Prove for the time derivative of a vector with constant magnitude

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First of all, sorry for my bad English, I have several doubts about the geometric demonstration made by Kleppner for the derivative of a vector that has a constant magnitude, page 25, which is attached in this photo:



photo.



Is this proof rigorously validated? I understand that $sin (x) approx x$ for small $x$, by dividing both sides by $Delta t$, and take the limit for the equality. I understand that equality is correct, but is the argument correct? In the book, i understand the intuitive part, but for example what would have happened if I had taken an approximation of higher order, this would not have had any contribution in the limit? How are these terms depreciated rigorously, since I think that depends on how the time angle $θ (t)$ depends, for example, you can say that the vector varies with $Δθ (t)$, very slow or very fast so that the terms of higher order have a contribution in the limit, and therefore the equality raised is not correct, I apologize in case the question is a triviality.







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  • 3




    Your question is perfectly valid. Merely using differentials is a bit hand-wavy here, but the idea is that $Delta theta$ is the difference between the vectors $A(t+Delta t)$ and $A(t)$, and as $Delta t to 0$, $Delta theta to 0$. The rate at which $Delta theta to 0$ is linearly related to the rate at which $Delta t to 0$ by some basic geometry about circles
    – Brevan Ellefsen
    Jul 17 at 8:31










  • Welcome to MSE. It is in your best interest that you type your questions (using MathJax) instead of posting links to pictures.
    – José Carlos Santos
    Jul 17 at 8:38






  • 1




    Kleppner's book is a really good introductory mechanics book. Thanks for reminding me of this book.
    – Sou
    Jul 17 at 18:57















up vote
3
down vote

favorite












First of all, sorry for my bad English, I have several doubts about the geometric demonstration made by Kleppner for the derivative of a vector that has a constant magnitude, page 25, which is attached in this photo:



photo.



Is this proof rigorously validated? I understand that $sin (x) approx x$ for small $x$, by dividing both sides by $Delta t$, and take the limit for the equality. I understand that equality is correct, but is the argument correct? In the book, i understand the intuitive part, but for example what would have happened if I had taken an approximation of higher order, this would not have had any contribution in the limit? How are these terms depreciated rigorously, since I think that depends on how the time angle $θ (t)$ depends, for example, you can say that the vector varies with $Δθ (t)$, very slow or very fast so that the terms of higher order have a contribution in the limit, and therefore the equality raised is not correct, I apologize in case the question is a triviality.







share|cite|improve this question

















  • 3




    Your question is perfectly valid. Merely using differentials is a bit hand-wavy here, but the idea is that $Delta theta$ is the difference between the vectors $A(t+Delta t)$ and $A(t)$, and as $Delta t to 0$, $Delta theta to 0$. The rate at which $Delta theta to 0$ is linearly related to the rate at which $Delta t to 0$ by some basic geometry about circles
    – Brevan Ellefsen
    Jul 17 at 8:31










  • Welcome to MSE. It is in your best interest that you type your questions (using MathJax) instead of posting links to pictures.
    – José Carlos Santos
    Jul 17 at 8:38






  • 1




    Kleppner's book is a really good introductory mechanics book. Thanks for reminding me of this book.
    – Sou
    Jul 17 at 18:57













up vote
3
down vote

favorite









up vote
3
down vote

favorite











First of all, sorry for my bad English, I have several doubts about the geometric demonstration made by Kleppner for the derivative of a vector that has a constant magnitude, page 25, which is attached in this photo:



photo.



Is this proof rigorously validated? I understand that $sin (x) approx x$ for small $x$, by dividing both sides by $Delta t$, and take the limit for the equality. I understand that equality is correct, but is the argument correct? In the book, i understand the intuitive part, but for example what would have happened if I had taken an approximation of higher order, this would not have had any contribution in the limit? How are these terms depreciated rigorously, since I think that depends on how the time angle $θ (t)$ depends, for example, you can say that the vector varies with $Δθ (t)$, very slow or very fast so that the terms of higher order have a contribution in the limit, and therefore the equality raised is not correct, I apologize in case the question is a triviality.







share|cite|improve this question













First of all, sorry for my bad English, I have several doubts about the geometric demonstration made by Kleppner for the derivative of a vector that has a constant magnitude, page 25, which is attached in this photo:



photo.



Is this proof rigorously validated? I understand that $sin (x) approx x$ for small $x$, by dividing both sides by $Delta t$, and take the limit for the equality. I understand that equality is correct, but is the argument correct? In the book, i understand the intuitive part, but for example what would have happened if I had taken an approximation of higher order, this would not have had any contribution in the limit? How are these terms depreciated rigorously, since I think that depends on how the time angle $θ (t)$ depends, for example, you can say that the vector varies with $Δθ (t)$, very slow or very fast so that the terms of higher order have a contribution in the limit, and therefore the equality raised is not correct, I apologize in case the question is a triviality.









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edited Jul 17 at 9:08
























asked Jul 17 at 8:18









Jalil Varela Manjarres

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  • 3




    Your question is perfectly valid. Merely using differentials is a bit hand-wavy here, but the idea is that $Delta theta$ is the difference between the vectors $A(t+Delta t)$ and $A(t)$, and as $Delta t to 0$, $Delta theta to 0$. The rate at which $Delta theta to 0$ is linearly related to the rate at which $Delta t to 0$ by some basic geometry about circles
    – Brevan Ellefsen
    Jul 17 at 8:31










  • Welcome to MSE. It is in your best interest that you type your questions (using MathJax) instead of posting links to pictures.
    – José Carlos Santos
    Jul 17 at 8:38






  • 1




    Kleppner's book is a really good introductory mechanics book. Thanks for reminding me of this book.
    – Sou
    Jul 17 at 18:57













  • 3




    Your question is perfectly valid. Merely using differentials is a bit hand-wavy here, but the idea is that $Delta theta$ is the difference between the vectors $A(t+Delta t)$ and $A(t)$, and as $Delta t to 0$, $Delta theta to 0$. The rate at which $Delta theta to 0$ is linearly related to the rate at which $Delta t to 0$ by some basic geometry about circles
    – Brevan Ellefsen
    Jul 17 at 8:31










  • Welcome to MSE. It is in your best interest that you type your questions (using MathJax) instead of posting links to pictures.
    – José Carlos Santos
    Jul 17 at 8:38






  • 1




    Kleppner's book is a really good introductory mechanics book. Thanks for reminding me of this book.
    – Sou
    Jul 17 at 18:57








3




3




Your question is perfectly valid. Merely using differentials is a bit hand-wavy here, but the idea is that $Delta theta$ is the difference between the vectors $A(t+Delta t)$ and $A(t)$, and as $Delta t to 0$, $Delta theta to 0$. The rate at which $Delta theta to 0$ is linearly related to the rate at which $Delta t to 0$ by some basic geometry about circles
– Brevan Ellefsen
Jul 17 at 8:31




Your question is perfectly valid. Merely using differentials is a bit hand-wavy here, but the idea is that $Delta theta$ is the difference between the vectors $A(t+Delta t)$ and $A(t)$, and as $Delta t to 0$, $Delta theta to 0$. The rate at which $Delta theta to 0$ is linearly related to the rate at which $Delta t to 0$ by some basic geometry about circles
– Brevan Ellefsen
Jul 17 at 8:31












Welcome to MSE. It is in your best interest that you type your questions (using MathJax) instead of posting links to pictures.
– José Carlos Santos
Jul 17 at 8:38




Welcome to MSE. It is in your best interest that you type your questions (using MathJax) instead of posting links to pictures.
– José Carlos Santos
Jul 17 at 8:38




1




1




Kleppner's book is a really good introductory mechanics book. Thanks for reminding me of this book.
– Sou
Jul 17 at 18:57





Kleppner's book is a really good introductory mechanics book. Thanks for reminding me of this book.
– Sou
Jul 17 at 18:57











2 Answers
2






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The argument can be made more rigorous by using the well-known
$displaystylelim_xto0sin xover x=1$:
$$
left|Delta AoverDelta tright|=2Asin(Deltatheta/2)overDelta t
=2Asin(Deltatheta/2)overDeltatheta/2Deltatheta/2overDelta t
=Asin(Deltatheta/2)overDeltatheta/2DeltathetaoverDelta t,
$$
and $displaystylesin(Deltatheta/2)overDeltatheta/2to1$, because $Deltathetato0$ as $Delta tto0$.






share|cite|improve this answer




























    up vote
    0
    down vote













    If you are looking for an intuitive way to justify your book, I repeat my comment above:




    Your question is perfectly valid. Merely using differentials is a bit hand-wavy here, but the idea is that $Delta theta$ is the difference between the vectors $A(t+Δt)$ and $A(t)$, and as $Δt→0$, $Δθ→0$. The rate at which $Δθ→0$ is linearly related to the rate at which $Δt→0$ by some basic geometry about circles




    I also provide the following if you want an alternative, perhaps more mathematically satisfying approach:



    Consider the image at the bottom of this post (from Wikipedia), where we can denote the vector in the diagram with radius $r$ by $bfA$$(t)$ as your textbook does. Then we have $bfA$$(theta)= left[rcostheta,rsinthetaright]$ so $bfv$$(t) = fracdbf A(t)dt = fracdbf A(theta)dtheta fracdthetadt =left[-rsintheta,rcosthetaright]fracdthetadt$ (where we used the chain rule) so that $|bfv(t)| = sqrt(-rsintheta)^2+(rcostheta)^2fracdthetadt = sqrtr^2(sin^2theta+cos^2theta)fracdthetadt = rfracdthetadt$



    Which is precisely what your textbook claims.



    enter image description here






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      2 Answers
      2






      active

      oldest

      votes








      2 Answers
      2






      active

      oldest

      votes









      active

      oldest

      votes






      active

      oldest

      votes








      up vote
      0
      down vote



      accepted










      The argument can be made more rigorous by using the well-known
      $displaystylelim_xto0sin xover x=1$:
      $$
      left|Delta AoverDelta tright|=2Asin(Deltatheta/2)overDelta t
      =2Asin(Deltatheta/2)overDeltatheta/2Deltatheta/2overDelta t
      =Asin(Deltatheta/2)overDeltatheta/2DeltathetaoverDelta t,
      $$
      and $displaystylesin(Deltatheta/2)overDeltatheta/2to1$, because $Deltathetato0$ as $Delta tto0$.






      share|cite|improve this answer

























        up vote
        0
        down vote



        accepted










        The argument can be made more rigorous by using the well-known
        $displaystylelim_xto0sin xover x=1$:
        $$
        left|Delta AoverDelta tright|=2Asin(Deltatheta/2)overDelta t
        =2Asin(Deltatheta/2)overDeltatheta/2Deltatheta/2overDelta t
        =Asin(Deltatheta/2)overDeltatheta/2DeltathetaoverDelta t,
        $$
        and $displaystylesin(Deltatheta/2)overDeltatheta/2to1$, because $Deltathetato0$ as $Delta tto0$.






        share|cite|improve this answer























          up vote
          0
          down vote



          accepted







          up vote
          0
          down vote



          accepted






          The argument can be made more rigorous by using the well-known
          $displaystylelim_xto0sin xover x=1$:
          $$
          left|Delta AoverDelta tright|=2Asin(Deltatheta/2)overDelta t
          =2Asin(Deltatheta/2)overDeltatheta/2Deltatheta/2overDelta t
          =Asin(Deltatheta/2)overDeltatheta/2DeltathetaoverDelta t,
          $$
          and $displaystylesin(Deltatheta/2)overDeltatheta/2to1$, because $Deltathetato0$ as $Delta tto0$.






          share|cite|improve this answer













          The argument can be made more rigorous by using the well-known
          $displaystylelim_xto0sin xover x=1$:
          $$
          left|Delta AoverDelta tright|=2Asin(Deltatheta/2)overDelta t
          =2Asin(Deltatheta/2)overDeltatheta/2Deltatheta/2overDelta t
          =Asin(Deltatheta/2)overDeltatheta/2DeltathetaoverDelta t,
          $$
          and $displaystylesin(Deltatheta/2)overDeltatheta/2to1$, because $Deltathetato0$ as $Delta tto0$.







          share|cite|improve this answer













          share|cite|improve this answer



          share|cite|improve this answer











          answered Jul 17 at 8:39









          Aretino

          21.8k21342




          21.8k21342




















              up vote
              0
              down vote













              If you are looking for an intuitive way to justify your book, I repeat my comment above:




              Your question is perfectly valid. Merely using differentials is a bit hand-wavy here, but the idea is that $Delta theta$ is the difference between the vectors $A(t+Δt)$ and $A(t)$, and as $Δt→0$, $Δθ→0$. The rate at which $Δθ→0$ is linearly related to the rate at which $Δt→0$ by some basic geometry about circles




              I also provide the following if you want an alternative, perhaps more mathematically satisfying approach:



              Consider the image at the bottom of this post (from Wikipedia), where we can denote the vector in the diagram with radius $r$ by $bfA$$(t)$ as your textbook does. Then we have $bfA$$(theta)= left[rcostheta,rsinthetaright]$ so $bfv$$(t) = fracdbf A(t)dt = fracdbf A(theta)dtheta fracdthetadt =left[-rsintheta,rcosthetaright]fracdthetadt$ (where we used the chain rule) so that $|bfv(t)| = sqrt(-rsintheta)^2+(rcostheta)^2fracdthetadt = sqrtr^2(sin^2theta+cos^2theta)fracdthetadt = rfracdthetadt$



              Which is precisely what your textbook claims.



              enter image description here






              share|cite|improve this answer

























                up vote
                0
                down vote













                If you are looking for an intuitive way to justify your book, I repeat my comment above:




                Your question is perfectly valid. Merely using differentials is a bit hand-wavy here, but the idea is that $Delta theta$ is the difference between the vectors $A(t+Δt)$ and $A(t)$, and as $Δt→0$, $Δθ→0$. The rate at which $Δθ→0$ is linearly related to the rate at which $Δt→0$ by some basic geometry about circles




                I also provide the following if you want an alternative, perhaps more mathematically satisfying approach:



                Consider the image at the bottom of this post (from Wikipedia), where we can denote the vector in the diagram with radius $r$ by $bfA$$(t)$ as your textbook does. Then we have $bfA$$(theta)= left[rcostheta,rsinthetaright]$ so $bfv$$(t) = fracdbf A(t)dt = fracdbf A(theta)dtheta fracdthetadt =left[-rsintheta,rcosthetaright]fracdthetadt$ (where we used the chain rule) so that $|bfv(t)| = sqrt(-rsintheta)^2+(rcostheta)^2fracdthetadt = sqrtr^2(sin^2theta+cos^2theta)fracdthetadt = rfracdthetadt$



                Which is precisely what your textbook claims.



                enter image description here






                share|cite|improve this answer























                  up vote
                  0
                  down vote










                  up vote
                  0
                  down vote









                  If you are looking for an intuitive way to justify your book, I repeat my comment above:




                  Your question is perfectly valid. Merely using differentials is a bit hand-wavy here, but the idea is that $Delta theta$ is the difference between the vectors $A(t+Δt)$ and $A(t)$, and as $Δt→0$, $Δθ→0$. The rate at which $Δθ→0$ is linearly related to the rate at which $Δt→0$ by some basic geometry about circles




                  I also provide the following if you want an alternative, perhaps more mathematically satisfying approach:



                  Consider the image at the bottom of this post (from Wikipedia), where we can denote the vector in the diagram with radius $r$ by $bfA$$(t)$ as your textbook does. Then we have $bfA$$(theta)= left[rcostheta,rsinthetaright]$ so $bfv$$(t) = fracdbf A(t)dt = fracdbf A(theta)dtheta fracdthetadt =left[-rsintheta,rcosthetaright]fracdthetadt$ (where we used the chain rule) so that $|bfv(t)| = sqrt(-rsintheta)^2+(rcostheta)^2fracdthetadt = sqrtr^2(sin^2theta+cos^2theta)fracdthetadt = rfracdthetadt$



                  Which is precisely what your textbook claims.



                  enter image description here






                  share|cite|improve this answer













                  If you are looking for an intuitive way to justify your book, I repeat my comment above:




                  Your question is perfectly valid. Merely using differentials is a bit hand-wavy here, but the idea is that $Delta theta$ is the difference between the vectors $A(t+Δt)$ and $A(t)$, and as $Δt→0$, $Δθ→0$. The rate at which $Δθ→0$ is linearly related to the rate at which $Δt→0$ by some basic geometry about circles




                  I also provide the following if you want an alternative, perhaps more mathematically satisfying approach:



                  Consider the image at the bottom of this post (from Wikipedia), where we can denote the vector in the diagram with radius $r$ by $bfA$$(t)$ as your textbook does. Then we have $bfA$$(theta)= left[rcostheta,rsinthetaright]$ so $bfv$$(t) = fracdbf A(t)dt = fracdbf A(theta)dtheta fracdthetadt =left[-rsintheta,rcosthetaright]fracdthetadt$ (where we used the chain rule) so that $|bfv(t)| = sqrt(-rsintheta)^2+(rcostheta)^2fracdthetadt = sqrtr^2(sin^2theta+cos^2theta)fracdthetadt = rfracdthetadt$



                  Which is precisely what your textbook claims.



                  enter image description here







                  share|cite|improve this answer













                  share|cite|improve this answer



                  share|cite|improve this answer











                  answered Jul 17 at 8:48









                  Brevan Ellefsen

                  11.4k31449




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