Can the graph of $tan^{-1}{left(frac{sin x}{x}right)}$ be expressed as $Ce^{-kx}cos(omega x + phi)$?












2














After graphing $sin x$, I thought of trying something interesting. I wanted to plot the angle $theta$ that a point $(x,sin x )$ makes with the origin on the $y$-axis, against $x$ on the $x$-axis.



$$tantheta = frac{sin x}{x}Rightarrow theta=tan^{-1}{left(frac{sin x}{x}right)}$$



Graphing $y = 20timestheta$ (multiply by 20 for graphical purposes):
Diagram 1



Part of it reminded me of the graph for the damped oscillator (specifically, the $x>0$ part).
That made me wonder if it was possible to find constants $C,k,omega,$ and $phi$ such that $$theta = Ce^{-kx}cos(omega x + phi)$$



However, after toying with Grapher for a while, $y = theta$ didn't seem to decrease exponentially.



That led me to this question: is there any analytical way to find real constants $C,k,omega,$ and $phi$ such that $theta = Ce^{-kx}cos(omega x + phi)$?



Furthermore, are there any complex constants $C,k,omega, text{and } phi$?










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  • No for real constants: the derivatives are quite different.
    – Bernard
    Apr 5 '17 at 8:54










  • Certainly not, there is a serious mismatch for negative $x$.
    – Yves Daoust
    Apr 5 '17 at 14:47


















2














After graphing $sin x$, I thought of trying something interesting. I wanted to plot the angle $theta$ that a point $(x,sin x )$ makes with the origin on the $y$-axis, against $x$ on the $x$-axis.



$$tantheta = frac{sin x}{x}Rightarrow theta=tan^{-1}{left(frac{sin x}{x}right)}$$



Graphing $y = 20timestheta$ (multiply by 20 for graphical purposes):
Diagram 1



Part of it reminded me of the graph for the damped oscillator (specifically, the $x>0$ part).
That made me wonder if it was possible to find constants $C,k,omega,$ and $phi$ such that $$theta = Ce^{-kx}cos(omega x + phi)$$



However, after toying with Grapher for a while, $y = theta$ didn't seem to decrease exponentially.



That led me to this question: is there any analytical way to find real constants $C,k,omega,$ and $phi$ such that $theta = Ce^{-kx}cos(omega x + phi)$?



Furthermore, are there any complex constants $C,k,omega, text{and } phi$?










share|cite|improve this question
























  • No for real constants: the derivatives are quite different.
    – Bernard
    Apr 5 '17 at 8:54










  • Certainly not, there is a serious mismatch for negative $x$.
    – Yves Daoust
    Apr 5 '17 at 14:47
















2












2








2


1





After graphing $sin x$, I thought of trying something interesting. I wanted to plot the angle $theta$ that a point $(x,sin x )$ makes with the origin on the $y$-axis, against $x$ on the $x$-axis.



$$tantheta = frac{sin x}{x}Rightarrow theta=tan^{-1}{left(frac{sin x}{x}right)}$$



Graphing $y = 20timestheta$ (multiply by 20 for graphical purposes):
Diagram 1



Part of it reminded me of the graph for the damped oscillator (specifically, the $x>0$ part).
That made me wonder if it was possible to find constants $C,k,omega,$ and $phi$ such that $$theta = Ce^{-kx}cos(omega x + phi)$$



However, after toying with Grapher for a while, $y = theta$ didn't seem to decrease exponentially.



That led me to this question: is there any analytical way to find real constants $C,k,omega,$ and $phi$ such that $theta = Ce^{-kx}cos(omega x + phi)$?



Furthermore, are there any complex constants $C,k,omega, text{and } phi$?










share|cite|improve this question















After graphing $sin x$, I thought of trying something interesting. I wanted to plot the angle $theta$ that a point $(x,sin x )$ makes with the origin on the $y$-axis, against $x$ on the $x$-axis.



$$tantheta = frac{sin x}{x}Rightarrow theta=tan^{-1}{left(frac{sin x}{x}right)}$$



Graphing $y = 20timestheta$ (multiply by 20 for graphical purposes):
Diagram 1



Part of it reminded me of the graph for the damped oscillator (specifically, the $x>0$ part).
That made me wonder if it was possible to find constants $C,k,omega,$ and $phi$ such that $$theta = Ce^{-kx}cos(omega x + phi)$$



However, after toying with Grapher for a while, $y = theta$ didn't seem to decrease exponentially.



That led me to this question: is there any analytical way to find real constants $C,k,omega,$ and $phi$ such that $theta = Ce^{-kx}cos(omega x + phi)$?



Furthermore, are there any complex constants $C,k,omega, text{and } phi$?







real-analysis complex-analysis trigonometry exponential-function graphing-functions






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edited Dec 9 at 4:36









user1101010

7551630




7551630










asked Apr 5 '17 at 8:46









Ujkan Sulejmani

1586




1586












  • No for real constants: the derivatives are quite different.
    – Bernard
    Apr 5 '17 at 8:54










  • Certainly not, there is a serious mismatch for negative $x$.
    – Yves Daoust
    Apr 5 '17 at 14:47




















  • No for real constants: the derivatives are quite different.
    – Bernard
    Apr 5 '17 at 8:54










  • Certainly not, there is a serious mismatch for negative $x$.
    – Yves Daoust
    Apr 5 '17 at 14:47


















No for real constants: the derivatives are quite different.
– Bernard
Apr 5 '17 at 8:54




No for real constants: the derivatives are quite different.
– Bernard
Apr 5 '17 at 8:54












Certainly not, there is a serious mismatch for negative $x$.
– Yves Daoust
Apr 5 '17 at 14:47






Certainly not, there is a serious mismatch for negative $x$.
– Yves Daoust
Apr 5 '17 at 14:47












2 Answers
2






active

oldest

votes


















1














The damping that you see is



$$frac{arctandfrac{sin x}x}{sin x}.$$



It is very close to the hyperbola $dfrac1x$, as you remain in the linear part of the arc tangent.






share|cite|improve this answer





















  • Is there an explanation as to why the damping/envelope is represented by that expression?
    – Ujkan Sulejmani
    Apr 5 '17 at 16:49










  • @UjkanSulejmani: look again, this is obvious.
    – Yves Daoust
    Apr 5 '17 at 17:40



















3














The envelope of $frac{sin x}{x}$ is $pm frac{1}{x}$, and for large $x$, $arctan frac{1}{x} approx frac{1}{x}$. So the decay of the function is inverse to $x$, not exponential, and no constant $k$ exists (real or complex; an imaginary part to $k$ will just introduce a sinusoidal oscillation in the envelope, in addition to the exponential decay or growth).






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    2 Answers
    2






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    2 Answers
    2






    active

    oldest

    votes









    active

    oldest

    votes






    active

    oldest

    votes









    1














    The damping that you see is



    $$frac{arctandfrac{sin x}x}{sin x}.$$



    It is very close to the hyperbola $dfrac1x$, as you remain in the linear part of the arc tangent.






    share|cite|improve this answer





















    • Is there an explanation as to why the damping/envelope is represented by that expression?
      – Ujkan Sulejmani
      Apr 5 '17 at 16:49










    • @UjkanSulejmani: look again, this is obvious.
      – Yves Daoust
      Apr 5 '17 at 17:40
















    1














    The damping that you see is



    $$frac{arctandfrac{sin x}x}{sin x}.$$



    It is very close to the hyperbola $dfrac1x$, as you remain in the linear part of the arc tangent.






    share|cite|improve this answer





















    • Is there an explanation as to why the damping/envelope is represented by that expression?
      – Ujkan Sulejmani
      Apr 5 '17 at 16:49










    • @UjkanSulejmani: look again, this is obvious.
      – Yves Daoust
      Apr 5 '17 at 17:40














    1












    1








    1






    The damping that you see is



    $$frac{arctandfrac{sin x}x}{sin x}.$$



    It is very close to the hyperbola $dfrac1x$, as you remain in the linear part of the arc tangent.






    share|cite|improve this answer












    The damping that you see is



    $$frac{arctandfrac{sin x}x}{sin x}.$$



    It is very close to the hyperbola $dfrac1x$, as you remain in the linear part of the arc tangent.







    share|cite|improve this answer












    share|cite|improve this answer



    share|cite|improve this answer










    answered Apr 5 '17 at 14:51









    Yves Daoust

    124k671221




    124k671221












    • Is there an explanation as to why the damping/envelope is represented by that expression?
      – Ujkan Sulejmani
      Apr 5 '17 at 16:49










    • @UjkanSulejmani: look again, this is obvious.
      – Yves Daoust
      Apr 5 '17 at 17:40


















    • Is there an explanation as to why the damping/envelope is represented by that expression?
      – Ujkan Sulejmani
      Apr 5 '17 at 16:49










    • @UjkanSulejmani: look again, this is obvious.
      – Yves Daoust
      Apr 5 '17 at 17:40
















    Is there an explanation as to why the damping/envelope is represented by that expression?
    – Ujkan Sulejmani
    Apr 5 '17 at 16:49




    Is there an explanation as to why the damping/envelope is represented by that expression?
    – Ujkan Sulejmani
    Apr 5 '17 at 16:49












    @UjkanSulejmani: look again, this is obvious.
    – Yves Daoust
    Apr 5 '17 at 17:40




    @UjkanSulejmani: look again, this is obvious.
    – Yves Daoust
    Apr 5 '17 at 17:40











    3














    The envelope of $frac{sin x}{x}$ is $pm frac{1}{x}$, and for large $x$, $arctan frac{1}{x} approx frac{1}{x}$. So the decay of the function is inverse to $x$, not exponential, and no constant $k$ exists (real or complex; an imaginary part to $k$ will just introduce a sinusoidal oscillation in the envelope, in addition to the exponential decay or growth).






    share|cite|improve this answer




























      3














      The envelope of $frac{sin x}{x}$ is $pm frac{1}{x}$, and for large $x$, $arctan frac{1}{x} approx frac{1}{x}$. So the decay of the function is inverse to $x$, not exponential, and no constant $k$ exists (real or complex; an imaginary part to $k$ will just introduce a sinusoidal oscillation in the envelope, in addition to the exponential decay or growth).






      share|cite|improve this answer


























        3












        3








        3






        The envelope of $frac{sin x}{x}$ is $pm frac{1}{x}$, and for large $x$, $arctan frac{1}{x} approx frac{1}{x}$. So the decay of the function is inverse to $x$, not exponential, and no constant $k$ exists (real or complex; an imaginary part to $k$ will just introduce a sinusoidal oscillation in the envelope, in addition to the exponential decay or growth).






        share|cite|improve this answer














        The envelope of $frac{sin x}{x}$ is $pm frac{1}{x}$, and for large $x$, $arctan frac{1}{x} approx frac{1}{x}$. So the decay of the function is inverse to $x$, not exponential, and no constant $k$ exists (real or complex; an imaginary part to $k$ will just introduce a sinusoidal oscillation in the envelope, in addition to the exponential decay or growth).







        share|cite|improve this answer














        share|cite|improve this answer



        share|cite|improve this answer








        edited Apr 5 '17 at 14:37

























        answered Apr 5 '17 at 14:07









        Connor Harris

        4,303723




        4,303723






























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