Calculate integral where S is the surface of the half ball $x^2 + y^2 + z^2 = 1, space z geq 0,$ and $F = (x...












0














I am asked to calculate this integral and want to make sure I am doing this set up correctly, So I tried to paramatize this surface by :



$x = rcos(theta), space y = rsin(theta), space z = sqrt{1 - r}$



$0 leq r leq 1 $ and $ 0 leq theta leq 2pi$



then I found :



$Phi_{theta} = -rsin(theta)i + rcos(theta)j + 0k , space Phi_{r} = cos(theta)i + sin(theta)j + frac{1}{2sqrt{1-r}}k$



which would make:



$Phi_{theta} times Phi_{r} = frac{1}{2}bigl(frac{rcos(theta)}{sqrt{1-r}}bigr)i + frac{1}{2}bigl(frac{rsin(theta)}{sqrt{1-r}}bigr)j -rk$



then my surface integral would be :



$ int_0^{2pi} int_0^1 ((rcos(theta) + 3(rsin(theta))^5)i + (rsin(theta) + 10(rcos(theta))(sqrt{1 - r}))j + (sqrt{1 - r} - (rcos(theta)rsin(theta))k )space cdot (frac{1}{2}bigl(frac{rcos(theta)}{sqrt{1-r}}bigr)i + frac{1}{2}bigl(frac{rsin(theta)}{sqrt{1-r}}bigr)j -rk )$



is this set up correct ? I have tried to reduce it after taking the dot product with the trig identity's but I still end up with a fairly complicated expression










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  • 3




    It should be $z = sqrt{1-r^2}$, not $sqrt{1-r}$.
    – Nick
    Nov 21 at 23:17
















0














I am asked to calculate this integral and want to make sure I am doing this set up correctly, So I tried to paramatize this surface by :



$x = rcos(theta), space y = rsin(theta), space z = sqrt{1 - r}$



$0 leq r leq 1 $ and $ 0 leq theta leq 2pi$



then I found :



$Phi_{theta} = -rsin(theta)i + rcos(theta)j + 0k , space Phi_{r} = cos(theta)i + sin(theta)j + frac{1}{2sqrt{1-r}}k$



which would make:



$Phi_{theta} times Phi_{r} = frac{1}{2}bigl(frac{rcos(theta)}{sqrt{1-r}}bigr)i + frac{1}{2}bigl(frac{rsin(theta)}{sqrt{1-r}}bigr)j -rk$



then my surface integral would be :



$ int_0^{2pi} int_0^1 ((rcos(theta) + 3(rsin(theta))^5)i + (rsin(theta) + 10(rcos(theta))(sqrt{1 - r}))j + (sqrt{1 - r} - (rcos(theta)rsin(theta))k )space cdot (frac{1}{2}bigl(frac{rcos(theta)}{sqrt{1-r}}bigr)i + frac{1}{2}bigl(frac{rsin(theta)}{sqrt{1-r}}bigr)j -rk )$



is this set up correct ? I have tried to reduce it after taking the dot product with the trig identity's but I still end up with a fairly complicated expression










share|cite|improve this question




















  • 3




    It should be $z = sqrt{1-r^2}$, not $sqrt{1-r}$.
    – Nick
    Nov 21 at 23:17














0












0








0


0





I am asked to calculate this integral and want to make sure I am doing this set up correctly, So I tried to paramatize this surface by :



$x = rcos(theta), space y = rsin(theta), space z = sqrt{1 - r}$



$0 leq r leq 1 $ and $ 0 leq theta leq 2pi$



then I found :



$Phi_{theta} = -rsin(theta)i + rcos(theta)j + 0k , space Phi_{r} = cos(theta)i + sin(theta)j + frac{1}{2sqrt{1-r}}k$



which would make:



$Phi_{theta} times Phi_{r} = frac{1}{2}bigl(frac{rcos(theta)}{sqrt{1-r}}bigr)i + frac{1}{2}bigl(frac{rsin(theta)}{sqrt{1-r}}bigr)j -rk$



then my surface integral would be :



$ int_0^{2pi} int_0^1 ((rcos(theta) + 3(rsin(theta))^5)i + (rsin(theta) + 10(rcos(theta))(sqrt{1 - r}))j + (sqrt{1 - r} - (rcos(theta)rsin(theta))k )space cdot (frac{1}{2}bigl(frac{rcos(theta)}{sqrt{1-r}}bigr)i + frac{1}{2}bigl(frac{rsin(theta)}{sqrt{1-r}}bigr)j -rk )$



is this set up correct ? I have tried to reduce it after taking the dot product with the trig identity's but I still end up with a fairly complicated expression










share|cite|improve this question















I am asked to calculate this integral and want to make sure I am doing this set up correctly, So I tried to paramatize this surface by :



$x = rcos(theta), space y = rsin(theta), space z = sqrt{1 - r}$



$0 leq r leq 1 $ and $ 0 leq theta leq 2pi$



then I found :



$Phi_{theta} = -rsin(theta)i + rcos(theta)j + 0k , space Phi_{r} = cos(theta)i + sin(theta)j + frac{1}{2sqrt{1-r}}k$



which would make:



$Phi_{theta} times Phi_{r} = frac{1}{2}bigl(frac{rcos(theta)}{sqrt{1-r}}bigr)i + frac{1}{2}bigl(frac{rsin(theta)}{sqrt{1-r}}bigr)j -rk$



then my surface integral would be :



$ int_0^{2pi} int_0^1 ((rcos(theta) + 3(rsin(theta))^5)i + (rsin(theta) + 10(rcos(theta))(sqrt{1 - r}))j + (sqrt{1 - r} - (rcos(theta)rsin(theta))k )space cdot (frac{1}{2}bigl(frac{rcos(theta)}{sqrt{1-r}}bigr)i + frac{1}{2}bigl(frac{rsin(theta)}{sqrt{1-r}}bigr)j -rk )$



is this set up correct ? I have tried to reduce it after taking the dot product with the trig identity's but I still end up with a fairly complicated expression







multivariable-calculus trigonometry surface-integrals






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edited Nov 24 at 23:07

























asked Nov 21 at 23:14









Doug Ray

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  • 3




    It should be $z = sqrt{1-r^2}$, not $sqrt{1-r}$.
    – Nick
    Nov 21 at 23:17














  • 3




    It should be $z = sqrt{1-r^2}$, not $sqrt{1-r}$.
    – Nick
    Nov 21 at 23:17








3




3




It should be $z = sqrt{1-r^2}$, not $sqrt{1-r}$.
– Nick
Nov 21 at 23:17




It should be $z = sqrt{1-r^2}$, not $sqrt{1-r}$.
– Nick
Nov 21 at 23:17










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The problem is ambiguous. If the surface of the half ball includes the flat surface at $z=0$ the problem simplifies to a very simple integral using the divergence theorem. If not, the problem simplifies too but needs to calculate the flux through that flat surface.



1.- For the flat surface included ($B$ is the half ball, $partial B$ its surface and $mathbf F=F_xmathbf i+F_ymathbf j+F_zmathbf k$), the divergence theorem gives:



$$phi=int_{partial B}mathbf F·mathbb dmathbf S=int_Bnabla·mathbf F,mathbb dV$$



$$nabla·mathbf F=dfrac{partial F_x}{partial x}+dfrac{partial F_y}{partial y}+dfrac{partial F_z}{partial z}=1+1+1=3$$



In spherical coordinates $(r,theta,phi)$



$$phi=int_B 3mathbb d V=int_0^1int_0^{pi/2}int_o^{2pi}3r^2sintheta,mathbb dphi,mathbb dtheta,mathbb d r=2pi$$



2.- If the flat surface, $D={x^2+y^2leq 1;z=0}$, is not included we need to subtract the flux through it:



For the surface element with its vector pointing outwards is $-mathbf k$:



$$mathbb dmathbf S=-mathbb dxmathbb dy,mathbf k$$



For the flux through the surface element ($z=0$):



$$mathbf F·mathbb dmathbf S=((x + 3y^5)mathbf i + (y + 10xz)mathbf j + (z - xy)mathbf k)·(-mathbb dxmathbb dy,mathbf k)=xy,mathbb dxmathbb dy$$



$$phi_D=int_{-1}^1int_{-sqrt{1-x^2}}^{sqrt{1-x^2}}xy,mathbb dxmathbb dy=0$$



The flux is zero. It seems that in any case the answer is $2pi$






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    The problem is ambiguous. If the surface of the half ball includes the flat surface at $z=0$ the problem simplifies to a very simple integral using the divergence theorem. If not, the problem simplifies too but needs to calculate the flux through that flat surface.



    1.- For the flat surface included ($B$ is the half ball, $partial B$ its surface and $mathbf F=F_xmathbf i+F_ymathbf j+F_zmathbf k$), the divergence theorem gives:



    $$phi=int_{partial B}mathbf F·mathbb dmathbf S=int_Bnabla·mathbf F,mathbb dV$$



    $$nabla·mathbf F=dfrac{partial F_x}{partial x}+dfrac{partial F_y}{partial y}+dfrac{partial F_z}{partial z}=1+1+1=3$$



    In spherical coordinates $(r,theta,phi)$



    $$phi=int_B 3mathbb d V=int_0^1int_0^{pi/2}int_o^{2pi}3r^2sintheta,mathbb dphi,mathbb dtheta,mathbb d r=2pi$$



    2.- If the flat surface, $D={x^2+y^2leq 1;z=0}$, is not included we need to subtract the flux through it:



    For the surface element with its vector pointing outwards is $-mathbf k$:



    $$mathbb dmathbf S=-mathbb dxmathbb dy,mathbf k$$



    For the flux through the surface element ($z=0$):



    $$mathbf F·mathbb dmathbf S=((x + 3y^5)mathbf i + (y + 10xz)mathbf j + (z - xy)mathbf k)·(-mathbb dxmathbb dy,mathbf k)=xy,mathbb dxmathbb dy$$



    $$phi_D=int_{-1}^1int_{-sqrt{1-x^2}}^{sqrt{1-x^2}}xy,mathbb dxmathbb dy=0$$



    The flux is zero. It seems that in any case the answer is $2pi$






    share|cite|improve this answer




























      0














      The problem is ambiguous. If the surface of the half ball includes the flat surface at $z=0$ the problem simplifies to a very simple integral using the divergence theorem. If not, the problem simplifies too but needs to calculate the flux through that flat surface.



      1.- For the flat surface included ($B$ is the half ball, $partial B$ its surface and $mathbf F=F_xmathbf i+F_ymathbf j+F_zmathbf k$), the divergence theorem gives:



      $$phi=int_{partial B}mathbf F·mathbb dmathbf S=int_Bnabla·mathbf F,mathbb dV$$



      $$nabla·mathbf F=dfrac{partial F_x}{partial x}+dfrac{partial F_y}{partial y}+dfrac{partial F_z}{partial z}=1+1+1=3$$



      In spherical coordinates $(r,theta,phi)$



      $$phi=int_B 3mathbb d V=int_0^1int_0^{pi/2}int_o^{2pi}3r^2sintheta,mathbb dphi,mathbb dtheta,mathbb d r=2pi$$



      2.- If the flat surface, $D={x^2+y^2leq 1;z=0}$, is not included we need to subtract the flux through it:



      For the surface element with its vector pointing outwards is $-mathbf k$:



      $$mathbb dmathbf S=-mathbb dxmathbb dy,mathbf k$$



      For the flux through the surface element ($z=0$):



      $$mathbf F·mathbb dmathbf S=((x + 3y^5)mathbf i + (y + 10xz)mathbf j + (z - xy)mathbf k)·(-mathbb dxmathbb dy,mathbf k)=xy,mathbb dxmathbb dy$$



      $$phi_D=int_{-1}^1int_{-sqrt{1-x^2}}^{sqrt{1-x^2}}xy,mathbb dxmathbb dy=0$$



      The flux is zero. It seems that in any case the answer is $2pi$






      share|cite|improve this answer


























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        0






        The problem is ambiguous. If the surface of the half ball includes the flat surface at $z=0$ the problem simplifies to a very simple integral using the divergence theorem. If not, the problem simplifies too but needs to calculate the flux through that flat surface.



        1.- For the flat surface included ($B$ is the half ball, $partial B$ its surface and $mathbf F=F_xmathbf i+F_ymathbf j+F_zmathbf k$), the divergence theorem gives:



        $$phi=int_{partial B}mathbf F·mathbb dmathbf S=int_Bnabla·mathbf F,mathbb dV$$



        $$nabla·mathbf F=dfrac{partial F_x}{partial x}+dfrac{partial F_y}{partial y}+dfrac{partial F_z}{partial z}=1+1+1=3$$



        In spherical coordinates $(r,theta,phi)$



        $$phi=int_B 3mathbb d V=int_0^1int_0^{pi/2}int_o^{2pi}3r^2sintheta,mathbb dphi,mathbb dtheta,mathbb d r=2pi$$



        2.- If the flat surface, $D={x^2+y^2leq 1;z=0}$, is not included we need to subtract the flux through it:



        For the surface element with its vector pointing outwards is $-mathbf k$:



        $$mathbb dmathbf S=-mathbb dxmathbb dy,mathbf k$$



        For the flux through the surface element ($z=0$):



        $$mathbf F·mathbb dmathbf S=((x + 3y^5)mathbf i + (y + 10xz)mathbf j + (z - xy)mathbf k)·(-mathbb dxmathbb dy,mathbf k)=xy,mathbb dxmathbb dy$$



        $$phi_D=int_{-1}^1int_{-sqrt{1-x^2}}^{sqrt{1-x^2}}xy,mathbb dxmathbb dy=0$$



        The flux is zero. It seems that in any case the answer is $2pi$






        share|cite|improve this answer














        The problem is ambiguous. If the surface of the half ball includes the flat surface at $z=0$ the problem simplifies to a very simple integral using the divergence theorem. If not, the problem simplifies too but needs to calculate the flux through that flat surface.



        1.- For the flat surface included ($B$ is the half ball, $partial B$ its surface and $mathbf F=F_xmathbf i+F_ymathbf j+F_zmathbf k$), the divergence theorem gives:



        $$phi=int_{partial B}mathbf F·mathbb dmathbf S=int_Bnabla·mathbf F,mathbb dV$$



        $$nabla·mathbf F=dfrac{partial F_x}{partial x}+dfrac{partial F_y}{partial y}+dfrac{partial F_z}{partial z}=1+1+1=3$$



        In spherical coordinates $(r,theta,phi)$



        $$phi=int_B 3mathbb d V=int_0^1int_0^{pi/2}int_o^{2pi}3r^2sintheta,mathbb dphi,mathbb dtheta,mathbb d r=2pi$$



        2.- If the flat surface, $D={x^2+y^2leq 1;z=0}$, is not included we need to subtract the flux through it:



        For the surface element with its vector pointing outwards is $-mathbf k$:



        $$mathbb dmathbf S=-mathbb dxmathbb dy,mathbf k$$



        For the flux through the surface element ($z=0$):



        $$mathbf F·mathbb dmathbf S=((x + 3y^5)mathbf i + (y + 10xz)mathbf j + (z - xy)mathbf k)·(-mathbb dxmathbb dy,mathbf k)=xy,mathbb dxmathbb dy$$



        $$phi_D=int_{-1}^1int_{-sqrt{1-x^2}}^{sqrt{1-x^2}}xy,mathbb dxmathbb dy=0$$



        The flux is zero. It seems that in any case the answer is $2pi$







        share|cite|improve this answer














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        edited Nov 22 at 13:26

























        answered Nov 22 at 9:31









        Rafa Budría

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