How can you determine if a point is inside a parametric 2D manifold?












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Asume I have an arbitrary, parametric, closed, orientable, surface; a sphere, ellipsoid, closed cylinder, weird general cone....



If you only have access to the parametrization, how can you determine whether a 3D point is inside or outside of the manifold?










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    1












    $begingroup$


    Asume I have an arbitrary, parametric, closed, orientable, surface; a sphere, ellipsoid, closed cylinder, weird general cone....



    If you only have access to the parametrization, how can you determine whether a 3D point is inside or outside of the manifold?










    share|cite|improve this question











    $endgroup$















      1












      1








      1





      $begingroup$


      Asume I have an arbitrary, parametric, closed, orientable, surface; a sphere, ellipsoid, closed cylinder, weird general cone....



      If you only have access to the parametrization, how can you determine whether a 3D point is inside or outside of the manifold?










      share|cite|improve this question











      $endgroup$




      Asume I have an arbitrary, parametric, closed, orientable, surface; a sphere, ellipsoid, closed cylinder, weird general cone....



      If you only have access to the parametrization, how can you determine whether a 3D point is inside or outside of the manifold?







      calculus geometry manifolds parametric geometric-topology






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      edited Nov 29 '18 at 22:38









      Bernard

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      119k639112










      asked Nov 29 '18 at 21:42









      MakoganMakogan

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          $begingroup$

          I presume you are trying to determine is if a point $p$ is inside or outside the region $Omega$ of space enclosed by the manifold, which can be seen as the boundary $partial Omega$ of $Omega$. A solution is to use use Stokes–Cartan theorem:
          $$
          int_{partial Omega} omega = int_{Omega} domega
          $$

          with a suitable choice of the differential form $omega$. In our case the following will work, compute:
          $$
          I = int_{partial Omega} frac{(x-p)}{|x-p|^3} dS
          $$

          over the manifold, where $x$ is the (3-dim) variable of integration, and $dS$ is the 2-form representing the area element of the surface. If $p$ is outside $Omega$ then $I=0$. If $p$ is inside then $|I|$ yields the area of a unit sphere. Replace the exponent 3 in the denominator with the number of dimensions for a more general result, e.g., for $n=2$ (a curve in the 2-dim space) what you get is the winding-number of the curve around $p$ multiplied by $2pi$.






          share|cite|improve this answer









          $endgroup$









          • 1




            $begingroup$
            I am going to stare really hard at this until i understand at least half
            $endgroup$
            – Makogan
            Nov 29 '18 at 23:00










          • $begingroup$
            Informally, think of the integrand as a small solid angle determined by rays traced from $p$ to a small portion of your surface around a point $x$ selected on the surface. E.g. see how it looks if your surface is a sphere of radius $r$ and $p$ is the origin of coordinates, then compute the integral in polar coord. On the other hand, if $p$ is outside the region enclosed by the manifold then by the Stokes theorem the integral has to be zero because our $omega = frac{(x-p)dS}{|x-p|^3}$ is a closed form and $domega = 0$. I believe I saw a similar example in Spivak's book on diff.geom.
            $endgroup$
            – mlerma54
            Nov 30 '18 at 3:34











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          $begingroup$

          I presume you are trying to determine is if a point $p$ is inside or outside the region $Omega$ of space enclosed by the manifold, which can be seen as the boundary $partial Omega$ of $Omega$. A solution is to use use Stokes–Cartan theorem:
          $$
          int_{partial Omega} omega = int_{Omega} domega
          $$

          with a suitable choice of the differential form $omega$. In our case the following will work, compute:
          $$
          I = int_{partial Omega} frac{(x-p)}{|x-p|^3} dS
          $$

          over the manifold, where $x$ is the (3-dim) variable of integration, and $dS$ is the 2-form representing the area element of the surface. If $p$ is outside $Omega$ then $I=0$. If $p$ is inside then $|I|$ yields the area of a unit sphere. Replace the exponent 3 in the denominator with the number of dimensions for a more general result, e.g., for $n=2$ (a curve in the 2-dim space) what you get is the winding-number of the curve around $p$ multiplied by $2pi$.






          share|cite|improve this answer









          $endgroup$









          • 1




            $begingroup$
            I am going to stare really hard at this until i understand at least half
            $endgroup$
            – Makogan
            Nov 29 '18 at 23:00










          • $begingroup$
            Informally, think of the integrand as a small solid angle determined by rays traced from $p$ to a small portion of your surface around a point $x$ selected on the surface. E.g. see how it looks if your surface is a sphere of radius $r$ and $p$ is the origin of coordinates, then compute the integral in polar coord. On the other hand, if $p$ is outside the region enclosed by the manifold then by the Stokes theorem the integral has to be zero because our $omega = frac{(x-p)dS}{|x-p|^3}$ is a closed form and $domega = 0$. I believe I saw a similar example in Spivak's book on diff.geom.
            $endgroup$
            – mlerma54
            Nov 30 '18 at 3:34
















          3












          $begingroup$

          I presume you are trying to determine is if a point $p$ is inside or outside the region $Omega$ of space enclosed by the manifold, which can be seen as the boundary $partial Omega$ of $Omega$. A solution is to use use Stokes–Cartan theorem:
          $$
          int_{partial Omega} omega = int_{Omega} domega
          $$

          with a suitable choice of the differential form $omega$. In our case the following will work, compute:
          $$
          I = int_{partial Omega} frac{(x-p)}{|x-p|^3} dS
          $$

          over the manifold, where $x$ is the (3-dim) variable of integration, and $dS$ is the 2-form representing the area element of the surface. If $p$ is outside $Omega$ then $I=0$. If $p$ is inside then $|I|$ yields the area of a unit sphere. Replace the exponent 3 in the denominator with the number of dimensions for a more general result, e.g., for $n=2$ (a curve in the 2-dim space) what you get is the winding-number of the curve around $p$ multiplied by $2pi$.






          share|cite|improve this answer









          $endgroup$









          • 1




            $begingroup$
            I am going to stare really hard at this until i understand at least half
            $endgroup$
            – Makogan
            Nov 29 '18 at 23:00










          • $begingroup$
            Informally, think of the integrand as a small solid angle determined by rays traced from $p$ to a small portion of your surface around a point $x$ selected on the surface. E.g. see how it looks if your surface is a sphere of radius $r$ and $p$ is the origin of coordinates, then compute the integral in polar coord. On the other hand, if $p$ is outside the region enclosed by the manifold then by the Stokes theorem the integral has to be zero because our $omega = frac{(x-p)dS}{|x-p|^3}$ is a closed form and $domega = 0$. I believe I saw a similar example in Spivak's book on diff.geom.
            $endgroup$
            – mlerma54
            Nov 30 '18 at 3:34














          3












          3








          3





          $begingroup$

          I presume you are trying to determine is if a point $p$ is inside or outside the region $Omega$ of space enclosed by the manifold, which can be seen as the boundary $partial Omega$ of $Omega$. A solution is to use use Stokes–Cartan theorem:
          $$
          int_{partial Omega} omega = int_{Omega} domega
          $$

          with a suitable choice of the differential form $omega$. In our case the following will work, compute:
          $$
          I = int_{partial Omega} frac{(x-p)}{|x-p|^3} dS
          $$

          over the manifold, where $x$ is the (3-dim) variable of integration, and $dS$ is the 2-form representing the area element of the surface. If $p$ is outside $Omega$ then $I=0$. If $p$ is inside then $|I|$ yields the area of a unit sphere. Replace the exponent 3 in the denominator with the number of dimensions for a more general result, e.g., for $n=2$ (a curve in the 2-dim space) what you get is the winding-number of the curve around $p$ multiplied by $2pi$.






          share|cite|improve this answer









          $endgroup$



          I presume you are trying to determine is if a point $p$ is inside or outside the region $Omega$ of space enclosed by the manifold, which can be seen as the boundary $partial Omega$ of $Omega$. A solution is to use use Stokes–Cartan theorem:
          $$
          int_{partial Omega} omega = int_{Omega} domega
          $$

          with a suitable choice of the differential form $omega$. In our case the following will work, compute:
          $$
          I = int_{partial Omega} frac{(x-p)}{|x-p|^3} dS
          $$

          over the manifold, where $x$ is the (3-dim) variable of integration, and $dS$ is the 2-form representing the area element of the surface. If $p$ is outside $Omega$ then $I=0$. If $p$ is inside then $|I|$ yields the area of a unit sphere. Replace the exponent 3 in the denominator with the number of dimensions for a more general result, e.g., for $n=2$ (a curve in the 2-dim space) what you get is the winding-number of the curve around $p$ multiplied by $2pi$.







          share|cite|improve this answer












          share|cite|improve this answer



          share|cite|improve this answer










          answered Nov 29 '18 at 22:56









          mlerma54mlerma54

          1,152148




          1,152148








          • 1




            $begingroup$
            I am going to stare really hard at this until i understand at least half
            $endgroup$
            – Makogan
            Nov 29 '18 at 23:00










          • $begingroup$
            Informally, think of the integrand as a small solid angle determined by rays traced from $p$ to a small portion of your surface around a point $x$ selected on the surface. E.g. see how it looks if your surface is a sphere of radius $r$ and $p$ is the origin of coordinates, then compute the integral in polar coord. On the other hand, if $p$ is outside the region enclosed by the manifold then by the Stokes theorem the integral has to be zero because our $omega = frac{(x-p)dS}{|x-p|^3}$ is a closed form and $domega = 0$. I believe I saw a similar example in Spivak's book on diff.geom.
            $endgroup$
            – mlerma54
            Nov 30 '18 at 3:34














          • 1




            $begingroup$
            I am going to stare really hard at this until i understand at least half
            $endgroup$
            – Makogan
            Nov 29 '18 at 23:00










          • $begingroup$
            Informally, think of the integrand as a small solid angle determined by rays traced from $p$ to a small portion of your surface around a point $x$ selected on the surface. E.g. see how it looks if your surface is a sphere of radius $r$ and $p$ is the origin of coordinates, then compute the integral in polar coord. On the other hand, if $p$ is outside the region enclosed by the manifold then by the Stokes theorem the integral has to be zero because our $omega = frac{(x-p)dS}{|x-p|^3}$ is a closed form and $domega = 0$. I believe I saw a similar example in Spivak's book on diff.geom.
            $endgroup$
            – mlerma54
            Nov 30 '18 at 3:34








          1




          1




          $begingroup$
          I am going to stare really hard at this until i understand at least half
          $endgroup$
          – Makogan
          Nov 29 '18 at 23:00




          $begingroup$
          I am going to stare really hard at this until i understand at least half
          $endgroup$
          – Makogan
          Nov 29 '18 at 23:00












          $begingroup$
          Informally, think of the integrand as a small solid angle determined by rays traced from $p$ to a small portion of your surface around a point $x$ selected on the surface. E.g. see how it looks if your surface is a sphere of radius $r$ and $p$ is the origin of coordinates, then compute the integral in polar coord. On the other hand, if $p$ is outside the region enclosed by the manifold then by the Stokes theorem the integral has to be zero because our $omega = frac{(x-p)dS}{|x-p|^3}$ is a closed form and $domega = 0$. I believe I saw a similar example in Spivak's book on diff.geom.
          $endgroup$
          – mlerma54
          Nov 30 '18 at 3:34




          $begingroup$
          Informally, think of the integrand as a small solid angle determined by rays traced from $p$ to a small portion of your surface around a point $x$ selected on the surface. E.g. see how it looks if your surface is a sphere of radius $r$ and $p$ is the origin of coordinates, then compute the integral in polar coord. On the other hand, if $p$ is outside the region enclosed by the manifold then by the Stokes theorem the integral has to be zero because our $omega = frac{(x-p)dS}{|x-p|^3}$ is a closed form and $domega = 0$. I believe I saw a similar example in Spivak's book on diff.geom.
          $endgroup$
          – mlerma54
          Nov 30 '18 at 3:34


















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