Neumann problem with zero average sobolev space












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Let us considère the following Laplace-Neumann problem $-Delta u=0$ with homogenuous boundary condition of type neumann, i:e $frac{{partial u}}{{partial n}} = 0$.
The variational formulation is given as follows $a(u,v)=l(v)$, where $$a(u,v) = int_Omega {nabla unabla v} dx = 0$$ and $l(v)=0$.
Let us cinsidère the space
$$left{ V={u in H^1(Omega), int_Omega v(x)ds=0} right}$$
$l$ is continuous ( is zero), and $a$ is continuous and corecive. By lax-Milgram theoremn there exists a unique solution of the variational problem $$a(u,v)=l(v)$$. We can notice that the constant are alos solutions of the problem, but the constants don't satisfy the zero average condition, I don't understand that.










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    Let us considère the following Laplace-Neumann problem $-Delta u=0$ with homogenuous boundary condition of type neumann, i:e $frac{{partial u}}{{partial n}} = 0$.
    The variational formulation is given as follows $a(u,v)=l(v)$, where $$a(u,v) = int_Omega {nabla unabla v} dx = 0$$ and $l(v)=0$.
    Let us cinsidère the space
    $$left{ V={u in H^1(Omega), int_Omega v(x)ds=0} right}$$
    $l$ is continuous ( is zero), and $a$ is continuous and corecive. By lax-Milgram theoremn there exists a unique solution of the variational problem $$a(u,v)=l(v)$$. We can notice that the constant are alos solutions of the problem, but the constants don't satisfy the zero average condition, I don't understand that.










    share|cite|improve this question









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      $begingroup$


      Let us considère the following Laplace-Neumann problem $-Delta u=0$ with homogenuous boundary condition of type neumann, i:e $frac{{partial u}}{{partial n}} = 0$.
      The variational formulation is given as follows $a(u,v)=l(v)$, where $$a(u,v) = int_Omega {nabla unabla v} dx = 0$$ and $l(v)=0$.
      Let us cinsidère the space
      $$left{ V={u in H^1(Omega), int_Omega v(x)ds=0} right}$$
      $l$ is continuous ( is zero), and $a$ is continuous and corecive. By lax-Milgram theoremn there exists a unique solution of the variational problem $$a(u,v)=l(v)$$. We can notice that the constant are alos solutions of the problem, but the constants don't satisfy the zero average condition, I don't understand that.










      share|cite|improve this question









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      Let us considère the following Laplace-Neumann problem $-Delta u=0$ with homogenuous boundary condition of type neumann, i:e $frac{{partial u}}{{partial n}} = 0$.
      The variational formulation is given as follows $a(u,v)=l(v)$, where $$a(u,v) = int_Omega {nabla unabla v} dx = 0$$ and $l(v)=0$.
      Let us cinsidère the space
      $$left{ V={u in H^1(Omega), int_Omega v(x)ds=0} right}$$
      $l$ is continuous ( is zero), and $a$ is continuous and corecive. By lax-Milgram theoremn there exists a unique solution of the variational problem $$a(u,v)=l(v)$$. We can notice that the constant are alos solutions of the problem, but the constants don't satisfy the zero average condition, I don't understand that.







      pde laplacian elliptic-equations variational-analysis






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      asked Dec 2 '18 at 11:04









      GustaveGustave

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          In your case the problem is $-Delta u = 0$ subject to $frac{partial u}{partial n} = 0,$ which only has trivial solutions. Indeed if $u$ is such a solution with zero average $int_{Omega} u ,mathrm{d}x = 0,$ since $a(u,u) = int_{Omega} |nabla u|^2,mathrm{d}x = 0$ we conclude that $u$ is a.e. constant and hence zero as it has zero average.



          So the solution $u equiv 0$ is the unique solution subject to the zero average condition. The other constant solutions $u equiv k neq 0$ are also solutions, but they don't satisfy the zero average condition. I assume this is what is meant here.



          For a non-homogenous problem $-Delta u = f$, we get $ell(v) = int_{Omega} fv ,mathrm{d}x$ is non-trivial and hence we get non-trivial solutions. However if $u$ is a solution, then so is $u+k$ for any constant $k.$ The zero average condition removes this extra degree of freedom.






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            $begingroup$

            In your case the problem is $-Delta u = 0$ subject to $frac{partial u}{partial n} = 0,$ which only has trivial solutions. Indeed if $u$ is such a solution with zero average $int_{Omega} u ,mathrm{d}x = 0,$ since $a(u,u) = int_{Omega} |nabla u|^2,mathrm{d}x = 0$ we conclude that $u$ is a.e. constant and hence zero as it has zero average.



            So the solution $u equiv 0$ is the unique solution subject to the zero average condition. The other constant solutions $u equiv k neq 0$ are also solutions, but they don't satisfy the zero average condition. I assume this is what is meant here.



            For a non-homogenous problem $-Delta u = f$, we get $ell(v) = int_{Omega} fv ,mathrm{d}x$ is non-trivial and hence we get non-trivial solutions. However if $u$ is a solution, then so is $u+k$ for any constant $k.$ The zero average condition removes this extra degree of freedom.






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              $begingroup$

              In your case the problem is $-Delta u = 0$ subject to $frac{partial u}{partial n} = 0,$ which only has trivial solutions. Indeed if $u$ is such a solution with zero average $int_{Omega} u ,mathrm{d}x = 0,$ since $a(u,u) = int_{Omega} |nabla u|^2,mathrm{d}x = 0$ we conclude that $u$ is a.e. constant and hence zero as it has zero average.



              So the solution $u equiv 0$ is the unique solution subject to the zero average condition. The other constant solutions $u equiv k neq 0$ are also solutions, but they don't satisfy the zero average condition. I assume this is what is meant here.



              For a non-homogenous problem $-Delta u = f$, we get $ell(v) = int_{Omega} fv ,mathrm{d}x$ is non-trivial and hence we get non-trivial solutions. However if $u$ is a solution, then so is $u+k$ for any constant $k.$ The zero average condition removes this extra degree of freedom.






              share|cite|improve this answer









              $endgroup$
















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                1





                $begingroup$

                In your case the problem is $-Delta u = 0$ subject to $frac{partial u}{partial n} = 0,$ which only has trivial solutions. Indeed if $u$ is such a solution with zero average $int_{Omega} u ,mathrm{d}x = 0,$ since $a(u,u) = int_{Omega} |nabla u|^2,mathrm{d}x = 0$ we conclude that $u$ is a.e. constant and hence zero as it has zero average.



                So the solution $u equiv 0$ is the unique solution subject to the zero average condition. The other constant solutions $u equiv k neq 0$ are also solutions, but they don't satisfy the zero average condition. I assume this is what is meant here.



                For a non-homogenous problem $-Delta u = f$, we get $ell(v) = int_{Omega} fv ,mathrm{d}x$ is non-trivial and hence we get non-trivial solutions. However if $u$ is a solution, then so is $u+k$ for any constant $k.$ The zero average condition removes this extra degree of freedom.






                share|cite|improve this answer









                $endgroup$



                In your case the problem is $-Delta u = 0$ subject to $frac{partial u}{partial n} = 0,$ which only has trivial solutions. Indeed if $u$ is such a solution with zero average $int_{Omega} u ,mathrm{d}x = 0,$ since $a(u,u) = int_{Omega} |nabla u|^2,mathrm{d}x = 0$ we conclude that $u$ is a.e. constant and hence zero as it has zero average.



                So the solution $u equiv 0$ is the unique solution subject to the zero average condition. The other constant solutions $u equiv k neq 0$ are also solutions, but they don't satisfy the zero average condition. I assume this is what is meant here.



                For a non-homogenous problem $-Delta u = f$, we get $ell(v) = int_{Omega} fv ,mathrm{d}x$ is non-trivial and hence we get non-trivial solutions. However if $u$ is a solution, then so is $u+k$ for any constant $k.$ The zero average condition removes this extra degree of freedom.







                share|cite|improve this answer












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                share|cite|improve this answer










                answered Dec 4 '18 at 20:11









                ktoiktoi

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                2,4061617






























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