Laplace equation with the Robin's boundary problem












0












$begingroup$



$textbf{Problem}$ Let $Omega$ be an open, bounded and connected subset of $mathbb{R}^n$. Suppose that $partial Omega$ is $C^{infty}$. Consider an eigenvalue problem
begin{align*}
begin{cases}
-Delta u=lambda u & textrm{ in } ; Omega \
frac{partial u}{partial nu}=-u & textrm{ on } partial Omega
end{cases}
end{align*}

Define a bilinear operater $(cdot,cdot)_{H^1}$ by
begin{align*}
(u,v)_{H^1}:=int_{Omega} nabla u cdot nabla v ;dx + int_{partial Omega} uv ; dsigma
end{align*}

Show that there exists a constant $theta>0$ independent of $u,v$ such that
begin{align*}
(u,u)_{H^1} geq theta Vert u Vert _{H^1(Omega)}^2
end{align*}




$textbf{Attempt}$



begin{align*}
(u,u)_{H^1}&=int_{Omega} nabla u cdot nabla u ;dx + int_{partial Omega} u^2 ; dsigma \
&=int_{Omega} nabla cdot(unabla u)-uDelta u ; dx +int_{partial Omega} u^2 ; dsigma \
&=int_{partial Omega} u frac{partial u}{partial nu} ; dsigma +int_{Omega} lambda u^2 dx +int_{partial Omega} u^2 ; dsigma \
&=-int_{partial Omega} u^2 ; dsigma +int_{Omega} lambda u^2 dx +int_{partial Omega} u^2 ; dsigma\
&=lambda Vert u Vert _{L^2(Omega)}^2
end{align*}

I don't know how to get $lambda Vert u Vert_{L^2(Omega)}^2 geq theta Vert u Vert_{H^1(Omega)}^2$...



Any help is appreciated..



Thank you!










share|cite|improve this question









$endgroup$












  • $begingroup$
    What is the connection between the taks 'Show that...' and the eigenvalue problem? As it is stated now, there is no connection, and it looks like the inequality has to be proven for all $uin H^1$.
    $endgroup$
    – daw
    Dec 10 '18 at 14:19










  • $begingroup$
    If I prove the problem, then I'll get every eigenvalue is a positive real number.
    $endgroup$
    – w.sdka
    Dec 10 '18 at 14:22
















0












$begingroup$



$textbf{Problem}$ Let $Omega$ be an open, bounded and connected subset of $mathbb{R}^n$. Suppose that $partial Omega$ is $C^{infty}$. Consider an eigenvalue problem
begin{align*}
begin{cases}
-Delta u=lambda u & textrm{ in } ; Omega \
frac{partial u}{partial nu}=-u & textrm{ on } partial Omega
end{cases}
end{align*}

Define a bilinear operater $(cdot,cdot)_{H^1}$ by
begin{align*}
(u,v)_{H^1}:=int_{Omega} nabla u cdot nabla v ;dx + int_{partial Omega} uv ; dsigma
end{align*}

Show that there exists a constant $theta>0$ independent of $u,v$ such that
begin{align*}
(u,u)_{H^1} geq theta Vert u Vert _{H^1(Omega)}^2
end{align*}




$textbf{Attempt}$



begin{align*}
(u,u)_{H^1}&=int_{Omega} nabla u cdot nabla u ;dx + int_{partial Omega} u^2 ; dsigma \
&=int_{Omega} nabla cdot(unabla u)-uDelta u ; dx +int_{partial Omega} u^2 ; dsigma \
&=int_{partial Omega} u frac{partial u}{partial nu} ; dsigma +int_{Omega} lambda u^2 dx +int_{partial Omega} u^2 ; dsigma \
&=-int_{partial Omega} u^2 ; dsigma +int_{Omega} lambda u^2 dx +int_{partial Omega} u^2 ; dsigma\
&=lambda Vert u Vert _{L^2(Omega)}^2
end{align*}

I don't know how to get $lambda Vert u Vert_{L^2(Omega)}^2 geq theta Vert u Vert_{H^1(Omega)}^2$...



Any help is appreciated..



Thank you!










share|cite|improve this question









$endgroup$












  • $begingroup$
    What is the connection between the taks 'Show that...' and the eigenvalue problem? As it is stated now, there is no connection, and it looks like the inequality has to be proven for all $uin H^1$.
    $endgroup$
    – daw
    Dec 10 '18 at 14:19










  • $begingroup$
    If I prove the problem, then I'll get every eigenvalue is a positive real number.
    $endgroup$
    – w.sdka
    Dec 10 '18 at 14:22














0












0








0





$begingroup$



$textbf{Problem}$ Let $Omega$ be an open, bounded and connected subset of $mathbb{R}^n$. Suppose that $partial Omega$ is $C^{infty}$. Consider an eigenvalue problem
begin{align*}
begin{cases}
-Delta u=lambda u & textrm{ in } ; Omega \
frac{partial u}{partial nu}=-u & textrm{ on } partial Omega
end{cases}
end{align*}

Define a bilinear operater $(cdot,cdot)_{H^1}$ by
begin{align*}
(u,v)_{H^1}:=int_{Omega} nabla u cdot nabla v ;dx + int_{partial Omega} uv ; dsigma
end{align*}

Show that there exists a constant $theta>0$ independent of $u,v$ such that
begin{align*}
(u,u)_{H^1} geq theta Vert u Vert _{H^1(Omega)}^2
end{align*}




$textbf{Attempt}$



begin{align*}
(u,u)_{H^1}&=int_{Omega} nabla u cdot nabla u ;dx + int_{partial Omega} u^2 ; dsigma \
&=int_{Omega} nabla cdot(unabla u)-uDelta u ; dx +int_{partial Omega} u^2 ; dsigma \
&=int_{partial Omega} u frac{partial u}{partial nu} ; dsigma +int_{Omega} lambda u^2 dx +int_{partial Omega} u^2 ; dsigma \
&=-int_{partial Omega} u^2 ; dsigma +int_{Omega} lambda u^2 dx +int_{partial Omega} u^2 ; dsigma\
&=lambda Vert u Vert _{L^2(Omega)}^2
end{align*}

I don't know how to get $lambda Vert u Vert_{L^2(Omega)}^2 geq theta Vert u Vert_{H^1(Omega)}^2$...



Any help is appreciated..



Thank you!










share|cite|improve this question









$endgroup$





$textbf{Problem}$ Let $Omega$ be an open, bounded and connected subset of $mathbb{R}^n$. Suppose that $partial Omega$ is $C^{infty}$. Consider an eigenvalue problem
begin{align*}
begin{cases}
-Delta u=lambda u & textrm{ in } ; Omega \
frac{partial u}{partial nu}=-u & textrm{ on } partial Omega
end{cases}
end{align*}

Define a bilinear operater $(cdot,cdot)_{H^1}$ by
begin{align*}
(u,v)_{H^1}:=int_{Omega} nabla u cdot nabla v ;dx + int_{partial Omega} uv ; dsigma
end{align*}

Show that there exists a constant $theta>0$ independent of $u,v$ such that
begin{align*}
(u,u)_{H^1} geq theta Vert u Vert _{H^1(Omega)}^2
end{align*}




$textbf{Attempt}$



begin{align*}
(u,u)_{H^1}&=int_{Omega} nabla u cdot nabla u ;dx + int_{partial Omega} u^2 ; dsigma \
&=int_{Omega} nabla cdot(unabla u)-uDelta u ; dx +int_{partial Omega} u^2 ; dsigma \
&=int_{partial Omega} u frac{partial u}{partial nu} ; dsigma +int_{Omega} lambda u^2 dx +int_{partial Omega} u^2 ; dsigma \
&=-int_{partial Omega} u^2 ; dsigma +int_{Omega} lambda u^2 dx +int_{partial Omega} u^2 ; dsigma\
&=lambda Vert u Vert _{L^2(Omega)}^2
end{align*}

I don't know how to get $lambda Vert u Vert_{L^2(Omega)}^2 geq theta Vert u Vert_{H^1(Omega)}^2$...



Any help is appreciated..



Thank you!







analysis pde spectral-theory boundary-value-problem elliptic-equations






share|cite|improve this question













share|cite|improve this question











share|cite|improve this question




share|cite|improve this question










asked Dec 10 '18 at 13:56









w.sdkaw.sdka

36919




36919












  • $begingroup$
    What is the connection between the taks 'Show that...' and the eigenvalue problem? As it is stated now, there is no connection, and it looks like the inequality has to be proven for all $uin H^1$.
    $endgroup$
    – daw
    Dec 10 '18 at 14:19










  • $begingroup$
    If I prove the problem, then I'll get every eigenvalue is a positive real number.
    $endgroup$
    – w.sdka
    Dec 10 '18 at 14:22


















  • $begingroup$
    What is the connection between the taks 'Show that...' and the eigenvalue problem? As it is stated now, there is no connection, and it looks like the inequality has to be proven for all $uin H^1$.
    $endgroup$
    – daw
    Dec 10 '18 at 14:19










  • $begingroup$
    If I prove the problem, then I'll get every eigenvalue is a positive real number.
    $endgroup$
    – w.sdka
    Dec 10 '18 at 14:22
















$begingroup$
What is the connection between the taks 'Show that...' and the eigenvalue problem? As it is stated now, there is no connection, and it looks like the inequality has to be proven for all $uin H^1$.
$endgroup$
– daw
Dec 10 '18 at 14:19




$begingroup$
What is the connection between the taks 'Show that...' and the eigenvalue problem? As it is stated now, there is no connection, and it looks like the inequality has to be proven for all $uin H^1$.
$endgroup$
– daw
Dec 10 '18 at 14:19












$begingroup$
If I prove the problem, then I'll get every eigenvalue is a positive real number.
$endgroup$
– w.sdka
Dec 10 '18 at 14:22




$begingroup$
If I prove the problem, then I'll get every eigenvalue is a positive real number.
$endgroup$
– w.sdka
Dec 10 '18 at 14:22










2 Answers
2






active

oldest

votes


















1












$begingroup$

Here is a standard proof by contradiction.
Assume that the inequality does not hold. Then for all $n$ there is $u_nin H^1(Omega)$
such that
$$
|nabla u_n|_{L^2(Omega)}^2 + |u_n|_{L^2(partialOmega)}^2 < n |u_n|_{H^1(Omega)}^2.
$$

This implies $u_nne0$, and we can assume w.l.o.g. $|u_n|_{H^1(Omega)}=1$. Then $nabla u_nto0$ in $L^2(Omega)$ and $uto0$ in $L^2(partialOmega)$ follows immediately.



Since $(u_n)$ is bounded in $H^1$, after extracting a subsequence (denoted the same for simplicity), we have $u_nrightharpoonup u$ in $H^1(Omega)$. Then $nabla u=0$, and $u$ is a constant. Since $|u|_{L^2(partialOmega)}=0$, it follows $u=0$.
By compact embedding, $u_nto0$ in $L^2(Omega)$. This implies $uto0$ strongly in $H^1(Omega)$, which is a contradiction to $|u_n|_{H^1}=1$.






share|cite|improve this answer









$endgroup$





















    1












    $begingroup$

    If you want to show that for $u$ that are solutions of the eigenvalue problem,$$(u,u)_{H^1}getheta int_Omega |nabla u|^2 + |u|^2 dx,$$ you have already done all the hard work. From your equalities, using the first and last line,
    $$
    (u,u)_{H^1}=frac12int_Omega nabla u cdot nabla u dx + frac12 int_{partialOmega} |u|^2 dsigma + fraclambda2 int_Omega u^2 dx.
    $$

    Dropping the middle term and using $theta=min(frac12,fraclambda 2)$ you get what you want.






    share|cite|improve this answer









    $endgroup$













    • $begingroup$
      Is $lambda$ always positive?
      $endgroup$
      – w.sdka
      Dec 10 '18 at 14:15










    • $begingroup$
      You have $lambda=frac{(u,u)_{H_1}}{|u|_{L^2}^2}$ (and you assume $u$ nonzero as it is an eigenfunction). That means clearly $lambdage 0$. If $lambda=0$, you get that $int_Omega |nabla u|^2 dx+int_{partialOmega} |u|^2 dsigma=0$ so $u$ is constant, and zero on the boundary, so zero everywhere. So $lambda>0$.
      $endgroup$
      – Kusma
      Dec 10 '18 at 14:29











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    2 Answers
    2






    active

    oldest

    votes








    2 Answers
    2






    active

    oldest

    votes









    active

    oldest

    votes






    active

    oldest

    votes









    1












    $begingroup$

    Here is a standard proof by contradiction.
    Assume that the inequality does not hold. Then for all $n$ there is $u_nin H^1(Omega)$
    such that
    $$
    |nabla u_n|_{L^2(Omega)}^2 + |u_n|_{L^2(partialOmega)}^2 < n |u_n|_{H^1(Omega)}^2.
    $$

    This implies $u_nne0$, and we can assume w.l.o.g. $|u_n|_{H^1(Omega)}=1$. Then $nabla u_nto0$ in $L^2(Omega)$ and $uto0$ in $L^2(partialOmega)$ follows immediately.



    Since $(u_n)$ is bounded in $H^1$, after extracting a subsequence (denoted the same for simplicity), we have $u_nrightharpoonup u$ in $H^1(Omega)$. Then $nabla u=0$, and $u$ is a constant. Since $|u|_{L^2(partialOmega)}=0$, it follows $u=0$.
    By compact embedding, $u_nto0$ in $L^2(Omega)$. This implies $uto0$ strongly in $H^1(Omega)$, which is a contradiction to $|u_n|_{H^1}=1$.






    share|cite|improve this answer









    $endgroup$


















      1












      $begingroup$

      Here is a standard proof by contradiction.
      Assume that the inequality does not hold. Then for all $n$ there is $u_nin H^1(Omega)$
      such that
      $$
      |nabla u_n|_{L^2(Omega)}^2 + |u_n|_{L^2(partialOmega)}^2 < n |u_n|_{H^1(Omega)}^2.
      $$

      This implies $u_nne0$, and we can assume w.l.o.g. $|u_n|_{H^1(Omega)}=1$. Then $nabla u_nto0$ in $L^2(Omega)$ and $uto0$ in $L^2(partialOmega)$ follows immediately.



      Since $(u_n)$ is bounded in $H^1$, after extracting a subsequence (denoted the same for simplicity), we have $u_nrightharpoonup u$ in $H^1(Omega)$. Then $nabla u=0$, and $u$ is a constant. Since $|u|_{L^2(partialOmega)}=0$, it follows $u=0$.
      By compact embedding, $u_nto0$ in $L^2(Omega)$. This implies $uto0$ strongly in $H^1(Omega)$, which is a contradiction to $|u_n|_{H^1}=1$.






      share|cite|improve this answer









      $endgroup$
















        1












        1








        1





        $begingroup$

        Here is a standard proof by contradiction.
        Assume that the inequality does not hold. Then for all $n$ there is $u_nin H^1(Omega)$
        such that
        $$
        |nabla u_n|_{L^2(Omega)}^2 + |u_n|_{L^2(partialOmega)}^2 < n |u_n|_{H^1(Omega)}^2.
        $$

        This implies $u_nne0$, and we can assume w.l.o.g. $|u_n|_{H^1(Omega)}=1$. Then $nabla u_nto0$ in $L^2(Omega)$ and $uto0$ in $L^2(partialOmega)$ follows immediately.



        Since $(u_n)$ is bounded in $H^1$, after extracting a subsequence (denoted the same for simplicity), we have $u_nrightharpoonup u$ in $H^1(Omega)$. Then $nabla u=0$, and $u$ is a constant. Since $|u|_{L^2(partialOmega)}=0$, it follows $u=0$.
        By compact embedding, $u_nto0$ in $L^2(Omega)$. This implies $uto0$ strongly in $H^1(Omega)$, which is a contradiction to $|u_n|_{H^1}=1$.






        share|cite|improve this answer









        $endgroup$



        Here is a standard proof by contradiction.
        Assume that the inequality does not hold. Then for all $n$ there is $u_nin H^1(Omega)$
        such that
        $$
        |nabla u_n|_{L^2(Omega)}^2 + |u_n|_{L^2(partialOmega)}^2 < n |u_n|_{H^1(Omega)}^2.
        $$

        This implies $u_nne0$, and we can assume w.l.o.g. $|u_n|_{H^1(Omega)}=1$. Then $nabla u_nto0$ in $L^2(Omega)$ and $uto0$ in $L^2(partialOmega)$ follows immediately.



        Since $(u_n)$ is bounded in $H^1$, after extracting a subsequence (denoted the same for simplicity), we have $u_nrightharpoonup u$ in $H^1(Omega)$. Then $nabla u=0$, and $u$ is a constant. Since $|u|_{L^2(partialOmega)}=0$, it follows $u=0$.
        By compact embedding, $u_nto0$ in $L^2(Omega)$. This implies $uto0$ strongly in $H^1(Omega)$, which is a contradiction to $|u_n|_{H^1}=1$.







        share|cite|improve this answer












        share|cite|improve this answer



        share|cite|improve this answer










        answered Dec 10 '18 at 14:30









        dawdaw

        24.1k1544




        24.1k1544























            1












            $begingroup$

            If you want to show that for $u$ that are solutions of the eigenvalue problem,$$(u,u)_{H^1}getheta int_Omega |nabla u|^2 + |u|^2 dx,$$ you have already done all the hard work. From your equalities, using the first and last line,
            $$
            (u,u)_{H^1}=frac12int_Omega nabla u cdot nabla u dx + frac12 int_{partialOmega} |u|^2 dsigma + fraclambda2 int_Omega u^2 dx.
            $$

            Dropping the middle term and using $theta=min(frac12,fraclambda 2)$ you get what you want.






            share|cite|improve this answer









            $endgroup$













            • $begingroup$
              Is $lambda$ always positive?
              $endgroup$
              – w.sdka
              Dec 10 '18 at 14:15










            • $begingroup$
              You have $lambda=frac{(u,u)_{H_1}}{|u|_{L^2}^2}$ (and you assume $u$ nonzero as it is an eigenfunction). That means clearly $lambdage 0$. If $lambda=0$, you get that $int_Omega |nabla u|^2 dx+int_{partialOmega} |u|^2 dsigma=0$ so $u$ is constant, and zero on the boundary, so zero everywhere. So $lambda>0$.
              $endgroup$
              – Kusma
              Dec 10 '18 at 14:29
















            1












            $begingroup$

            If you want to show that for $u$ that are solutions of the eigenvalue problem,$$(u,u)_{H^1}getheta int_Omega |nabla u|^2 + |u|^2 dx,$$ you have already done all the hard work. From your equalities, using the first and last line,
            $$
            (u,u)_{H^1}=frac12int_Omega nabla u cdot nabla u dx + frac12 int_{partialOmega} |u|^2 dsigma + fraclambda2 int_Omega u^2 dx.
            $$

            Dropping the middle term and using $theta=min(frac12,fraclambda 2)$ you get what you want.






            share|cite|improve this answer









            $endgroup$













            • $begingroup$
              Is $lambda$ always positive?
              $endgroup$
              – w.sdka
              Dec 10 '18 at 14:15










            • $begingroup$
              You have $lambda=frac{(u,u)_{H_1}}{|u|_{L^2}^2}$ (and you assume $u$ nonzero as it is an eigenfunction). That means clearly $lambdage 0$. If $lambda=0$, you get that $int_Omega |nabla u|^2 dx+int_{partialOmega} |u|^2 dsigma=0$ so $u$ is constant, and zero on the boundary, so zero everywhere. So $lambda>0$.
              $endgroup$
              – Kusma
              Dec 10 '18 at 14:29














            1












            1








            1





            $begingroup$

            If you want to show that for $u$ that are solutions of the eigenvalue problem,$$(u,u)_{H^1}getheta int_Omega |nabla u|^2 + |u|^2 dx,$$ you have already done all the hard work. From your equalities, using the first and last line,
            $$
            (u,u)_{H^1}=frac12int_Omega nabla u cdot nabla u dx + frac12 int_{partialOmega} |u|^2 dsigma + fraclambda2 int_Omega u^2 dx.
            $$

            Dropping the middle term and using $theta=min(frac12,fraclambda 2)$ you get what you want.






            share|cite|improve this answer









            $endgroup$



            If you want to show that for $u$ that are solutions of the eigenvalue problem,$$(u,u)_{H^1}getheta int_Omega |nabla u|^2 + |u|^2 dx,$$ you have already done all the hard work. From your equalities, using the first and last line,
            $$
            (u,u)_{H^1}=frac12int_Omega nabla u cdot nabla u dx + frac12 int_{partialOmega} |u|^2 dsigma + fraclambda2 int_Omega u^2 dx.
            $$

            Dropping the middle term and using $theta=min(frac12,fraclambda 2)$ you get what you want.







            share|cite|improve this answer












            share|cite|improve this answer



            share|cite|improve this answer










            answered Dec 10 '18 at 14:12









            KusmaKusma

            3,7181319




            3,7181319












            • $begingroup$
              Is $lambda$ always positive?
              $endgroup$
              – w.sdka
              Dec 10 '18 at 14:15










            • $begingroup$
              You have $lambda=frac{(u,u)_{H_1}}{|u|_{L^2}^2}$ (and you assume $u$ nonzero as it is an eigenfunction). That means clearly $lambdage 0$. If $lambda=0$, you get that $int_Omega |nabla u|^2 dx+int_{partialOmega} |u|^2 dsigma=0$ so $u$ is constant, and zero on the boundary, so zero everywhere. So $lambda>0$.
              $endgroup$
              – Kusma
              Dec 10 '18 at 14:29


















            • $begingroup$
              Is $lambda$ always positive?
              $endgroup$
              – w.sdka
              Dec 10 '18 at 14:15










            • $begingroup$
              You have $lambda=frac{(u,u)_{H_1}}{|u|_{L^2}^2}$ (and you assume $u$ nonzero as it is an eigenfunction). That means clearly $lambdage 0$. If $lambda=0$, you get that $int_Omega |nabla u|^2 dx+int_{partialOmega} |u|^2 dsigma=0$ so $u$ is constant, and zero on the boundary, so zero everywhere. So $lambda>0$.
              $endgroup$
              – Kusma
              Dec 10 '18 at 14:29
















            $begingroup$
            Is $lambda$ always positive?
            $endgroup$
            – w.sdka
            Dec 10 '18 at 14:15




            $begingroup$
            Is $lambda$ always positive?
            $endgroup$
            – w.sdka
            Dec 10 '18 at 14:15












            $begingroup$
            You have $lambda=frac{(u,u)_{H_1}}{|u|_{L^2}^2}$ (and you assume $u$ nonzero as it is an eigenfunction). That means clearly $lambdage 0$. If $lambda=0$, you get that $int_Omega |nabla u|^2 dx+int_{partialOmega} |u|^2 dsigma=0$ so $u$ is constant, and zero on the boundary, so zero everywhere. So $lambda>0$.
            $endgroup$
            – Kusma
            Dec 10 '18 at 14:29




            $begingroup$
            You have $lambda=frac{(u,u)_{H_1}}{|u|_{L^2}^2}$ (and you assume $u$ nonzero as it is an eigenfunction). That means clearly $lambdage 0$. If $lambda=0$, you get that $int_Omega |nabla u|^2 dx+int_{partialOmega} |u|^2 dsigma=0$ so $u$ is constant, and zero on the boundary, so zero everywhere. So $lambda>0$.
            $endgroup$
            – Kusma
            Dec 10 '18 at 14:29


















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