If $u$ is harmonic and vanishes on the boundary, then $uequiv 0$.

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Let's assume $u$ is harmonic on $D=x^2+y^2leq1$. If $u=0$ on $partial D$ then $uequiv 0$ on $D$.



$textbfProof$:
Let's use Green's theorem and set $P=-ufracpartial upartial y$ and $Q=ufracpartial upartial x$.



Then



$$1. fracpartial Qpartial x-fracpartial Ppartial y
=left(fracpartial upartial xright)^2+
uleft(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2+
uleft(fracpartial upartial yright)^2
=left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2.
$$



By Green's theorem,

$$
0=int_partial D -ufracpartial upartial ydx+ufracpartial upartial xdy=int int_D
left(
left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2right)dxdy.
$$



Because $uin C^2$, we get



$$
left(fracpartial upartial xright)^2 +
left(fracpartial upartial yright)^2=0.
$$



So $uequiv c$ on $D$ but on $partial D$ we have $u=0$. So $uequiv 0$.



What have we done on the first move for $1$.?







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  • You can also use the strong max/min principle of Harmonic Functions, which states that non-constant Harmonic Functions attain their max/min only on the boundary. Since the value on the boundary is identically 0, we see it's max and min are 0, so it must be constant, e.g. $u equiv 0$
    – Raymond Chu
    Jul 29 at 17:06














up vote
1
down vote

favorite
1












Let's assume $u$ is harmonic on $D=x^2+y^2leq1$. If $u=0$ on $partial D$ then $uequiv 0$ on $D$.



$textbfProof$:
Let's use Green's theorem and set $P=-ufracpartial upartial y$ and $Q=ufracpartial upartial x$.



Then



$$1. fracpartial Qpartial x-fracpartial Ppartial y
=left(fracpartial upartial xright)^2+
uleft(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2+
uleft(fracpartial upartial yright)^2
=left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2.
$$



By Green's theorem,

$$
0=int_partial D -ufracpartial upartial ydx+ufracpartial upartial xdy=int int_D
left(
left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2right)dxdy.
$$



Because $uin C^2$, we get



$$
left(fracpartial upartial xright)^2 +
left(fracpartial upartial yright)^2=0.
$$



So $uequiv c$ on $D$ but on $partial D$ we have $u=0$. So $uequiv 0$.



What have we done on the first move for $1$.?







share|cite|improve this question





















  • You can also use the strong max/min principle of Harmonic Functions, which states that non-constant Harmonic Functions attain their max/min only on the boundary. Since the value on the boundary is identically 0, we see it's max and min are 0, so it must be constant, e.g. $u equiv 0$
    – Raymond Chu
    Jul 29 at 17:06












up vote
1
down vote

favorite
1









up vote
1
down vote

favorite
1






1





Let's assume $u$ is harmonic on $D=x^2+y^2leq1$. If $u=0$ on $partial D$ then $uequiv 0$ on $D$.



$textbfProof$:
Let's use Green's theorem and set $P=-ufracpartial upartial y$ and $Q=ufracpartial upartial x$.



Then



$$1. fracpartial Qpartial x-fracpartial Ppartial y
=left(fracpartial upartial xright)^2+
uleft(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2+
uleft(fracpartial upartial yright)^2
=left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2.
$$



By Green's theorem,

$$
0=int_partial D -ufracpartial upartial ydx+ufracpartial upartial xdy=int int_D
left(
left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2right)dxdy.
$$



Because $uin C^2$, we get



$$
left(fracpartial upartial xright)^2 +
left(fracpartial upartial yright)^2=0.
$$



So $uequiv c$ on $D$ but on $partial D$ we have $u=0$. So $uequiv 0$.



What have we done on the first move for $1$.?







share|cite|improve this question













Let's assume $u$ is harmonic on $D=x^2+y^2leq1$. If $u=0$ on $partial D$ then $uequiv 0$ on $D$.



$textbfProof$:
Let's use Green's theorem and set $P=-ufracpartial upartial y$ and $Q=ufracpartial upartial x$.



Then



$$1. fracpartial Qpartial x-fracpartial Ppartial y
=left(fracpartial upartial xright)^2+
uleft(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2+
uleft(fracpartial upartial yright)^2
=left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2.
$$



By Green's theorem,

$$
0=int_partial D -ufracpartial upartial ydx+ufracpartial upartial xdy=int int_D
left(
left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2right)dxdy.
$$



Because $uin C^2$, we get



$$
left(fracpartial upartial xright)^2 +
left(fracpartial upartial yright)^2=0.
$$



So $uequiv c$ on $D$ but on $partial D$ we have $u=0$. So $uequiv 0$.



What have we done on the first move for $1$.?









share|cite|improve this question












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edited Jul 29 at 16:26









Mee Seong Im

2,5591517




2,5591517









asked Jul 29 at 15:02









newhere

742310




742310











  • You can also use the strong max/min principle of Harmonic Functions, which states that non-constant Harmonic Functions attain their max/min only on the boundary. Since the value on the boundary is identically 0, we see it's max and min are 0, so it must be constant, e.g. $u equiv 0$
    – Raymond Chu
    Jul 29 at 17:06
















  • You can also use the strong max/min principle of Harmonic Functions, which states that non-constant Harmonic Functions attain their max/min only on the boundary. Since the value on the boundary is identically 0, we see it's max and min are 0, so it must be constant, e.g. $u equiv 0$
    – Raymond Chu
    Jul 29 at 17:06















You can also use the strong max/min principle of Harmonic Functions, which states that non-constant Harmonic Functions attain their max/min only on the boundary. Since the value on the boundary is identically 0, we see it's max and min are 0, so it must be constant, e.g. $u equiv 0$
– Raymond Chu
Jul 29 at 17:06




You can also use the strong max/min principle of Harmonic Functions, which states that non-constant Harmonic Functions attain their max/min only on the boundary. Since the value on the boundary is identically 0, we see it's max and min are 0, so it must be constant, e.g. $u equiv 0$
– Raymond Chu
Jul 29 at 17:06










2 Answers
2






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oldest

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up vote
1
down vote



accepted










In the second line of your proof, it should be:



beginalign*
fracpartial Qpartial x-fracpartial Ppartial y
&=left(fracpartial upartial xright)^2+
ufracpartial^2 upartial x^2+
left(fracpartial upartial yright)^2+
u fracpartial^2 upartial y^2 \
&= left(fracpartial upartial xright)^2
+ left(fracpartial upartial yright)^2
+ u
underbraceleft( fracpartial^2 upartial x^2
+ fracpartial^2 upartial y^2right)_0 \
&=left(fracpartial upartial xright)^2+
left(fracpartial upartial yright)^2
endalign*
since $u$ is harmonic on $D$, i.e., $u$ must satisfy Laplace's equation.






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    up vote
    1
    down vote













    We have used the product rule; e.g.



    $$
    partial_x Q = partial (u partial_x u) = (partial_x u)^2 + u partial_x^2 u.
    $$



    (Your notation seems a bit off at that point.)






    share|cite|improve this answer





















    • Is the sentence true only on a circle?
      – newhere
      Jul 29 at 15:38










    • In fact, I now recall that using probabilistic methods, one can show uniqueness on arbitrary open and bounded sets. @newhere
      – AlgebraicsAnonymous
      Jul 29 at 15:39











    Your Answer




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    2 Answers
    2






    active

    oldest

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    2 Answers
    2






    active

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    active

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    active

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    up vote
    1
    down vote



    accepted










    In the second line of your proof, it should be:



    beginalign*
    fracpartial Qpartial x-fracpartial Ppartial y
    &=left(fracpartial upartial xright)^2+
    ufracpartial^2 upartial x^2+
    left(fracpartial upartial yright)^2+
    u fracpartial^2 upartial y^2 \
    &= left(fracpartial upartial xright)^2
    + left(fracpartial upartial yright)^2
    + u
    underbraceleft( fracpartial^2 upartial x^2
    + fracpartial^2 upartial y^2right)_0 \
    &=left(fracpartial upartial xright)^2+
    left(fracpartial upartial yright)^2
    endalign*
    since $u$ is harmonic on $D$, i.e., $u$ must satisfy Laplace's equation.






    share|cite|improve this answer

























      up vote
      1
      down vote



      accepted










      In the second line of your proof, it should be:



      beginalign*
      fracpartial Qpartial x-fracpartial Ppartial y
      &=left(fracpartial upartial xright)^2+
      ufracpartial^2 upartial x^2+
      left(fracpartial upartial yright)^2+
      u fracpartial^2 upartial y^2 \
      &= left(fracpartial upartial xright)^2
      + left(fracpartial upartial yright)^2
      + u
      underbraceleft( fracpartial^2 upartial x^2
      + fracpartial^2 upartial y^2right)_0 \
      &=left(fracpartial upartial xright)^2+
      left(fracpartial upartial yright)^2
      endalign*
      since $u$ is harmonic on $D$, i.e., $u$ must satisfy Laplace's equation.






      share|cite|improve this answer























        up vote
        1
        down vote



        accepted







        up vote
        1
        down vote



        accepted






        In the second line of your proof, it should be:



        beginalign*
        fracpartial Qpartial x-fracpartial Ppartial y
        &=left(fracpartial upartial xright)^2+
        ufracpartial^2 upartial x^2+
        left(fracpartial upartial yright)^2+
        u fracpartial^2 upartial y^2 \
        &= left(fracpartial upartial xright)^2
        + left(fracpartial upartial yright)^2
        + u
        underbraceleft( fracpartial^2 upartial x^2
        + fracpartial^2 upartial y^2right)_0 \
        &=left(fracpartial upartial xright)^2+
        left(fracpartial upartial yright)^2
        endalign*
        since $u$ is harmonic on $D$, i.e., $u$ must satisfy Laplace's equation.






        share|cite|improve this answer













        In the second line of your proof, it should be:



        beginalign*
        fracpartial Qpartial x-fracpartial Ppartial y
        &=left(fracpartial upartial xright)^2+
        ufracpartial^2 upartial x^2+
        left(fracpartial upartial yright)^2+
        u fracpartial^2 upartial y^2 \
        &= left(fracpartial upartial xright)^2
        + left(fracpartial upartial yright)^2
        + u
        underbraceleft( fracpartial^2 upartial x^2
        + fracpartial^2 upartial y^2right)_0 \
        &=left(fracpartial upartial xright)^2+
        left(fracpartial upartial yright)^2
        endalign*
        since $u$ is harmonic on $D$, i.e., $u$ must satisfy Laplace's equation.







        share|cite|improve this answer













        share|cite|improve this answer



        share|cite|improve this answer











        answered Jul 29 at 16:45









        Mee Seong Im

        2,5591517




        2,5591517




















            up vote
            1
            down vote













            We have used the product rule; e.g.



            $$
            partial_x Q = partial (u partial_x u) = (partial_x u)^2 + u partial_x^2 u.
            $$



            (Your notation seems a bit off at that point.)






            share|cite|improve this answer





















            • Is the sentence true only on a circle?
              – newhere
              Jul 29 at 15:38










            • In fact, I now recall that using probabilistic methods, one can show uniqueness on arbitrary open and bounded sets. @newhere
              – AlgebraicsAnonymous
              Jul 29 at 15:39















            up vote
            1
            down vote













            We have used the product rule; e.g.



            $$
            partial_x Q = partial (u partial_x u) = (partial_x u)^2 + u partial_x^2 u.
            $$



            (Your notation seems a bit off at that point.)






            share|cite|improve this answer





















            • Is the sentence true only on a circle?
              – newhere
              Jul 29 at 15:38










            • In fact, I now recall that using probabilistic methods, one can show uniqueness on arbitrary open and bounded sets. @newhere
              – AlgebraicsAnonymous
              Jul 29 at 15:39













            up vote
            1
            down vote










            up vote
            1
            down vote









            We have used the product rule; e.g.



            $$
            partial_x Q = partial (u partial_x u) = (partial_x u)^2 + u partial_x^2 u.
            $$



            (Your notation seems a bit off at that point.)






            share|cite|improve this answer













            We have used the product rule; e.g.



            $$
            partial_x Q = partial (u partial_x u) = (partial_x u)^2 + u partial_x^2 u.
            $$



            (Your notation seems a bit off at that point.)







            share|cite|improve this answer













            share|cite|improve this answer



            share|cite|improve this answer











            answered Jul 29 at 15:30









            AlgebraicsAnonymous

            66611




            66611











            • Is the sentence true only on a circle?
              – newhere
              Jul 29 at 15:38










            • In fact, I now recall that using probabilistic methods, one can show uniqueness on arbitrary open and bounded sets. @newhere
              – AlgebraicsAnonymous
              Jul 29 at 15:39

















            • Is the sentence true only on a circle?
              – newhere
              Jul 29 at 15:38










            • In fact, I now recall that using probabilistic methods, one can show uniqueness on arbitrary open and bounded sets. @newhere
              – AlgebraicsAnonymous
              Jul 29 at 15:39
















            Is the sentence true only on a circle?
            – newhere
            Jul 29 at 15:38




            Is the sentence true only on a circle?
            – newhere
            Jul 29 at 15:38












            In fact, I now recall that using probabilistic methods, one can show uniqueness on arbitrary open and bounded sets. @newhere
            – AlgebraicsAnonymous
            Jul 29 at 15:39





            In fact, I now recall that using probabilistic methods, one can show uniqueness on arbitrary open and bounded sets. @newhere
            – AlgebraicsAnonymous
            Jul 29 at 15:39













             

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