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Why do we need projection in the definition of the Stokes operator?


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1












$begingroup$


$DeclareMathOperator{div}{div}$
$defbu{mathbf{u}}$
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?










share|cite|improve this question











$endgroup$












  • $begingroup$
    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
















1












$begingroup$


$DeclareMathOperator{div}{div}$
$defbu{mathbf{u}}$
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?










share|cite|improve this question











$endgroup$












  • $begingroup$
    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














1












1








1


1



$begingroup$


$DeclareMathOperator{div}{div}$
$defbu{mathbf{u}}$
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?










share|cite|improve this question











$endgroup$




$DeclareMathOperator{div}{div}$
$defbu{mathbf{u}}$
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






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








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


















  • $begingroup$
    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










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