity field
u
=
−
(
a
g
r
a
d
p
+
b
p
)
{\mathbf {u}} = - (a\;{\mathbf {grad}}\;p + {\mathbf {b}}p)
in
L
2
(
Ω
)
{L^2}(\Omega )
and
H
−
s
(
Ω
)
{H^{ - s}}(\Omega )
,
0
⩽
s
⩽
k
+
1
0 \leqslant s \leqslant k + 1
, and, if
Ω
⊂
R
2
\Omega \subset {{\mathbf {R}}^2}
for
p
in
L
∞
(
Ω
)
{L^\infty }(\Omega )
.
Title: Global estimates for mixed methods for second order elliptic equations
Description:
Global error estimates in
L
2
(
Ω
)
{L^2}(\Omega )
,
L
∞
(
Ω
)
{L^\infty }(\Omega )
, and
H
−
s
(
Ω
)
{H^{ - s}}(\Omega )
,
Ω
\Omega
in
R
2
{{\mathbf {R}}^2}
or
R
3
{{\mathbf {R}}^3}
, are derived for a mixed finite element method for the Dirichlet problem for the elliptic operator
L
p
=
−
div
(
a
g
r
a
d
p
+
b
p
)
+
c
p
Lp = - \operatorname {div}(a\;{\mathbf {grad}}\;p + {\mathbf {b}}p) + cp
based on the Raviart-Thomas-Nedelec space
V
h
×
W
h
⊂
H
(
div
;
Ω
)
×
L
2
(
Ω
)
{{\mathbf {V}}_h} \times {W_h} \subset {\mathbf {H}}(\operatorname {div};\Omega ) \times {L^2}(\Omega )
.
Optimal order estimates are obtained for the approximation of
p
and the associated velocity field
u
=
−
(
a
g
r
a
d
p
+
b
p
)
{\mathbf {u}} = - (a\;{\mathbf {grad}}\;p + {\mathbf {b}}p)
in
L
2
(
Ω
)
{L^2}(\Omega )
and
H
−
s
(
Ω
)
{H^{ - s}}(\Omega )
,
0
⩽
s
⩽
k
+
1
0 \leqslant s \leqslant k + 1
, and, if
Ω
⊂
R
2
\Omega \subset {{\mathbf {R}}^2}
for
p
in
L
∞
(
Ω
)
{L^\infty }(\Omega )
.
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