Integral of 1-form $omega=dfrac-y ,dx + x ,dyx^2 +y^2$ over a triangle.

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I'm trying to evaluate the integral of the $1$-form




$$omega=dfrac-y ,dx +x,dyx^2 +y^2$$




through the corners of a triangle with the vertices $A= (-5,-2)$, $B=(5,-2)$, $C=(0,3)$.



I've tried to use Green's theorem but it didn't work because the 1-form isn't differentiable on (0,0) so I had to parametrize the paths from each point and got three line integrals but it got so complicated at the end, so it doesn't seem to be the right solution or at least the one I'm supposed to calculate. Is there anyway else to evaluate the integral?







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    up vote
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    down vote

    favorite












    I'm trying to evaluate the integral of the $1$-form




    $$omega=dfrac-y ,dx +x,dyx^2 +y^2$$




    through the corners of a triangle with the vertices $A= (-5,-2)$, $B=(5,-2)$, $C=(0,3)$.



    I've tried to use Green's theorem but it didn't work because the 1-form isn't differentiable on (0,0) so I had to parametrize the paths from each point and got three line integrals but it got so complicated at the end, so it doesn't seem to be the right solution or at least the one I'm supposed to calculate. Is there anyway else to evaluate the integral?







    share|cite|improve this question























      up vote
      0
      down vote

      favorite









      up vote
      0
      down vote

      favorite











      I'm trying to evaluate the integral of the $1$-form




      $$omega=dfrac-y ,dx +x,dyx^2 +y^2$$




      through the corners of a triangle with the vertices $A= (-5,-2)$, $B=(5,-2)$, $C=(0,3)$.



      I've tried to use Green's theorem but it didn't work because the 1-form isn't differentiable on (0,0) so I had to parametrize the paths from each point and got three line integrals but it got so complicated at the end, so it doesn't seem to be the right solution or at least the one I'm supposed to calculate. Is there anyway else to evaluate the integral?







      share|cite|improve this question













      I'm trying to evaluate the integral of the $1$-form




      $$omega=dfrac-y ,dx +x,dyx^2 +y^2$$




      through the corners of a triangle with the vertices $A= (-5,-2)$, $B=(5,-2)$, $C=(0,3)$.



      I've tried to use Green's theorem but it didn't work because the 1-form isn't differentiable on (0,0) so I had to parametrize the paths from each point and got three line integrals but it got so complicated at the end, so it doesn't seem to be the right solution or at least the one I'm supposed to calculate. Is there anyway else to evaluate the integral?









      share|cite|improve this question












      share|cite|improve this question




      share|cite|improve this question








      edited yesterday









      Michael Hardy

      204k23185460




      204k23185460









      asked yesterday









      Mohamed Mossad

      102




      102




















          2 Answers
          2






          active

          oldest

          votes

















          up vote
          2
          down vote



          accepted










          We know that
          $$omega=dfrac-y ,dx +x,dyx^2 +y^2=darctandfracyx$$
          is an exact differential and the area $Delta$ includes the origin, since the $arctandfracyx$ winds around the origin one time then
          $$int_Delta omega=2pi$$






          share|cite|improve this answer























          • May I ask how did you come to that answer? like what's intuitive about it? I know that 1-form is quite well-known but I am supposed to calculate the integral not use a trigonometric function which I don't know.
            – Mohamed Mossad
            yesterday










          • When you have an exact differential over a closed area, and while it winds around the origin $n$ times then it's integral is $2pi n$. Also as you said you can't apply green thm, except these you are forced to parametrize the triangle and substitude them in the exact form.
            – user 108128
            yesterday











          • My script says $omega$ is not exact because there's no function f such that $df= omega$ even though $domega = 0$, for $omega$ on $R^2 0$
            – Mohamed Mossad
            yesterday


















          up vote
          1
          down vote













          This is essentially a long comment to the other answer, but worth making an answer of its own, since it highlights a useful trick which also works for Stoke's Theorem, as well as explains the $2 pi n$ answer. It's true that you can't apply Green's theorem to this problem directly, since the function contains a pole at the origin, but this doesn't stop you from applying Green's theorem on other regions that may also be useful.



          Observe that your triangle $T$ does not pass through the origin. This means that you can find a small disk inside the triangle containing the origin $D$. Now consider the region $T - D$. This has two boundary components with opposite orientations, and we can consider the integral over $T - D$.



          This gives us:



          $$int_textinterior of T - D d omega = int_T omega - int_D omega$$ by Green's Theorem (or the Stoke's Theorem for differential forms, if you prefer to call it this). You can check that on this region, the left integral is $0$, as $d omega$ is $0$ everywhere here. This means that you can replace the integral of $T$ with the integral over any nice circle you like encompassing the origin, since the left side is $0$.



          Now recognize that this integral is super friendly to polar coordinates, and convert to these. You will get the correct answer.






          share|cite|improve this answer





















          • I know it's friendly to calculate in polar coordinates because I had an example of it on $c:[0,2pi] rightarrow R^2$ with $t rightarrow (cos t, sin t)$ which is equal $2pi$ when $omega$ isn't defined on 0, but is it the same with the triangle which doesn't pass through the origin?
            – Mohamed Mossad
            yesterday











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          2 Answers
          2






          active

          oldest

          votes








          2 Answers
          2






          active

          oldest

          votes









          active

          oldest

          votes






          active

          oldest

          votes








          up vote
          2
          down vote



          accepted










          We know that
          $$omega=dfrac-y ,dx +x,dyx^2 +y^2=darctandfracyx$$
          is an exact differential and the area $Delta$ includes the origin, since the $arctandfracyx$ winds around the origin one time then
          $$int_Delta omega=2pi$$






          share|cite|improve this answer























          • May I ask how did you come to that answer? like what's intuitive about it? I know that 1-form is quite well-known but I am supposed to calculate the integral not use a trigonometric function which I don't know.
            – Mohamed Mossad
            yesterday










          • When you have an exact differential over a closed area, and while it winds around the origin $n$ times then it's integral is $2pi n$. Also as you said you can't apply green thm, except these you are forced to parametrize the triangle and substitude them in the exact form.
            – user 108128
            yesterday











          • My script says $omega$ is not exact because there's no function f such that $df= omega$ even though $domega = 0$, for $omega$ on $R^2 0$
            – Mohamed Mossad
            yesterday















          up vote
          2
          down vote



          accepted










          We know that
          $$omega=dfrac-y ,dx +x,dyx^2 +y^2=darctandfracyx$$
          is an exact differential and the area $Delta$ includes the origin, since the $arctandfracyx$ winds around the origin one time then
          $$int_Delta omega=2pi$$






          share|cite|improve this answer























          • May I ask how did you come to that answer? like what's intuitive about it? I know that 1-form is quite well-known but I am supposed to calculate the integral not use a trigonometric function which I don't know.
            – Mohamed Mossad
            yesterday










          • When you have an exact differential over a closed area, and while it winds around the origin $n$ times then it's integral is $2pi n$. Also as you said you can't apply green thm, except these you are forced to parametrize the triangle and substitude them in the exact form.
            – user 108128
            yesterday











          • My script says $omega$ is not exact because there's no function f such that $df= omega$ even though $domega = 0$, for $omega$ on $R^2 0$
            – Mohamed Mossad
            yesterday













          up vote
          2
          down vote



          accepted







          up vote
          2
          down vote



          accepted






          We know that
          $$omega=dfrac-y ,dx +x,dyx^2 +y^2=darctandfracyx$$
          is an exact differential and the area $Delta$ includes the origin, since the $arctandfracyx$ winds around the origin one time then
          $$int_Delta omega=2pi$$






          share|cite|improve this answer















          We know that
          $$omega=dfrac-y ,dx +x,dyx^2 +y^2=darctandfracyx$$
          is an exact differential and the area $Delta$ includes the origin, since the $arctandfracyx$ winds around the origin one time then
          $$int_Delta omega=2pi$$







          share|cite|improve this answer















          share|cite|improve this answer



          share|cite|improve this answer








          edited yesterday









          Michael Hardy

          204k23185460




          204k23185460











          answered yesterday









          user 108128

          18.6k41544




          18.6k41544











          • May I ask how did you come to that answer? like what's intuitive about it? I know that 1-form is quite well-known but I am supposed to calculate the integral not use a trigonometric function which I don't know.
            – Mohamed Mossad
            yesterday










          • When you have an exact differential over a closed area, and while it winds around the origin $n$ times then it's integral is $2pi n$. Also as you said you can't apply green thm, except these you are forced to parametrize the triangle and substitude them in the exact form.
            – user 108128
            yesterday











          • My script says $omega$ is not exact because there's no function f such that $df= omega$ even though $domega = 0$, for $omega$ on $R^2 0$
            – Mohamed Mossad
            yesterday

















          • May I ask how did you come to that answer? like what's intuitive about it? I know that 1-form is quite well-known but I am supposed to calculate the integral not use a trigonometric function which I don't know.
            – Mohamed Mossad
            yesterday










          • When you have an exact differential over a closed area, and while it winds around the origin $n$ times then it's integral is $2pi n$. Also as you said you can't apply green thm, except these you are forced to parametrize the triangle and substitude them in the exact form.
            – user 108128
            yesterday











          • My script says $omega$ is not exact because there's no function f such that $df= omega$ even though $domega = 0$, for $omega$ on $R^2 0$
            – Mohamed Mossad
            yesterday
















          May I ask how did you come to that answer? like what's intuitive about it? I know that 1-form is quite well-known but I am supposed to calculate the integral not use a trigonometric function which I don't know.
          – Mohamed Mossad
          yesterday




          May I ask how did you come to that answer? like what's intuitive about it? I know that 1-form is quite well-known but I am supposed to calculate the integral not use a trigonometric function which I don't know.
          – Mohamed Mossad
          yesterday












          When you have an exact differential over a closed area, and while it winds around the origin $n$ times then it's integral is $2pi n$. Also as you said you can't apply green thm, except these you are forced to parametrize the triangle and substitude them in the exact form.
          – user 108128
          yesterday





          When you have an exact differential over a closed area, and while it winds around the origin $n$ times then it's integral is $2pi n$. Also as you said you can't apply green thm, except these you are forced to parametrize the triangle and substitude them in the exact form.
          – user 108128
          yesterday













          My script says $omega$ is not exact because there's no function f such that $df= omega$ even though $domega = 0$, for $omega$ on $R^2 0$
          – Mohamed Mossad
          yesterday





          My script says $omega$ is not exact because there's no function f such that $df= omega$ even though $domega = 0$, for $omega$ on $R^2 0$
          – Mohamed Mossad
          yesterday











          up vote
          1
          down vote













          This is essentially a long comment to the other answer, but worth making an answer of its own, since it highlights a useful trick which also works for Stoke's Theorem, as well as explains the $2 pi n$ answer. It's true that you can't apply Green's theorem to this problem directly, since the function contains a pole at the origin, but this doesn't stop you from applying Green's theorem on other regions that may also be useful.



          Observe that your triangle $T$ does not pass through the origin. This means that you can find a small disk inside the triangle containing the origin $D$. Now consider the region $T - D$. This has two boundary components with opposite orientations, and we can consider the integral over $T - D$.



          This gives us:



          $$int_textinterior of T - D d omega = int_T omega - int_D omega$$ by Green's Theorem (or the Stoke's Theorem for differential forms, if you prefer to call it this). You can check that on this region, the left integral is $0$, as $d omega$ is $0$ everywhere here. This means that you can replace the integral of $T$ with the integral over any nice circle you like encompassing the origin, since the left side is $0$.



          Now recognize that this integral is super friendly to polar coordinates, and convert to these. You will get the correct answer.






          share|cite|improve this answer





















          • I know it's friendly to calculate in polar coordinates because I had an example of it on $c:[0,2pi] rightarrow R^2$ with $t rightarrow (cos t, sin t)$ which is equal $2pi$ when $omega$ isn't defined on 0, but is it the same with the triangle which doesn't pass through the origin?
            – Mohamed Mossad
            yesterday















          up vote
          1
          down vote













          This is essentially a long comment to the other answer, but worth making an answer of its own, since it highlights a useful trick which also works for Stoke's Theorem, as well as explains the $2 pi n$ answer. It's true that you can't apply Green's theorem to this problem directly, since the function contains a pole at the origin, but this doesn't stop you from applying Green's theorem on other regions that may also be useful.



          Observe that your triangle $T$ does not pass through the origin. This means that you can find a small disk inside the triangle containing the origin $D$. Now consider the region $T - D$. This has two boundary components with opposite orientations, and we can consider the integral over $T - D$.



          This gives us:



          $$int_textinterior of T - D d omega = int_T omega - int_D omega$$ by Green's Theorem (or the Stoke's Theorem for differential forms, if you prefer to call it this). You can check that on this region, the left integral is $0$, as $d omega$ is $0$ everywhere here. This means that you can replace the integral of $T$ with the integral over any nice circle you like encompassing the origin, since the left side is $0$.



          Now recognize that this integral is super friendly to polar coordinates, and convert to these. You will get the correct answer.






          share|cite|improve this answer





















          • I know it's friendly to calculate in polar coordinates because I had an example of it on $c:[0,2pi] rightarrow R^2$ with $t rightarrow (cos t, sin t)$ which is equal $2pi$ when $omega$ isn't defined on 0, but is it the same with the triangle which doesn't pass through the origin?
            – Mohamed Mossad
            yesterday













          up vote
          1
          down vote










          up vote
          1
          down vote









          This is essentially a long comment to the other answer, but worth making an answer of its own, since it highlights a useful trick which also works for Stoke's Theorem, as well as explains the $2 pi n$ answer. It's true that you can't apply Green's theorem to this problem directly, since the function contains a pole at the origin, but this doesn't stop you from applying Green's theorem on other regions that may also be useful.



          Observe that your triangle $T$ does not pass through the origin. This means that you can find a small disk inside the triangle containing the origin $D$. Now consider the region $T - D$. This has two boundary components with opposite orientations, and we can consider the integral over $T - D$.



          This gives us:



          $$int_textinterior of T - D d omega = int_T omega - int_D omega$$ by Green's Theorem (or the Stoke's Theorem for differential forms, if you prefer to call it this). You can check that on this region, the left integral is $0$, as $d omega$ is $0$ everywhere here. This means that you can replace the integral of $T$ with the integral over any nice circle you like encompassing the origin, since the left side is $0$.



          Now recognize that this integral is super friendly to polar coordinates, and convert to these. You will get the correct answer.






          share|cite|improve this answer













          This is essentially a long comment to the other answer, but worth making an answer of its own, since it highlights a useful trick which also works for Stoke's Theorem, as well as explains the $2 pi n$ answer. It's true that you can't apply Green's theorem to this problem directly, since the function contains a pole at the origin, but this doesn't stop you from applying Green's theorem on other regions that may also be useful.



          Observe that your triangle $T$ does not pass through the origin. This means that you can find a small disk inside the triangle containing the origin $D$. Now consider the region $T - D$. This has two boundary components with opposite orientations, and we can consider the integral over $T - D$.



          This gives us:



          $$int_textinterior of T - D d omega = int_T omega - int_D omega$$ by Green's Theorem (or the Stoke's Theorem for differential forms, if you prefer to call it this). You can check that on this region, the left integral is $0$, as $d omega$ is $0$ everywhere here. This means that you can replace the integral of $T$ with the integral over any nice circle you like encompassing the origin, since the left side is $0$.



          Now recognize that this integral is super friendly to polar coordinates, and convert to these. You will get the correct answer.







          share|cite|improve this answer













          share|cite|improve this answer



          share|cite|improve this answer











          answered yesterday









          Alfred Yerger

          9,2761743




          9,2761743











          • I know it's friendly to calculate in polar coordinates because I had an example of it on $c:[0,2pi] rightarrow R^2$ with $t rightarrow (cos t, sin t)$ which is equal $2pi$ when $omega$ isn't defined on 0, but is it the same with the triangle which doesn't pass through the origin?
            – Mohamed Mossad
            yesterday

















          • I know it's friendly to calculate in polar coordinates because I had an example of it on $c:[0,2pi] rightarrow R^2$ with $t rightarrow (cos t, sin t)$ which is equal $2pi$ when $omega$ isn't defined on 0, but is it the same with the triangle which doesn't pass through the origin?
            – Mohamed Mossad
            yesterday
















          I know it's friendly to calculate in polar coordinates because I had an example of it on $c:[0,2pi] rightarrow R^2$ with $t rightarrow (cos t, sin t)$ which is equal $2pi$ when $omega$ isn't defined on 0, but is it the same with the triangle which doesn't pass through the origin?
          – Mohamed Mossad
          yesterday





          I know it's friendly to calculate in polar coordinates because I had an example of it on $c:[0,2pi] rightarrow R^2$ with $t rightarrow (cos t, sin t)$ which is equal $2pi$ when $omega$ isn't defined on 0, but is it the same with the triangle which doesn't pass through the origin?
          – Mohamed Mossad
          yesterday













           

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