differential forms- $omega $ closed but not exact












3












$begingroup$


let be
$$ omega= |x|^{-3} left(x_1 dx_2 wedge dx_3+x_2dx_3 wedge dx_1 + x_3dx_1 wedge dx_2right) $$
and $G:= mathbb{R}^3 backslash { 0 } $



I want to prove, that $ omega$ is closed, but not exact



That $ omega $ is closed, I can prove it by looking if $ domega =0 $



But how can I prove it's not exact?



I know that a continous 2-form is exact in $G$ if there exists a 1-Form $y$ so, that $omega = dy $
how can I show there doesn't exist such $y$?





Edit:
Showing $int_S omega neq 0 $



Where $S$ is the unitsphere
Set $r=1$ and set
$$x_1= sin phi cos theta $$
$$x_2= sin phi sin theta$$
$$x_3= cos phi $$



$ theta=[0, 2pi], phi=[0, pi]$



then $ dx_1 wedge dx_2 = -sin phi cos phi dtheta wedge dphi $



$ dx_2 wedge dx_3 = -sin^2 phi cos theta dtheta wedge dphi $



$ dx_3 wedge dx_1 = -sin^2 phi sin theta d theta wedge dphi $



Putting in the equation:
$$ int_0^{2 pi} int_0^{ pi} |x| ( sin phi cos theta - sin^2 phi cos theta ~d theta wedge d phi \+ sin phi sin theta -sin^2 phi sin theta ~dtheta wedge dphi + cos phi -sin phi cos phi~ d theta wedge dphi $$



what do I put for $x$ ?
I don't know how to solve the integral
thank you for any help!










share|cite|improve this question











$endgroup$








  • 1




    $begingroup$
    The first thing to try would be to integrate it on the unit sphere; if the result is not zero, then $omega$ is not exact.
    $endgroup$
    – Alex Provost
    Jan 16 at 12:42










  • $begingroup$
    @AlexProvost What does it mean to integrate the unit sphere?
    $endgroup$
    – MathOverview
    Jan 16 at 12:43










  • $begingroup$
    @MathOverview I said to "integrate it on the unit sphere", meaning the 2-form.
    $endgroup$
    – Alex Provost
    Jan 16 at 12:44










  • $begingroup$
    @AlexProvost But why integrate in the unitary sphere and not in $ G $?
    $endgroup$
    – MathOverview
    Jan 16 at 12:46






  • 1




    $begingroup$
    On the unit sphere, $|x| = 1$. By the way, this reduces to the standard volume form on $S^2$, so you expect the integral to yield the surface area, $4pi$.
    $endgroup$
    – Alex Provost
    Jan 16 at 13:42
















3












$begingroup$


let be
$$ omega= |x|^{-3} left(x_1 dx_2 wedge dx_3+x_2dx_3 wedge dx_1 + x_3dx_1 wedge dx_2right) $$
and $G:= mathbb{R}^3 backslash { 0 } $



I want to prove, that $ omega$ is closed, but not exact



That $ omega $ is closed, I can prove it by looking if $ domega =0 $



But how can I prove it's not exact?



I know that a continous 2-form is exact in $G$ if there exists a 1-Form $y$ so, that $omega = dy $
how can I show there doesn't exist such $y$?





Edit:
Showing $int_S omega neq 0 $



Where $S$ is the unitsphere
Set $r=1$ and set
$$x_1= sin phi cos theta $$
$$x_2= sin phi sin theta$$
$$x_3= cos phi $$



$ theta=[0, 2pi], phi=[0, pi]$



then $ dx_1 wedge dx_2 = -sin phi cos phi dtheta wedge dphi $



$ dx_2 wedge dx_3 = -sin^2 phi cos theta dtheta wedge dphi $



$ dx_3 wedge dx_1 = -sin^2 phi sin theta d theta wedge dphi $



Putting in the equation:
$$ int_0^{2 pi} int_0^{ pi} |x| ( sin phi cos theta - sin^2 phi cos theta ~d theta wedge d phi \+ sin phi sin theta -sin^2 phi sin theta ~dtheta wedge dphi + cos phi -sin phi cos phi~ d theta wedge dphi $$



what do I put for $x$ ?
I don't know how to solve the integral
thank you for any help!










share|cite|improve this question











$endgroup$








  • 1




    $begingroup$
    The first thing to try would be to integrate it on the unit sphere; if the result is not zero, then $omega$ is not exact.
    $endgroup$
    – Alex Provost
    Jan 16 at 12:42










  • $begingroup$
    @AlexProvost What does it mean to integrate the unit sphere?
    $endgroup$
    – MathOverview
    Jan 16 at 12:43










  • $begingroup$
    @MathOverview I said to "integrate it on the unit sphere", meaning the 2-form.
    $endgroup$
    – Alex Provost
    Jan 16 at 12:44










  • $begingroup$
    @AlexProvost But why integrate in the unitary sphere and not in $ G $?
    $endgroup$
    – MathOverview
    Jan 16 at 12:46






  • 1




    $begingroup$
    On the unit sphere, $|x| = 1$. By the way, this reduces to the standard volume form on $S^2$, so you expect the integral to yield the surface area, $4pi$.
    $endgroup$
    – Alex Provost
    Jan 16 at 13:42














3












3








3





$begingroup$


let be
$$ omega= |x|^{-3} left(x_1 dx_2 wedge dx_3+x_2dx_3 wedge dx_1 + x_3dx_1 wedge dx_2right) $$
and $G:= mathbb{R}^3 backslash { 0 } $



I want to prove, that $ omega$ is closed, but not exact



That $ omega $ is closed, I can prove it by looking if $ domega =0 $



But how can I prove it's not exact?



I know that a continous 2-form is exact in $G$ if there exists a 1-Form $y$ so, that $omega = dy $
how can I show there doesn't exist such $y$?





Edit:
Showing $int_S omega neq 0 $



Where $S$ is the unitsphere
Set $r=1$ and set
$$x_1= sin phi cos theta $$
$$x_2= sin phi sin theta$$
$$x_3= cos phi $$



$ theta=[0, 2pi], phi=[0, pi]$



then $ dx_1 wedge dx_2 = -sin phi cos phi dtheta wedge dphi $



$ dx_2 wedge dx_3 = -sin^2 phi cos theta dtheta wedge dphi $



$ dx_3 wedge dx_1 = -sin^2 phi sin theta d theta wedge dphi $



Putting in the equation:
$$ int_0^{2 pi} int_0^{ pi} |x| ( sin phi cos theta - sin^2 phi cos theta ~d theta wedge d phi \+ sin phi sin theta -sin^2 phi sin theta ~dtheta wedge dphi + cos phi -sin phi cos phi~ d theta wedge dphi $$



what do I put for $x$ ?
I don't know how to solve the integral
thank you for any help!










share|cite|improve this question











$endgroup$




let be
$$ omega= |x|^{-3} left(x_1 dx_2 wedge dx_3+x_2dx_3 wedge dx_1 + x_3dx_1 wedge dx_2right) $$
and $G:= mathbb{R}^3 backslash { 0 } $



I want to prove, that $ omega$ is closed, but not exact



That $ omega $ is closed, I can prove it by looking if $ domega =0 $



But how can I prove it's not exact?



I know that a continous 2-form is exact in $G$ if there exists a 1-Form $y$ so, that $omega = dy $
how can I show there doesn't exist such $y$?





Edit:
Showing $int_S omega neq 0 $



Where $S$ is the unitsphere
Set $r=1$ and set
$$x_1= sin phi cos theta $$
$$x_2= sin phi sin theta$$
$$x_3= cos phi $$



$ theta=[0, 2pi], phi=[0, pi]$



then $ dx_1 wedge dx_2 = -sin phi cos phi dtheta wedge dphi $



$ dx_2 wedge dx_3 = -sin^2 phi cos theta dtheta wedge dphi $



$ dx_3 wedge dx_1 = -sin^2 phi sin theta d theta wedge dphi $



Putting in the equation:
$$ int_0^{2 pi} int_0^{ pi} |x| ( sin phi cos theta - sin^2 phi cos theta ~d theta wedge d phi \+ sin phi sin theta -sin^2 phi sin theta ~dtheta wedge dphi + cos phi -sin phi cos phi~ d theta wedge dphi $$



what do I put for $x$ ?
I don't know how to solve the integral
thank you for any help!







real-analysis multivariable-calculus differential-forms






share|cite|improve this question















share|cite|improve this question













share|cite|improve this question




share|cite|improve this question








edited Jan 16 at 14:16









John Hughes

65.2k24293




65.2k24293










asked Jan 16 at 12:32









wondering1123wondering1123

14911




14911








  • 1




    $begingroup$
    The first thing to try would be to integrate it on the unit sphere; if the result is not zero, then $omega$ is not exact.
    $endgroup$
    – Alex Provost
    Jan 16 at 12:42










  • $begingroup$
    @AlexProvost What does it mean to integrate the unit sphere?
    $endgroup$
    – MathOverview
    Jan 16 at 12:43










  • $begingroup$
    @MathOverview I said to "integrate it on the unit sphere", meaning the 2-form.
    $endgroup$
    – Alex Provost
    Jan 16 at 12:44










  • $begingroup$
    @AlexProvost But why integrate in the unitary sphere and not in $ G $?
    $endgroup$
    – MathOverview
    Jan 16 at 12:46






  • 1




    $begingroup$
    On the unit sphere, $|x| = 1$. By the way, this reduces to the standard volume form on $S^2$, so you expect the integral to yield the surface area, $4pi$.
    $endgroup$
    – Alex Provost
    Jan 16 at 13:42














  • 1




    $begingroup$
    The first thing to try would be to integrate it on the unit sphere; if the result is not zero, then $omega$ is not exact.
    $endgroup$
    – Alex Provost
    Jan 16 at 12:42










  • $begingroup$
    @AlexProvost What does it mean to integrate the unit sphere?
    $endgroup$
    – MathOverview
    Jan 16 at 12:43










  • $begingroup$
    @MathOverview I said to "integrate it on the unit sphere", meaning the 2-form.
    $endgroup$
    – Alex Provost
    Jan 16 at 12:44










  • $begingroup$
    @AlexProvost But why integrate in the unitary sphere and not in $ G $?
    $endgroup$
    – MathOverview
    Jan 16 at 12:46






  • 1




    $begingroup$
    On the unit sphere, $|x| = 1$. By the way, this reduces to the standard volume form on $S^2$, so you expect the integral to yield the surface area, $4pi$.
    $endgroup$
    – Alex Provost
    Jan 16 at 13:42








1




1




$begingroup$
The first thing to try would be to integrate it on the unit sphere; if the result is not zero, then $omega$ is not exact.
$endgroup$
– Alex Provost
Jan 16 at 12:42




$begingroup$
The first thing to try would be to integrate it on the unit sphere; if the result is not zero, then $omega$ is not exact.
$endgroup$
– Alex Provost
Jan 16 at 12:42












$begingroup$
@AlexProvost What does it mean to integrate the unit sphere?
$endgroup$
– MathOverview
Jan 16 at 12:43




$begingroup$
@AlexProvost What does it mean to integrate the unit sphere?
$endgroup$
– MathOverview
Jan 16 at 12:43












$begingroup$
@MathOverview I said to "integrate it on the unit sphere", meaning the 2-form.
$endgroup$
– Alex Provost
Jan 16 at 12:44




$begingroup$
@MathOverview I said to "integrate it on the unit sphere", meaning the 2-form.
$endgroup$
– Alex Provost
Jan 16 at 12:44












$begingroup$
@AlexProvost But why integrate in the unitary sphere and not in $ G $?
$endgroup$
– MathOverview
Jan 16 at 12:46




$begingroup$
@AlexProvost But why integrate in the unitary sphere and not in $ G $?
$endgroup$
– MathOverview
Jan 16 at 12:46




1




1




$begingroup$
On the unit sphere, $|x| = 1$. By the way, this reduces to the standard volume form on $S^2$, so you expect the integral to yield the surface area, $4pi$.
$endgroup$
– Alex Provost
Jan 16 at 13:42




$begingroup$
On the unit sphere, $|x| = 1$. By the way, this reduces to the standard volume form on $S^2$, so you expect the integral to yield the surface area, $4pi$.
$endgroup$
– Alex Provost
Jan 16 at 13:42










1 Answer
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$begingroup$

Switch to spherical coordinates and integrate $omega$ on the unit sphere $r = 1$. Let $theta,phi$ denote the azimuth and polar angles, respectively; then $$dx = cos theta sin phi , dr - sin theta sin phi , dtheta + costheta cos phi , dphi$$
$$ dy = sin theta sin phi , dr + cos theta sinphi , dtheta + sin theta cos phi , dphi $$
$$dz = cos phi , dr - sinphi , dphi$$



and after some algebra we find that $omega = sinphi , dphi wedge dtheta$. Hence $$int_{S^2} omega = int_0^{2pi} int_0^pi sin phi , dphi , dtheta = 2cdot 2pi = 4pi.$$



This is the expected answer, namely the surface area of the sphere, as $omega$ restricted to $S^2$ is precisely the volume form induced by that of $mathbb R^3$. And since the integral is not zero, $omega$ cannot be exact, lest Stoke's theorem be violated.






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    $begingroup$

    Switch to spherical coordinates and integrate $omega$ on the unit sphere $r = 1$. Let $theta,phi$ denote the azimuth and polar angles, respectively; then $$dx = cos theta sin phi , dr - sin theta sin phi , dtheta + costheta cos phi , dphi$$
    $$ dy = sin theta sin phi , dr + cos theta sinphi , dtheta + sin theta cos phi , dphi $$
    $$dz = cos phi , dr - sinphi , dphi$$



    and after some algebra we find that $omega = sinphi , dphi wedge dtheta$. Hence $$int_{S^2} omega = int_0^{2pi} int_0^pi sin phi , dphi , dtheta = 2cdot 2pi = 4pi.$$



    This is the expected answer, namely the surface area of the sphere, as $omega$ restricted to $S^2$ is precisely the volume form induced by that of $mathbb R^3$. And since the integral is not zero, $omega$ cannot be exact, lest Stoke's theorem be violated.






    share|cite|improve this answer











    $endgroup$


















      2












      $begingroup$

      Switch to spherical coordinates and integrate $omega$ on the unit sphere $r = 1$. Let $theta,phi$ denote the azimuth and polar angles, respectively; then $$dx = cos theta sin phi , dr - sin theta sin phi , dtheta + costheta cos phi , dphi$$
      $$ dy = sin theta sin phi , dr + cos theta sinphi , dtheta + sin theta cos phi , dphi $$
      $$dz = cos phi , dr - sinphi , dphi$$



      and after some algebra we find that $omega = sinphi , dphi wedge dtheta$. Hence $$int_{S^2} omega = int_0^{2pi} int_0^pi sin phi , dphi , dtheta = 2cdot 2pi = 4pi.$$



      This is the expected answer, namely the surface area of the sphere, as $omega$ restricted to $S^2$ is precisely the volume form induced by that of $mathbb R^3$. And since the integral is not zero, $omega$ cannot be exact, lest Stoke's theorem be violated.






      share|cite|improve this answer











      $endgroup$
















        2












        2








        2





        $begingroup$

        Switch to spherical coordinates and integrate $omega$ on the unit sphere $r = 1$. Let $theta,phi$ denote the azimuth and polar angles, respectively; then $$dx = cos theta sin phi , dr - sin theta sin phi , dtheta + costheta cos phi , dphi$$
        $$ dy = sin theta sin phi , dr + cos theta sinphi , dtheta + sin theta cos phi , dphi $$
        $$dz = cos phi , dr - sinphi , dphi$$



        and after some algebra we find that $omega = sinphi , dphi wedge dtheta$. Hence $$int_{S^2} omega = int_0^{2pi} int_0^pi sin phi , dphi , dtheta = 2cdot 2pi = 4pi.$$



        This is the expected answer, namely the surface area of the sphere, as $omega$ restricted to $S^2$ is precisely the volume form induced by that of $mathbb R^3$. And since the integral is not zero, $omega$ cannot be exact, lest Stoke's theorem be violated.






        share|cite|improve this answer











        $endgroup$



        Switch to spherical coordinates and integrate $omega$ on the unit sphere $r = 1$. Let $theta,phi$ denote the azimuth and polar angles, respectively; then $$dx = cos theta sin phi , dr - sin theta sin phi , dtheta + costheta cos phi , dphi$$
        $$ dy = sin theta sin phi , dr + cos theta sinphi , dtheta + sin theta cos phi , dphi $$
        $$dz = cos phi , dr - sinphi , dphi$$



        and after some algebra we find that $omega = sinphi , dphi wedge dtheta$. Hence $$int_{S^2} omega = int_0^{2pi} int_0^pi sin phi , dphi , dtheta = 2cdot 2pi = 4pi.$$



        This is the expected answer, namely the surface area of the sphere, as $omega$ restricted to $S^2$ is precisely the volume form induced by that of $mathbb R^3$. And since the integral is not zero, $omega$ cannot be exact, lest Stoke's theorem be violated.







        share|cite|improve this answer














        share|cite|improve this answer



        share|cite|improve this answer








        edited Jan 16 at 20:54

























        answered Jan 16 at 17:32









        Alex ProvostAlex Provost

        15.6k22351




        15.6k22351






























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