velocity and acceleration in a parabola












2












$begingroup$


A particle moves with constant speed along a parabola of equation $y^{2}=2px$ with $p=constant$. I want to find its velocity and acceleration vector.



Since the velocity magnitude is constant I know the acceleration will be along the normal of the parabola and of the form



$$vec{a}=frac{v^{2}}{R(t)}vec{n}, v=constant$$



where $R(t)$ is the time dependent radius of curvature of the parabola and $vec{n}$ is the normal.



To find the velocity I parametrize the parabola with $(y^{2}(t)/(2p),y(t))$. The velocity is the tangent vector given by deriving this parametric position



Then $vec{v}=left(frac{y}{p}frac{dy}{dt},frac{dy}{dt}right)$ and the constraint of constant speed leads to



$$|vec{v}|=constant=frac{dy}{dt}sqrt{left(frac{y}{p}right)^{2}+1}$$



This seems to be a first order differential equation. Is it solvable?
How do I find $vec{n}$ and $R(t)$?










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    2












    $begingroup$


    A particle moves with constant speed along a parabola of equation $y^{2}=2px$ with $p=constant$. I want to find its velocity and acceleration vector.



    Since the velocity magnitude is constant I know the acceleration will be along the normal of the parabola and of the form



    $$vec{a}=frac{v^{2}}{R(t)}vec{n}, v=constant$$



    where $R(t)$ is the time dependent radius of curvature of the parabola and $vec{n}$ is the normal.



    To find the velocity I parametrize the parabola with $(y^{2}(t)/(2p),y(t))$. The velocity is the tangent vector given by deriving this parametric position



    Then $vec{v}=left(frac{y}{p}frac{dy}{dt},frac{dy}{dt}right)$ and the constraint of constant speed leads to



    $$|vec{v}|=constant=frac{dy}{dt}sqrt{left(frac{y}{p}right)^{2}+1}$$



    This seems to be a first order differential equation. Is it solvable?
    How do I find $vec{n}$ and $R(t)$?










    share|cite|improve this question









    $endgroup$















      2












      2








      2





      $begingroup$


      A particle moves with constant speed along a parabola of equation $y^{2}=2px$ with $p=constant$. I want to find its velocity and acceleration vector.



      Since the velocity magnitude is constant I know the acceleration will be along the normal of the parabola and of the form



      $$vec{a}=frac{v^{2}}{R(t)}vec{n}, v=constant$$



      where $R(t)$ is the time dependent radius of curvature of the parabola and $vec{n}$ is the normal.



      To find the velocity I parametrize the parabola with $(y^{2}(t)/(2p),y(t))$. The velocity is the tangent vector given by deriving this parametric position



      Then $vec{v}=left(frac{y}{p}frac{dy}{dt},frac{dy}{dt}right)$ and the constraint of constant speed leads to



      $$|vec{v}|=constant=frac{dy}{dt}sqrt{left(frac{y}{p}right)^{2}+1}$$



      This seems to be a first order differential equation. Is it solvable?
      How do I find $vec{n}$ and $R(t)$?










      share|cite|improve this question









      $endgroup$




      A particle moves with constant speed along a parabola of equation $y^{2}=2px$ with $p=constant$. I want to find its velocity and acceleration vector.



      Since the velocity magnitude is constant I know the acceleration will be along the normal of the parabola and of the form



      $$vec{a}=frac{v^{2}}{R(t)}vec{n}, v=constant$$



      where $R(t)$ is the time dependent radius of curvature of the parabola and $vec{n}$ is the normal.



      To find the velocity I parametrize the parabola with $(y^{2}(t)/(2p),y(t))$. The velocity is the tangent vector given by deriving this parametric position



      Then $vec{v}=left(frac{y}{p}frac{dy}{dt},frac{dy}{dt}right)$ and the constraint of constant speed leads to



      $$|vec{v}|=constant=frac{dy}{dt}sqrt{left(frac{y}{p}right)^{2}+1}$$



      This seems to be a first order differential equation. Is it solvable?
      How do I find $vec{n}$ and $R(t)$?







      polar-coordinates tangent-line kinematics






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      share|cite|improve this question











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      asked Dec 5 '18 at 14:08









      JennyToyJennyToy

      25018




      25018






















          1 Answer
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          1












          $begingroup$

          The diferential equation is solvable, the integral $intsqrt{1+x^2}dx$ can be found in the tables (or found via integration by parts).



          What you actually found is the mapping between $y$ and $t$. For the radius of curvature, it's much easier to just get it geometrically, with respect to position (parameterized with $y$). The standard differential geometry of curves gives you:



          $$frac{1}{R(x(y))}=frac{x''(y)}{sqrt{1+x'(y)^2}^3}$$



          where $x=frac{y^2}{2p}$.



          So, the acceleration, expressed with $y$, is straight forward and does not require integration. However, converting $a(y)$ into $a(t)$ requires the function $y(t)$ which will be problematic, because the solution of your differential equation gives you $t(y)$ that is transcendental and thus not invertible in closed form.






          share|cite|improve this answer









          $endgroup$













          • $begingroup$
            The normal $vec{n}$ can be obtained by picking any vector of unit length whose dot product with $vec{v}$ is zero?
            $endgroup$
            – JennyToy
            Dec 5 '18 at 15:02










          • $begingroup$
            There are only two options - one points in, one points out. One is wrong.
            $endgroup$
            – orion
            Dec 5 '18 at 15:04











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          1 Answer
          1






          active

          oldest

          votes








          1 Answer
          1






          active

          oldest

          votes









          active

          oldest

          votes






          active

          oldest

          votes









          1












          $begingroup$

          The diferential equation is solvable, the integral $intsqrt{1+x^2}dx$ can be found in the tables (or found via integration by parts).



          What you actually found is the mapping between $y$ and $t$. For the radius of curvature, it's much easier to just get it geometrically, with respect to position (parameterized with $y$). The standard differential geometry of curves gives you:



          $$frac{1}{R(x(y))}=frac{x''(y)}{sqrt{1+x'(y)^2}^3}$$



          where $x=frac{y^2}{2p}$.



          So, the acceleration, expressed with $y$, is straight forward and does not require integration. However, converting $a(y)$ into $a(t)$ requires the function $y(t)$ which will be problematic, because the solution of your differential equation gives you $t(y)$ that is transcendental and thus not invertible in closed form.






          share|cite|improve this answer









          $endgroup$













          • $begingroup$
            The normal $vec{n}$ can be obtained by picking any vector of unit length whose dot product with $vec{v}$ is zero?
            $endgroup$
            – JennyToy
            Dec 5 '18 at 15:02










          • $begingroup$
            There are only two options - one points in, one points out. One is wrong.
            $endgroup$
            – orion
            Dec 5 '18 at 15:04
















          1












          $begingroup$

          The diferential equation is solvable, the integral $intsqrt{1+x^2}dx$ can be found in the tables (or found via integration by parts).



          What you actually found is the mapping between $y$ and $t$. For the radius of curvature, it's much easier to just get it geometrically, with respect to position (parameterized with $y$). The standard differential geometry of curves gives you:



          $$frac{1}{R(x(y))}=frac{x''(y)}{sqrt{1+x'(y)^2}^3}$$



          where $x=frac{y^2}{2p}$.



          So, the acceleration, expressed with $y$, is straight forward and does not require integration. However, converting $a(y)$ into $a(t)$ requires the function $y(t)$ which will be problematic, because the solution of your differential equation gives you $t(y)$ that is transcendental and thus not invertible in closed form.






          share|cite|improve this answer









          $endgroup$













          • $begingroup$
            The normal $vec{n}$ can be obtained by picking any vector of unit length whose dot product with $vec{v}$ is zero?
            $endgroup$
            – JennyToy
            Dec 5 '18 at 15:02










          • $begingroup$
            There are only two options - one points in, one points out. One is wrong.
            $endgroup$
            – orion
            Dec 5 '18 at 15:04














          1












          1








          1





          $begingroup$

          The diferential equation is solvable, the integral $intsqrt{1+x^2}dx$ can be found in the tables (or found via integration by parts).



          What you actually found is the mapping between $y$ and $t$. For the radius of curvature, it's much easier to just get it geometrically, with respect to position (parameterized with $y$). The standard differential geometry of curves gives you:



          $$frac{1}{R(x(y))}=frac{x''(y)}{sqrt{1+x'(y)^2}^3}$$



          where $x=frac{y^2}{2p}$.



          So, the acceleration, expressed with $y$, is straight forward and does not require integration. However, converting $a(y)$ into $a(t)$ requires the function $y(t)$ which will be problematic, because the solution of your differential equation gives you $t(y)$ that is transcendental and thus not invertible in closed form.






          share|cite|improve this answer









          $endgroup$



          The diferential equation is solvable, the integral $intsqrt{1+x^2}dx$ can be found in the tables (or found via integration by parts).



          What you actually found is the mapping between $y$ and $t$. For the radius of curvature, it's much easier to just get it geometrically, with respect to position (parameterized with $y$). The standard differential geometry of curves gives you:



          $$frac{1}{R(x(y))}=frac{x''(y)}{sqrt{1+x'(y)^2}^3}$$



          where $x=frac{y^2}{2p}$.



          So, the acceleration, expressed with $y$, is straight forward and does not require integration. However, converting $a(y)$ into $a(t)$ requires the function $y(t)$ which will be problematic, because the solution of your differential equation gives you $t(y)$ that is transcendental and thus not invertible in closed form.







          share|cite|improve this answer












          share|cite|improve this answer



          share|cite|improve this answer










          answered Dec 5 '18 at 14:22









          orionorion

          13.3k11836




          13.3k11836












          • $begingroup$
            The normal $vec{n}$ can be obtained by picking any vector of unit length whose dot product with $vec{v}$ is zero?
            $endgroup$
            – JennyToy
            Dec 5 '18 at 15:02










          • $begingroup$
            There are only two options - one points in, one points out. One is wrong.
            $endgroup$
            – orion
            Dec 5 '18 at 15:04


















          • $begingroup$
            The normal $vec{n}$ can be obtained by picking any vector of unit length whose dot product with $vec{v}$ is zero?
            $endgroup$
            – JennyToy
            Dec 5 '18 at 15:02










          • $begingroup$
            There are only two options - one points in, one points out. One is wrong.
            $endgroup$
            – orion
            Dec 5 '18 at 15:04
















          $begingroup$
          The normal $vec{n}$ can be obtained by picking any vector of unit length whose dot product with $vec{v}$ is zero?
          $endgroup$
          – JennyToy
          Dec 5 '18 at 15:02




          $begingroup$
          The normal $vec{n}$ can be obtained by picking any vector of unit length whose dot product with $vec{v}$ is zero?
          $endgroup$
          – JennyToy
          Dec 5 '18 at 15:02












          $begingroup$
          There are only two options - one points in, one points out. One is wrong.
          $endgroup$
          – orion
          Dec 5 '18 at 15:04




          $begingroup$
          There are only two options - one points in, one points out. One is wrong.
          $endgroup$
          – orion
          Dec 5 '18 at 15:04


















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