Why do we need projection in the definition of the Stokes operator?Do the maximum and minimum values of a...
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Why do we need projection in the definition of the Stokes operator?
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$begingroup$
$DeclareMathOperator{div}{div}$
$defbu{mathbf{u}}$
Let $D$ be the square $[0,1]^2$ and consider the following space:
$$
V:={bu: buin H^2(D)^2, div bu=0, u|_{partial D}=0 }.
$$
Introduce also
$$
H:={bu: buin L^2(D)^2, div bu=0}.
$$
Then the Stokes operator is defined as an operator $Vto H$ as
$$
Abu:=-P_LDeltabu,
$$
where $P_L$ is the projection on $H$.
I don't understand, why the Stokes operator is not equal to minus Laplacian? Indeed, if $buin V$, then $div bu=0$ and thus
$$
div Deltabu=u^1_{xxx}+u^1_{yyx}+u^2_{xxy}+u^2_{yyy}=(u^1_x+u^2_y)_{xx}+(u^1_x+u^2_y)_{yy}=Deltadivbu=0.
$$
In this case, $Delta buin H$ and thus the projection is not needed.
Question: what is wrong in my reasoning? Why the Stokes operator is not equal to Laplacian?
Related question: Can one write explicitly the eigenfunctions of Stokes operator in this simple situation? At least can maybe one bound $lambda_1$, the smallest eigenvalue, from below?
functional-analysis operator-theory orthonormal laplacian
$endgroup$
|
show 6 more comments
$begingroup$
$DeclareMathOperator{div}{div}$
$defbu{mathbf{u}}$
Let $D$ be the square $[0,1]^2$ and consider the following space:
$$
V:={bu: buin H^2(D)^2, div bu=0, u|_{partial D}=0 }.
$$
Introduce also
$$
H:={bu: buin L^2(D)^2, div bu=0}.
$$
Then the Stokes operator is defined as an operator $Vto H$ as
$$
Abu:=-P_LDeltabu,
$$
where $P_L$ is the projection on $H$.
I don't understand, why the Stokes operator is not equal to minus Laplacian? Indeed, if $buin V$, then $div bu=0$ and thus
$$
div Deltabu=u^1_{xxx}+u^1_{yyx}+u^2_{xxy}+u^2_{yyy}=(u^1_x+u^2_y)_{xx}+(u^1_x+u^2_y)_{yy}=Deltadivbu=0.
$$
In this case, $Delta buin H$ and thus the projection is not needed.
Question: what is wrong in my reasoning? Why the Stokes operator is not equal to Laplacian?
Related question: Can one write explicitly the eigenfunctions of Stokes operator in this simple situation? At least can maybe one bound $lambda_1$, the smallest eigenvalue, from below?
functional-analysis operator-theory orthonormal laplacian
$endgroup$
$begingroup$
What are the extra exponents $2$ ($H^2(D)^2$, $L^2(D)^2$)??
$endgroup$
– Ted Shifrin
Mar 14 at 21:47
$begingroup$
@TedShifrin $mathbf{u}=(u_1,u_2)$ is a vector. Each of its 2 coordinates $u_1$ and $u_2$ belongs to $H^2(D)$. Thus, $mathbf{u}in H^2(D)^2$.
$endgroup$
– Oleg
Mar 14 at 21:52
$begingroup$
Oh, I see ... So, offhand, my answer to your question is that you need $C^3$ to interchange partial derivatives, and you don't have $C^3$ functions.
$endgroup$
– Ted Shifrin
Mar 14 at 21:53
$begingroup$
@TedShifrin Then why in the periodic case (periodic boundary conditions) the Stokes operator is equal to Laplacian?
$endgroup$
– Oleg
Mar 14 at 22:01
$begingroup$
Hint: In the definition of $H$, in what sense is the divergence equal to zero?
$endgroup$
– maxmilgram
Mar 15 at 17:42
|
show 6 more comments
$begingroup$
$DeclareMathOperator{div}{div}$
$defbu{mathbf{u}}$
Let $D$ be the square $[0,1]^2$ and consider the following space:
$$
V:={bu: buin H^2(D)^2, div bu=0, u|_{partial D}=0 }.
$$
Introduce also
$$
H:={bu: buin L^2(D)^2, div bu=0}.
$$
Then the Stokes operator is defined as an operator $Vto H$ as
$$
Abu:=-P_LDeltabu,
$$
where $P_L$ is the projection on $H$.
I don't understand, why the Stokes operator is not equal to minus Laplacian? Indeed, if $buin V$, then $div bu=0$ and thus
$$
div Deltabu=u^1_{xxx}+u^1_{yyx}+u^2_{xxy}+u^2_{yyy}=(u^1_x+u^2_y)_{xx}+(u^1_x+u^2_y)_{yy}=Deltadivbu=0.
$$
In this case, $Delta buin H$ and thus the projection is not needed.
Question: what is wrong in my reasoning? Why the Stokes operator is not equal to Laplacian?
Related question: Can one write explicitly the eigenfunctions of Stokes operator in this simple situation? At least can maybe one bound $lambda_1$, the smallest eigenvalue, from below?
functional-analysis operator-theory orthonormal laplacian
$endgroup$
$DeclareMathOperator{div}{div}$
$defbu{mathbf{u}}$
Let $D$ be the square $[0,1]^2$ and consider the following space:
$$
V:={bu: buin H^2(D)^2, div bu=0, u|_{partial D}=0 }.
$$
Introduce also
$$
H:={bu: buin L^2(D)^2, div bu=0}.
$$
Then the Stokes operator is defined as an operator $Vto H$ as
$$
Abu:=-P_LDeltabu,
$$
where $P_L$ is the projection on $H$.
I don't understand, why the Stokes operator is not equal to minus Laplacian? Indeed, if $buin V$, then $div bu=0$ and thus
$$
div Deltabu=u^1_{xxx}+u^1_{yyx}+u^2_{xxy}+u^2_{yyy}=(u^1_x+u^2_y)_{xx}+(u^1_x+u^2_y)_{yy}=Deltadivbu=0.
$$
In this case, $Delta buin H$ and thus the projection is not needed.
Question: what is wrong in my reasoning? Why the Stokes operator is not equal to Laplacian?
Related question: Can one write explicitly the eigenfunctions of Stokes operator in this simple situation? At least can maybe one bound $lambda_1$, the smallest eigenvalue, from below?
functional-analysis operator-theory orthonormal laplacian
functional-analysis operator-theory orthonormal laplacian
edited Mar 15 at 14:42
Oleg
asked Mar 14 at 21:37
OlegOleg
301212
301212
$begingroup$
What are the extra exponents $2$ ($H^2(D)^2$, $L^2(D)^2$)??
$endgroup$
– Ted Shifrin
Mar 14 at 21:47
$begingroup$
@TedShifrin $mathbf{u}=(u_1,u_2)$ is a vector. Each of its 2 coordinates $u_1$ and $u_2$ belongs to $H^2(D)$. Thus, $mathbf{u}in H^2(D)^2$.
$endgroup$
– Oleg
Mar 14 at 21:52
$begingroup$
Oh, I see ... So, offhand, my answer to your question is that you need $C^3$ to interchange partial derivatives, and you don't have $C^3$ functions.
$endgroup$
– Ted Shifrin
Mar 14 at 21:53
$begingroup$
@TedShifrin Then why in the periodic case (periodic boundary conditions) the Stokes operator is equal to Laplacian?
$endgroup$
– Oleg
Mar 14 at 22:01
$begingroup$
Hint: In the definition of $H$, in what sense is the divergence equal to zero?
$endgroup$
– maxmilgram
Mar 15 at 17:42
|
show 6 more comments
$begingroup$
What are the extra exponents $2$ ($H^2(D)^2$, $L^2(D)^2$)??
$endgroup$
– Ted Shifrin
Mar 14 at 21:47
$begingroup$
@TedShifrin $mathbf{u}=(u_1,u_2)$ is a vector. Each of its 2 coordinates $u_1$ and $u_2$ belongs to $H^2(D)$. Thus, $mathbf{u}in H^2(D)^2$.
$endgroup$
– Oleg
Mar 14 at 21:52
$begingroup$
Oh, I see ... So, offhand, my answer to your question is that you need $C^3$ to interchange partial derivatives, and you don't have $C^3$ functions.
$endgroup$
– Ted Shifrin
Mar 14 at 21:53
$begingroup$
@TedShifrin Then why in the periodic case (periodic boundary conditions) the Stokes operator is equal to Laplacian?
$endgroup$
– Oleg
Mar 14 at 22:01
$begingroup$
Hint: In the definition of $H$, in what sense is the divergence equal to zero?
$endgroup$
– maxmilgram
Mar 15 at 17:42
$begingroup$
What are the extra exponents $2$ ($H^2(D)^2$, $L^2(D)^2$)??
$endgroup$
– Ted Shifrin
Mar 14 at 21:47
$begingroup$
What are the extra exponents $2$ ($H^2(D)^2$, $L^2(D)^2$)??
$endgroup$
– Ted Shifrin
Mar 14 at 21:47
$begingroup$
@TedShifrin $mathbf{u}=(u_1,u_2)$ is a vector. Each of its 2 coordinates $u_1$ and $u_2$ belongs to $H^2(D)$. Thus, $mathbf{u}in H^2(D)^2$.
$endgroup$
– Oleg
Mar 14 at 21:52
$begingroup$
@TedShifrin $mathbf{u}=(u_1,u_2)$ is a vector. Each of its 2 coordinates $u_1$ and $u_2$ belongs to $H^2(D)$. Thus, $mathbf{u}in H^2(D)^2$.
$endgroup$
– Oleg
Mar 14 at 21:52
$begingroup$
Oh, I see ... So, offhand, my answer to your question is that you need $C^3$ to interchange partial derivatives, and you don't have $C^3$ functions.
$endgroup$
– Ted Shifrin
Mar 14 at 21:53
$begingroup$
Oh, I see ... So, offhand, my answer to your question is that you need $C^3$ to interchange partial derivatives, and you don't have $C^3$ functions.
$endgroup$
– Ted Shifrin
Mar 14 at 21:53
$begingroup$
@TedShifrin Then why in the periodic case (periodic boundary conditions) the Stokes operator is equal to Laplacian?
$endgroup$
– Oleg
Mar 14 at 22:01
$begingroup$
@TedShifrin Then why in the periodic case (periodic boundary conditions) the Stokes operator is equal to Laplacian?
$endgroup$
– Oleg
Mar 14 at 22:01
$begingroup$
Hint: In the definition of $H$, in what sense is the divergence equal to zero?
$endgroup$
– maxmilgram
Mar 15 at 17:42
$begingroup$
Hint: In the definition of $H$, in what sense is the divergence equal to zero?
$endgroup$
– maxmilgram
Mar 15 at 17:42
|
show 6 more comments
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$begingroup$
What are the extra exponents $2$ ($H^2(D)^2$, $L^2(D)^2$)??
$endgroup$
– Ted Shifrin
Mar 14 at 21:47
$begingroup$
@TedShifrin $mathbf{u}=(u_1,u_2)$ is a vector. Each of its 2 coordinates $u_1$ and $u_2$ belongs to $H^2(D)$. Thus, $mathbf{u}in H^2(D)^2$.
$endgroup$
– Oleg
Mar 14 at 21:52
$begingroup$
Oh, I see ... So, offhand, my answer to your question is that you need $C^3$ to interchange partial derivatives, and you don't have $C^3$ functions.
$endgroup$
– Ted Shifrin
Mar 14 at 21:53
$begingroup$
@TedShifrin Then why in the periodic case (periodic boundary conditions) the Stokes operator is equal to Laplacian?
$endgroup$
– Oleg
Mar 14 at 22:01
$begingroup$
Hint: In the definition of $H$, in what sense is the divergence equal to zero?
$endgroup$
– maxmilgram
Mar 15 at 17:42