How to evaluate $S=int_partial Dfrac1^2ds(y)$?A Particular Metric: $(mathbbR^2,d_2)$Linear transformation that does thisShow that $int_[0,1]^2g(y_1-y_2) Bbb1_y_1>y_2dy_1dy_2 = int_[0,1]g(m)(1-m), dm$Product metric spaces is again a metric spaceSum of two Dense setsHow do I show that for a multivariate function, Lipschitz continuity in each variable implies Lipschitz continuity for the whole function?Continuity of the inverse mapGiven two real numbers $a$ and $b$ such that $a<b$, what about the convergence of these two sequences?Partial derivative of function with respect to itselfLipschitz property of $f(x,y)= fracxysqrtx^2+y^2$ for $(x,y)neq (0,0)$ and $f(0,0)=0.$

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How to evaluate $S=int_partial Dfrac1x-yds(y)$?


A Particular Metric: $(mathbbR^2,d_2)$Linear transformation that does thisShow that $int_[0,1]^2g(y_1-y_2) Bbb1_y_1>y_2dy_1dy_2 = int_[0,1]g(m)(1-m), dm$Product metric spaces is again a metric spaceSum of two Dense setsHow do I show that for a multivariate function, Lipschitz continuity in each variable implies Lipschitz continuity for the whole function?Continuity of the inverse mapGiven two real numbers $a$ and $b$ such that $a<b$, what about the convergence of these two sequences?Partial derivative of function with respect to itselfLipschitz property of $f(x,y)= fracxysqrtx^2+y^2$ for $(x,y)neq (0,0)$ and $f(0,0)=0.$













2












$begingroup$


Let $D=B(0,r_0), x,y in mathbbR^3$ and $xin D$.
beginalign*
& S=int_partial Dfrac1x-yds(y)=int_partial Dfrac1(x_1-y_1)^2+(x_2-y_2)^2+(x_3-y_3)^2ds(y)
endalign*

I want to prove that $Sleq k$ ($k>0$ and $k$ only depends on $r_0$).



In case $x ne 0$, my idea is
beginsplit
S^+ &=int_y_1^2+y_2^2leq r_0^2frac1(x_1-y_1)^2+(x_2-y_2)^2+Big(x_3-sqrtr_0^2-y_1^2-y_2^2Big)^2fracr_0sqrtr_0^2-y_1^2-y_2^2dy_1dy_2\
&leq int_y_1^2+y_2^2leq r_0^2frac1Big(x_3-sqrtr_0^2-y_1^2-y_2^2Big)^2fracr_0sqrtr_0^2-y_1^2-y_2^2dy_1dy_2: text (assume x_3 ne 0)
endsplit

Let $y_1=rcosphi, y_2=rsinphi, 0leq phi leq 2pi$
beginsplit
S^+&=int_0^2pidphiint_0^r_0frac1Big(x_3-sqrtr_0^2-r^2Big)^2fracr_0sqrtr_0^2-r^2rdr\
&=2r_0pileft(frac1-x_3-frac1r_0-x_3right)\
endsplit

with $-r_0<x_3<r_0, x_3 ne 0$, I can't show that $left(frac1-x_3-frac1r_0-x_3right)$ is bounded. Please help me, thank you so much!










share|cite|improve this question











$endgroup$







  • 1




    $begingroup$
    What has this to do with functional-analysis?
    $endgroup$
    – José Carlos Santos
    yesterday






  • 1




    $begingroup$
    It's not true... for instance, when $|x-y|to 0$, it explose.
    $endgroup$
    – user657324
    yesterday










  • $begingroup$
    @user657324 since $xin D$ and $y in partial D$ there exists $delta>0$ with $|x-y|>delta$
    $endgroup$
    – Chloe.Sannon
    yesterday











  • $begingroup$
    Yes, but $delta $ depend on $x$, so you can't upper bound $S$ uniformly in $x$. @Chloe.Sannon
    $endgroup$
    – user657324
    yesterday
















2












$begingroup$


Let $D=B(0,r_0), x,y in mathbbR^3$ and $xin D$.
beginalign*
& S=int_partial Dfrac1x-yds(y)=int_partial Dfrac1(x_1-y_1)^2+(x_2-y_2)^2+(x_3-y_3)^2ds(y)
endalign*

I want to prove that $Sleq k$ ($k>0$ and $k$ only depends on $r_0$).



In case $x ne 0$, my idea is
beginsplit
S^+ &=int_y_1^2+y_2^2leq r_0^2frac1(x_1-y_1)^2+(x_2-y_2)^2+Big(x_3-sqrtr_0^2-y_1^2-y_2^2Big)^2fracr_0sqrtr_0^2-y_1^2-y_2^2dy_1dy_2\
&leq int_y_1^2+y_2^2leq r_0^2frac1Big(x_3-sqrtr_0^2-y_1^2-y_2^2Big)^2fracr_0sqrtr_0^2-y_1^2-y_2^2dy_1dy_2: text (assume x_3 ne 0)
endsplit

Let $y_1=rcosphi, y_2=rsinphi, 0leq phi leq 2pi$
beginsplit
S^+&=int_0^2pidphiint_0^r_0frac1Big(x_3-sqrtr_0^2-r^2Big)^2fracr_0sqrtr_0^2-r^2rdr\
&=2r_0pileft(frac1-x_3-frac1r_0-x_3right)\
endsplit

with $-r_0<x_3<r_0, x_3 ne 0$, I can't show that $left(frac1-x_3-frac1r_0-x_3right)$ is bounded. Please help me, thank you so much!










share|cite|improve this question











$endgroup$







  • 1




    $begingroup$
    What has this to do with functional-analysis?
    $endgroup$
    – José Carlos Santos
    yesterday






  • 1




    $begingroup$
    It's not true... for instance, when $|x-y|to 0$, it explose.
    $endgroup$
    – user657324
    yesterday










  • $begingroup$
    @user657324 since $xin D$ and $y in partial D$ there exists $delta>0$ with $|x-y|>delta$
    $endgroup$
    – Chloe.Sannon
    yesterday











  • $begingroup$
    Yes, but $delta $ depend on $x$, so you can't upper bound $S$ uniformly in $x$. @Chloe.Sannon
    $endgroup$
    – user657324
    yesterday














2












2








2





$begingroup$


Let $D=B(0,r_0), x,y in mathbbR^3$ and $xin D$.
beginalign*
& S=int_partial Dfrac1x-yds(y)=int_partial Dfrac1(x_1-y_1)^2+(x_2-y_2)^2+(x_3-y_3)^2ds(y)
endalign*

I want to prove that $Sleq k$ ($k>0$ and $k$ only depends on $r_0$).



In case $x ne 0$, my idea is
beginsplit
S^+ &=int_y_1^2+y_2^2leq r_0^2frac1(x_1-y_1)^2+(x_2-y_2)^2+Big(x_3-sqrtr_0^2-y_1^2-y_2^2Big)^2fracr_0sqrtr_0^2-y_1^2-y_2^2dy_1dy_2\
&leq int_y_1^2+y_2^2leq r_0^2frac1Big(x_3-sqrtr_0^2-y_1^2-y_2^2Big)^2fracr_0sqrtr_0^2-y_1^2-y_2^2dy_1dy_2: text (assume x_3 ne 0)
endsplit

Let $y_1=rcosphi, y_2=rsinphi, 0leq phi leq 2pi$
beginsplit
S^+&=int_0^2pidphiint_0^r_0frac1Big(x_3-sqrtr_0^2-r^2Big)^2fracr_0sqrtr_0^2-r^2rdr\
&=2r_0pileft(frac1-x_3-frac1r_0-x_3right)\
endsplit

with $-r_0<x_3<r_0, x_3 ne 0$, I can't show that $left(frac1-x_3-frac1r_0-x_3right)$ is bounded. Please help me, thank you so much!










share|cite|improve this question











$endgroup$




Let $D=B(0,r_0), x,y in mathbbR^3$ and $xin D$.
beginalign*
& S=int_partial Dfrac1x-yds(y)=int_partial Dfrac1(x_1-y_1)^2+(x_2-y_2)^2+(x_3-y_3)^2ds(y)
endalign*

I want to prove that $Sleq k$ ($k>0$ and $k$ only depends on $r_0$).



In case $x ne 0$, my idea is
beginsplit
S^+ &=int_y_1^2+y_2^2leq r_0^2frac1(x_1-y_1)^2+(x_2-y_2)^2+Big(x_3-sqrtr_0^2-y_1^2-y_2^2Big)^2fracr_0sqrtr_0^2-y_1^2-y_2^2dy_1dy_2\
&leq int_y_1^2+y_2^2leq r_0^2frac1Big(x_3-sqrtr_0^2-y_1^2-y_2^2Big)^2fracr_0sqrtr_0^2-y_1^2-y_2^2dy_1dy_2: text (assume x_3 ne 0)
endsplit

Let $y_1=rcosphi, y_2=rsinphi, 0leq phi leq 2pi$
beginsplit
S^+&=int_0^2pidphiint_0^r_0frac1Big(x_3-sqrtr_0^2-r^2Big)^2fracr_0sqrtr_0^2-r^2rdr\
&=2r_0pileft(frac1-x_3-frac1r_0-x_3right)\
endsplit

with $-r_0<x_3<r_0, x_3 ne 0$, I can't show that $left(frac1-x_3-frac1r_0-x_3right)$ is bounded. Please help me, thank you so much!







real-analysis singular-integrals






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share|cite|improve this question













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edited yesterday









folouer of kaklas

340110




340110










asked yesterday









Chloe.SannonChloe.Sannon

1208




1208







  • 1




    $begingroup$
    What has this to do with functional-analysis?
    $endgroup$
    – José Carlos Santos
    yesterday






  • 1




    $begingroup$
    It's not true... for instance, when $|x-y|to 0$, it explose.
    $endgroup$
    – user657324
    yesterday










  • $begingroup$
    @user657324 since $xin D$ and $y in partial D$ there exists $delta>0$ with $|x-y|>delta$
    $endgroup$
    – Chloe.Sannon
    yesterday











  • $begingroup$
    Yes, but $delta $ depend on $x$, so you can't upper bound $S$ uniformly in $x$. @Chloe.Sannon
    $endgroup$
    – user657324
    yesterday













  • 1




    $begingroup$
    What has this to do with functional-analysis?
    $endgroup$
    – José Carlos Santos
    yesterday






  • 1




    $begingroup$
    It's not true... for instance, when $|x-y|to 0$, it explose.
    $endgroup$
    – user657324
    yesterday










  • $begingroup$
    @user657324 since $xin D$ and $y in partial D$ there exists $delta>0$ with $|x-y|>delta$
    $endgroup$
    – Chloe.Sannon
    yesterday











  • $begingroup$
    Yes, but $delta $ depend on $x$, so you can't upper bound $S$ uniformly in $x$. @Chloe.Sannon
    $endgroup$
    – user657324
    yesterday








1




1




$begingroup$
What has this to do with functional-analysis?
$endgroup$
– José Carlos Santos
yesterday




$begingroup$
What has this to do with functional-analysis?
$endgroup$
– José Carlos Santos
yesterday




1




1




$begingroup$
It's not true... for instance, when $|x-y|to 0$, it explose.
$endgroup$
– user657324
yesterday




$begingroup$
It's not true... for instance, when $|x-y|to 0$, it explose.
$endgroup$
– user657324
yesterday












$begingroup$
@user657324 since $xin D$ and $y in partial D$ there exists $delta>0$ with $|x-y|>delta$
$endgroup$
– Chloe.Sannon
yesterday





$begingroup$
@user657324 since $xin D$ and $y in partial D$ there exists $delta>0$ with $|x-y|>delta$
$endgroup$
– Chloe.Sannon
yesterday













$begingroup$
Yes, but $delta $ depend on $x$, so you can't upper bound $S$ uniformly in $x$. @Chloe.Sannon
$endgroup$
– user657324
yesterday





$begingroup$
Yes, but $delta $ depend on $x$, so you can't upper bound $S$ uniformly in $x$. @Chloe.Sannon
$endgroup$
– user657324
yesterday











2 Answers
2






active

oldest

votes


















1












$begingroup$

You may use spherical coordinates and the cosine-theorem:
$$
frac1x-y = frac1
$$

where $theta_x,y$ is the angle between $x$ and $y$.
Putting it into the integral you have:
$$
intlimits_fracdsx-y =
intlimits_frac r_0^2sin(theta) dphi dthetax=2pi r_0^2intlimits_-1^1frac dcos(theta)x
$$

where we chose to allign $x$ along the z-axis, which we are free to do due to symmetry. Then $theta_x,y$ simply becomes the coordinate $theta$.






share|cite|improve this answer









$endgroup$




















    1












    $begingroup$

    Clearly,
    $$
    F(y)=int_fracds^2
    $$

    is a function of $|y|$. For simplicity, assume that $y=(|y|,0,0)$.



    Since the sphere is a solid by revolution, and in particular of revolution of the graph of the function $f(x)=sqrtr^2-x^2$ around the $x-$axis, then
    $$
    F(y)=2piint_-r_0^r_0 f(x)sqrt1+big(f'(x)big)^2g(x),dx
    =cdots=2pi r_0int_-r_0^r_0 g(x),dx
    $$

    where
    $$
    g(x)=frac1big(x,sqrtr_0^2-x^2,0big)-(=frac1(x-=frac1r_0^2-2x
    $$

    and hence
    $$
    F(y)=2pi r_0int_-r_0^r_0fracdxy=
    left.-fraclog(r_0^2+yright|_-r_0^r_0
    =fraclogleft(fracyr^2_0-2r_0right)y=
    frac
    logleft(
    fracr_0+y
    right)

    $$

    Clearly,
    $$
    lim_yF(y)=infty
    $$






    share|cite|improve this answer









    $endgroup$












      Your Answer





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      2 Answers
      2






      active

      oldest

      votes








      2 Answers
      2






      active

      oldest

      votes









      active

      oldest

      votes






      active

      oldest

      votes









      1












      $begingroup$

      You may use spherical coordinates and the cosine-theorem:
      $$
      frac1x-y = frac1
      $$

      where $theta_x,y$ is the angle between $x$ and $y$.
      Putting it into the integral you have:
      $$
      intlimits_fracdsx-y =
      intlimits_frac r_0^2sin(theta) dphi dthetax=2pi r_0^2intlimits_-1^1frac dcos(theta)x
      $$

      where we chose to allign $x$ along the z-axis, which we are free to do due to symmetry. Then $theta_x,y$ simply becomes the coordinate $theta$.






      share|cite|improve this answer









      $endgroup$

















        1












        $begingroup$

        You may use spherical coordinates and the cosine-theorem:
        $$
        frac1x-y = frac1
        $$

        where $theta_x,y$ is the angle between $x$ and $y$.
        Putting it into the integral you have:
        $$
        intlimits_fracdsx-y =
        intlimits_frac r_0^2sin(theta) dphi dthetax=2pi r_0^2intlimits_-1^1frac dcos(theta)x
        $$

        where we chose to allign $x$ along the z-axis, which we are free to do due to symmetry. Then $theta_x,y$ simply becomes the coordinate $theta$.






        share|cite|improve this answer









        $endgroup$















          1












          1








          1





          $begingroup$

          You may use spherical coordinates and the cosine-theorem:
          $$
          frac1x-y = frac1
          $$

          where $theta_x,y$ is the angle between $x$ and $y$.
          Putting it into the integral you have:
          $$
          intlimits_fracdsx-y =
          intlimits_frac r_0^2sin(theta) dphi dthetax=2pi r_0^2intlimits_-1^1frac dcos(theta)x
          $$

          where we chose to allign $x$ along the z-axis, which we are free to do due to symmetry. Then $theta_x,y$ simply becomes the coordinate $theta$.






          share|cite|improve this answer









          $endgroup$



          You may use spherical coordinates and the cosine-theorem:
          $$
          frac1x-y = frac1
          $$

          where $theta_x,y$ is the angle between $x$ and $y$.
          Putting it into the integral you have:
          $$
          intlimits_fracdsx-y =
          intlimits_frac r_0^2sin(theta) dphi dthetax=2pi r_0^2intlimits_-1^1frac dcos(theta)x
          $$

          where we chose to allign $x$ along the z-axis, which we are free to do due to symmetry. Then $theta_x,y$ simply becomes the coordinate $theta$.







          share|cite|improve this answer












          share|cite|improve this answer



          share|cite|improve this answer










          answered yesterday









          denklodenklo

          4457




          4457





















              1












              $begingroup$

              Clearly,
              $$
              F(y)=int_fracds^2
              $$

              is a function of $|y|$. For simplicity, assume that $y=(|y|,0,0)$.



              Since the sphere is a solid by revolution, and in particular of revolution of the graph of the function $f(x)=sqrtr^2-x^2$ around the $x-$axis, then
              $$
              F(y)=2piint_-r_0^r_0 f(x)sqrt1+big(f'(x)big)^2g(x),dx
              =cdots=2pi r_0int_-r_0^r_0 g(x),dx
              $$

              where
              $$
              g(x)=frac1big(x,sqrtr_0^2-x^2,0big)-(=frac1(x-=frac1r_0^2-2x
              $$

              and hence
              $$
              F(y)=2pi r_0int_-r_0^r_0fracdxy=
              left.-fraclog(r_0^2+yright|_-r_0^r_0
              =fraclogleft(fracyr^2_0-2r_0right)y=
              frac
              logleft(
              fracr_0+y
              right)

              $$

              Clearly,
              $$
              lim_yF(y)=infty
              $$






              share|cite|improve this answer









              $endgroup$

















                1












                $begingroup$

                Clearly,
                $$
                F(y)=int_fracds^2
                $$

                is a function of $|y|$. For simplicity, assume that $y=(|y|,0,0)$.



                Since the sphere is a solid by revolution, and in particular of revolution of the graph of the function $f(x)=sqrtr^2-x^2$ around the $x-$axis, then
                $$
                F(y)=2piint_-r_0^r_0 f(x)sqrt1+big(f'(x)big)^2g(x),dx
                =cdots=2pi r_0int_-r_0^r_0 g(x),dx
                $$

                where
                $$
                g(x)=frac1big(x,sqrtr_0^2-x^2,0big)-(=frac1(x-=frac1r_0^2-2x
                $$

                and hence
                $$
                F(y)=2pi r_0int_-r_0^r_0fracdxy=
                left.-fraclog(r_0^2+yright|_-r_0^r_0
                =fraclogleft(fracyr^2_0-2r_0right)y=
                frac
                logleft(
                fracr_0+y
                right)

                $$

                Clearly,
                $$
                lim_yF(y)=infty
                $$






                share|cite|improve this answer









                $endgroup$















                  1












                  1








                  1





                  $begingroup$

                  Clearly,
                  $$
                  F(y)=int_fracds^2
                  $$

                  is a function of $|y|$. For simplicity, assume that $y=(|y|,0,0)$.



                  Since the sphere is a solid by revolution, and in particular of revolution of the graph of the function $f(x)=sqrtr^2-x^2$ around the $x-$axis, then
                  $$
                  F(y)=2piint_-r_0^r_0 f(x)sqrt1+big(f'(x)big)^2g(x),dx
                  =cdots=2pi r_0int_-r_0^r_0 g(x),dx
                  $$

                  where
                  $$
                  g(x)=frac1big(x,sqrtr_0^2-x^2,0big)-(=frac1(x-=frac1r_0^2-2x
                  $$

                  and hence
                  $$
                  F(y)=2pi r_0int_-r_0^r_0fracdxy=
                  left.-fraclog(r_0^2+yright|_-r_0^r_0
                  =fraclogleft(fracyr^2_0-2r_0right)y=
                  frac
                  logleft(
                  fracr_0+y
                  right)

                  $$

                  Clearly,
                  $$
                  lim_yF(y)=infty
                  $$






                  share|cite|improve this answer









                  $endgroup$



                  Clearly,
                  $$
                  F(y)=int_fracds^2
                  $$

                  is a function of $|y|$. For simplicity, assume that $y=(|y|,0,0)$.



                  Since the sphere is a solid by revolution, and in particular of revolution of the graph of the function $f(x)=sqrtr^2-x^2$ around the $x-$axis, then
                  $$
                  F(y)=2piint_-r_0^r_0 f(x)sqrt1+big(f'(x)big)^2g(x),dx
                  =cdots=2pi r_0int_-r_0^r_0 g(x),dx
                  $$

                  where
                  $$
                  g(x)=frac1big(x,sqrtr_0^2-x^2,0big)-(=frac1(x-=frac1r_0^2-2x
                  $$

                  and hence
                  $$
                  F(y)=2pi r_0int_-r_0^r_0fracdxy=
                  left.-fraclog(r_0^2+yright|_-r_0^r_0
                  =fraclogleft(fracyr^2_0-2r_0right)y=
                  frac
                  logleft(
                  fracr_0+y
                  right)

                  $$

                  Clearly,
                  $$
                  lim_yF(y)=infty
                  $$







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                  answered yesterday









                  Yiorgos S. SmyrlisYiorgos S. Smyrlis

                  63.6k1385165




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