Parametric integration negative area?












1












$begingroup$


I know there is a question very similar to mine already here Why does using an integral to calculate an area sometimes return a negative value when using a parametric equation?
, but I am still a bit unsure after reading the answers as to when the integral gives you a positive area and when it gives you a negative area. My text book says that the area is positive if t traces out the curve clockwise and negative for anticlockwise, however I think there is more going on with regards to whether the curve is above or below the x axis.



Since $A=int_a^b yfrac{dx}{dt}dt$, my guess is that you get a positive answer if either the graph is above the x axis (y is positive) and the point is moving to the right (dx/dt positive) or the graph is below the x axis and the point is moving to the left. Then you get a negative answer if either the graph is below the x axis but is being traced out moving to the right, or the graph is above the x axis but is being traced out moving to the left.



Was my book wrong? Is my thinking correct?



Thank you in advance :)










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$endgroup$

















    1












    $begingroup$


    I know there is a question very similar to mine already here Why does using an integral to calculate an area sometimes return a negative value when using a parametric equation?
    , but I am still a bit unsure after reading the answers as to when the integral gives you a positive area and when it gives you a negative area. My text book says that the area is positive if t traces out the curve clockwise and negative for anticlockwise, however I think there is more going on with regards to whether the curve is above or below the x axis.



    Since $A=int_a^b yfrac{dx}{dt}dt$, my guess is that you get a positive answer if either the graph is above the x axis (y is positive) and the point is moving to the right (dx/dt positive) or the graph is below the x axis and the point is moving to the left. Then you get a negative answer if either the graph is below the x axis but is being traced out moving to the right, or the graph is above the x axis but is being traced out moving to the left.



    Was my book wrong? Is my thinking correct?



    Thank you in advance :)










    share|cite|improve this question











    $endgroup$















      1












      1








      1





      $begingroup$


      I know there is a question very similar to mine already here Why does using an integral to calculate an area sometimes return a negative value when using a parametric equation?
      , but I am still a bit unsure after reading the answers as to when the integral gives you a positive area and when it gives you a negative area. My text book says that the area is positive if t traces out the curve clockwise and negative for anticlockwise, however I think there is more going on with regards to whether the curve is above or below the x axis.



      Since $A=int_a^b yfrac{dx}{dt}dt$, my guess is that you get a positive answer if either the graph is above the x axis (y is positive) and the point is moving to the right (dx/dt positive) or the graph is below the x axis and the point is moving to the left. Then you get a negative answer if either the graph is below the x axis but is being traced out moving to the right, or the graph is above the x axis but is being traced out moving to the left.



      Was my book wrong? Is my thinking correct?



      Thank you in advance :)










      share|cite|improve this question











      $endgroup$




      I know there is a question very similar to mine already here Why does using an integral to calculate an area sometimes return a negative value when using a parametric equation?
      , but I am still a bit unsure after reading the answers as to when the integral gives you a positive area and when it gives you a negative area. My text book says that the area is positive if t traces out the curve clockwise and negative for anticlockwise, however I think there is more going on with regards to whether the curve is above or below the x axis.



      Since $A=int_a^b yfrac{dx}{dt}dt$, my guess is that you get a positive answer if either the graph is above the x axis (y is positive) and the point is moving to the right (dx/dt positive) or the graph is below the x axis and the point is moving to the left. Then you get a negative answer if either the graph is below the x axis but is being traced out moving to the right, or the graph is above the x axis but is being traced out moving to the left.



      Was my book wrong? Is my thinking correct?



      Thank you in advance :)







      integration definite-integrals coordinate-systems parametric area






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      edited Apr 13 '17 at 12:20









      Community

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      asked Feb 19 '15 at 13:00









      21joanna1221joanna12

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          $begingroup$

          Your thinking is correct, and your book is not wrong.



          You say that that the integral $int_a^b y frac{dx}{dt},dt$ is positive when either $y>0$ and $frac{dx}{dt}>0$ (above the $x$-axis, moving left-to-right), or $y < 0$ and $frac{dx}{dt} < 0$ (below the $x$-axis, moving right-to-left).

          In both of these cases, the particle moves clockwise with respect to the origin.






          share|cite|improve this answer









          $endgroup$





















            0












            $begingroup$

            Your thinking is correct, but the book is wrong in general.



            Assuming that $tin [a,b]$ with $a<b$, then considering $displaystyle int_a^b y frac{dx}{dt}dt$, we can split into two cases:



            (i) The integrand $y dfrac{dx}{dt} > 0$, which can happen (a) if $y$ and $dfrac{dx}{dt}$ are both positive, or (b) both are negative.



            (ii) The integrand $y dfrac{dx}{dt} < 0$, which can happen if either $y > 0$ and $dfrac{dx}{dt} < 0$, vice-versa.



            Both cases above correlate with your interpretation, which is correct.



            Of course, the integrand can change sign within $[a,b]$, in which case the negative and positive areas will cancel each other out. Let's forget about that for now.



            It is not true to say that $y dfrac{dx}{dt} > 0$ corresponds to clockwise motion about the origin. This is a really important point.



            Consider the parametric curve $x=t, y=t^2$ for $tin [0,1]$. This is just the parabola $y=x^2$. Intuitively, one can see that in moving from $(0,0)$ ($t=0$) to $(1,1)$ ($t=1$) the curve moves anti-clockwise relative to the origin. Yet, computing the integral $displaystyle int_a^b y frac{dx}{dt}dt = dfrac{1}{3}$, which is positive.



            More rigorously, we can convert the problem above to polar coordinates using the transformations $x=rcostheta, y=rsintheta$. We find that $rgeq0$ and $0leq theta < dfrac{pi}{2}$. It's quite easy to show that $dfrac{dtheta}{dr} > 0$, thus the 'motion' is counter-clockwise throughout.



            Compare this to $x=costheta, y=sintheta$ for $thetainleft[0,dfrac{pi}{2}right]$. The 'motion' is also counter-clockwise. However, if you compute the integral, you'll get the negative result $-dfrac{pi}{4}$.



            The conclusion? Forget clockwise vs anticlockwise motion. What's important is the sign of $y dfrac{dx}{dt}$, nothing more.






            share|cite|improve this answer











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              2 Answers
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              2 Answers
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              0












              $begingroup$

              Your thinking is correct, and your book is not wrong.



              You say that that the integral $int_a^b y frac{dx}{dt},dt$ is positive when either $y>0$ and $frac{dx}{dt}>0$ (above the $x$-axis, moving left-to-right), or $y < 0$ and $frac{dx}{dt} < 0$ (below the $x$-axis, moving right-to-left).

              In both of these cases, the particle moves clockwise with respect to the origin.






              share|cite|improve this answer









              $endgroup$


















                0












                $begingroup$

                Your thinking is correct, and your book is not wrong.



                You say that that the integral $int_a^b y frac{dx}{dt},dt$ is positive when either $y>0$ and $frac{dx}{dt}>0$ (above the $x$-axis, moving left-to-right), or $y < 0$ and $frac{dx}{dt} < 0$ (below the $x$-axis, moving right-to-left).

                In both of these cases, the particle moves clockwise with respect to the origin.






                share|cite|improve this answer









                $endgroup$
















                  0












                  0








                  0





                  $begingroup$

                  Your thinking is correct, and your book is not wrong.



                  You say that that the integral $int_a^b y frac{dx}{dt},dt$ is positive when either $y>0$ and $frac{dx}{dt}>0$ (above the $x$-axis, moving left-to-right), or $y < 0$ and $frac{dx}{dt} < 0$ (below the $x$-axis, moving right-to-left).

                  In both of these cases, the particle moves clockwise with respect to the origin.






                  share|cite|improve this answer









                  $endgroup$



                  Your thinking is correct, and your book is not wrong.



                  You say that that the integral $int_a^b y frac{dx}{dt},dt$ is positive when either $y>0$ and $frac{dx}{dt}>0$ (above the $x$-axis, moving left-to-right), or $y < 0$ and $frac{dx}{dt} < 0$ (below the $x$-axis, moving right-to-left).

                  In both of these cases, the particle moves clockwise with respect to the origin.







                  share|cite|improve this answer












                  share|cite|improve this answer



                  share|cite|improve this answer










                  answered May 9 '16 at 13:31









                  Matthew LeingangMatthew Leingang

                  16.4k12244




                  16.4k12244























                      0












                      $begingroup$

                      Your thinking is correct, but the book is wrong in general.



                      Assuming that $tin [a,b]$ with $a<b$, then considering $displaystyle int_a^b y frac{dx}{dt}dt$, we can split into two cases:



                      (i) The integrand $y dfrac{dx}{dt} > 0$, which can happen (a) if $y$ and $dfrac{dx}{dt}$ are both positive, or (b) both are negative.



                      (ii) The integrand $y dfrac{dx}{dt} < 0$, which can happen if either $y > 0$ and $dfrac{dx}{dt} < 0$, vice-versa.



                      Both cases above correlate with your interpretation, which is correct.



                      Of course, the integrand can change sign within $[a,b]$, in which case the negative and positive areas will cancel each other out. Let's forget about that for now.



                      It is not true to say that $y dfrac{dx}{dt} > 0$ corresponds to clockwise motion about the origin. This is a really important point.



                      Consider the parametric curve $x=t, y=t^2$ for $tin [0,1]$. This is just the parabola $y=x^2$. Intuitively, one can see that in moving from $(0,0)$ ($t=0$) to $(1,1)$ ($t=1$) the curve moves anti-clockwise relative to the origin. Yet, computing the integral $displaystyle int_a^b y frac{dx}{dt}dt = dfrac{1}{3}$, which is positive.



                      More rigorously, we can convert the problem above to polar coordinates using the transformations $x=rcostheta, y=rsintheta$. We find that $rgeq0$ and $0leq theta < dfrac{pi}{2}$. It's quite easy to show that $dfrac{dtheta}{dr} > 0$, thus the 'motion' is counter-clockwise throughout.



                      Compare this to $x=costheta, y=sintheta$ for $thetainleft[0,dfrac{pi}{2}right]$. The 'motion' is also counter-clockwise. However, if you compute the integral, you'll get the negative result $-dfrac{pi}{4}$.



                      The conclusion? Forget clockwise vs anticlockwise motion. What's important is the sign of $y dfrac{dx}{dt}$, nothing more.






                      share|cite|improve this answer











                      $endgroup$


















                        0












                        $begingroup$

                        Your thinking is correct, but the book is wrong in general.



                        Assuming that $tin [a,b]$ with $a<b$, then considering $displaystyle int_a^b y frac{dx}{dt}dt$, we can split into two cases:



                        (i) The integrand $y dfrac{dx}{dt} > 0$, which can happen (a) if $y$ and $dfrac{dx}{dt}$ are both positive, or (b) both are negative.



                        (ii) The integrand $y dfrac{dx}{dt} < 0$, which can happen if either $y > 0$ and $dfrac{dx}{dt} < 0$, vice-versa.



                        Both cases above correlate with your interpretation, which is correct.



                        Of course, the integrand can change sign within $[a,b]$, in which case the negative and positive areas will cancel each other out. Let's forget about that for now.



                        It is not true to say that $y dfrac{dx}{dt} > 0$ corresponds to clockwise motion about the origin. This is a really important point.



                        Consider the parametric curve $x=t, y=t^2$ for $tin [0,1]$. This is just the parabola $y=x^2$. Intuitively, one can see that in moving from $(0,0)$ ($t=0$) to $(1,1)$ ($t=1$) the curve moves anti-clockwise relative to the origin. Yet, computing the integral $displaystyle int_a^b y frac{dx}{dt}dt = dfrac{1}{3}$, which is positive.



                        More rigorously, we can convert the problem above to polar coordinates using the transformations $x=rcostheta, y=rsintheta$. We find that $rgeq0$ and $0leq theta < dfrac{pi}{2}$. It's quite easy to show that $dfrac{dtheta}{dr} > 0$, thus the 'motion' is counter-clockwise throughout.



                        Compare this to $x=costheta, y=sintheta$ for $thetainleft[0,dfrac{pi}{2}right]$. The 'motion' is also counter-clockwise. However, if you compute the integral, you'll get the negative result $-dfrac{pi}{4}$.



                        The conclusion? Forget clockwise vs anticlockwise motion. What's important is the sign of $y dfrac{dx}{dt}$, nothing more.






                        share|cite|improve this answer











                        $endgroup$
















                          0












                          0








                          0





                          $begingroup$

                          Your thinking is correct, but the book is wrong in general.



                          Assuming that $tin [a,b]$ with $a<b$, then considering $displaystyle int_a^b y frac{dx}{dt}dt$, we can split into two cases:



                          (i) The integrand $y dfrac{dx}{dt} > 0$, which can happen (a) if $y$ and $dfrac{dx}{dt}$ are both positive, or (b) both are negative.



                          (ii) The integrand $y dfrac{dx}{dt} < 0$, which can happen if either $y > 0$ and $dfrac{dx}{dt} < 0$, vice-versa.



                          Both cases above correlate with your interpretation, which is correct.



                          Of course, the integrand can change sign within $[a,b]$, in which case the negative and positive areas will cancel each other out. Let's forget about that for now.



                          It is not true to say that $y dfrac{dx}{dt} > 0$ corresponds to clockwise motion about the origin. This is a really important point.



                          Consider the parametric curve $x=t, y=t^2$ for $tin [0,1]$. This is just the parabola $y=x^2$. Intuitively, one can see that in moving from $(0,0)$ ($t=0$) to $(1,1)$ ($t=1$) the curve moves anti-clockwise relative to the origin. Yet, computing the integral $displaystyle int_a^b y frac{dx}{dt}dt = dfrac{1}{3}$, which is positive.



                          More rigorously, we can convert the problem above to polar coordinates using the transformations $x=rcostheta, y=rsintheta$. We find that $rgeq0$ and $0leq theta < dfrac{pi}{2}$. It's quite easy to show that $dfrac{dtheta}{dr} > 0$, thus the 'motion' is counter-clockwise throughout.



                          Compare this to $x=costheta, y=sintheta$ for $thetainleft[0,dfrac{pi}{2}right]$. The 'motion' is also counter-clockwise. However, if you compute the integral, you'll get the negative result $-dfrac{pi}{4}$.



                          The conclusion? Forget clockwise vs anticlockwise motion. What's important is the sign of $y dfrac{dx}{dt}$, nothing more.






                          share|cite|improve this answer











                          $endgroup$



                          Your thinking is correct, but the book is wrong in general.



                          Assuming that $tin [a,b]$ with $a<b$, then considering $displaystyle int_a^b y frac{dx}{dt}dt$, we can split into two cases:



                          (i) The integrand $y dfrac{dx}{dt} > 0$, which can happen (a) if $y$ and $dfrac{dx}{dt}$ are both positive, or (b) both are negative.



                          (ii) The integrand $y dfrac{dx}{dt} < 0$, which can happen if either $y > 0$ and $dfrac{dx}{dt} < 0$, vice-versa.



                          Both cases above correlate with your interpretation, which is correct.



                          Of course, the integrand can change sign within $[a,b]$, in which case the negative and positive areas will cancel each other out. Let's forget about that for now.



                          It is not true to say that $y dfrac{dx}{dt} > 0$ corresponds to clockwise motion about the origin. This is a really important point.



                          Consider the parametric curve $x=t, y=t^2$ for $tin [0,1]$. This is just the parabola $y=x^2$. Intuitively, one can see that in moving from $(0,0)$ ($t=0$) to $(1,1)$ ($t=1$) the curve moves anti-clockwise relative to the origin. Yet, computing the integral $displaystyle int_a^b y frac{dx}{dt}dt = dfrac{1}{3}$, which is positive.



                          More rigorously, we can convert the problem above to polar coordinates using the transformations $x=rcostheta, y=rsintheta$. We find that $rgeq0$ and $0leq theta < dfrac{pi}{2}$. It's quite easy to show that $dfrac{dtheta}{dr} > 0$, thus the 'motion' is counter-clockwise throughout.



                          Compare this to $x=costheta, y=sintheta$ for $thetainleft[0,dfrac{pi}{2}right]$. The 'motion' is also counter-clockwise. However, if you compute the integral, you'll get the negative result $-dfrac{pi}{4}$.



                          The conclusion? Forget clockwise vs anticlockwise motion. What's important is the sign of $y dfrac{dx}{dt}$, nothing more.







                          share|cite|improve this answer














                          share|cite|improve this answer



                          share|cite|improve this answer








                          edited Jan 18 at 22:40

























                          answered Jan 18 at 22:31









                          CatManDooCatManDoo

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