Regarding the shortest path connecting two points on a sphere of radius $R$












0












$begingroup$


Consider a path on the surface of the sphere given by a function $phi(theta)$. The line element along the path $phi$ is given by
$$
mathrm{d}s=Rmathrm{d}thetasqrt{1+left (frac{ mathrm{d} phi}{mathrm{d} theta}right )^2sin^2theta}.
$$

Deriving the Euler-Lagrange equation for $phi(theta)$, they lead to the differential equation
$$
frac{mathrm{d} phi}{mathrm{d} theta}=frac{c}{sinthetasqrt{sin^2theta-c^2}}tag{1}
$$

with $c$ some constant. Now, there are two things I'd like to figure out. How do I show that Euler-Lagrange equation is solved by
$$
phi=arcsin(C_1cottheta),
$$

where $C_1$ is constant? Determining such an integral is difficult for me. I think I should apply the identites identites $(arcsin x)'=frac{1}{sqrt{1-x^2}}$ and $(cot x)'=-frac{1}{sin^2(x)}$. Secondly, I want to transform $(1)$ into cartesian coordinates, but I am not sure how to do it. Should I use the trigonometric addition formula here?










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migrated from physics.stackexchange.com Dec 14 '18 at 21:05


This question came from our site for active researchers, academics and students of physics.


















  • $begingroup$
    Would Mathematics be a better home for this question?
    $endgroup$
    – Qmechanic
    Dec 14 '18 at 20:41










  • $begingroup$
    Yes, this is a pure math question. If it were in the context of a physics problem, like geodesics in GR, or the path of a moving particle I'd say otherwise.
    $endgroup$
    – ggcg
    Dec 14 '18 at 20:45
















0












$begingroup$


Consider a path on the surface of the sphere given by a function $phi(theta)$. The line element along the path $phi$ is given by
$$
mathrm{d}s=Rmathrm{d}thetasqrt{1+left (frac{ mathrm{d} phi}{mathrm{d} theta}right )^2sin^2theta}.
$$

Deriving the Euler-Lagrange equation for $phi(theta)$, they lead to the differential equation
$$
frac{mathrm{d} phi}{mathrm{d} theta}=frac{c}{sinthetasqrt{sin^2theta-c^2}}tag{1}
$$

with $c$ some constant. Now, there are two things I'd like to figure out. How do I show that Euler-Lagrange equation is solved by
$$
phi=arcsin(C_1cottheta),
$$

where $C_1$ is constant? Determining such an integral is difficult for me. I think I should apply the identites identites $(arcsin x)'=frac{1}{sqrt{1-x^2}}$ and $(cot x)'=-frac{1}{sin^2(x)}$. Secondly, I want to transform $(1)$ into cartesian coordinates, but I am not sure how to do it. Should I use the trigonometric addition formula here?










share|cite|improve this question











$endgroup$



migrated from physics.stackexchange.com Dec 14 '18 at 21:05


This question came from our site for active researchers, academics and students of physics.


















  • $begingroup$
    Would Mathematics be a better home for this question?
    $endgroup$
    – Qmechanic
    Dec 14 '18 at 20:41










  • $begingroup$
    Yes, this is a pure math question. If it were in the context of a physics problem, like geodesics in GR, or the path of a moving particle I'd say otherwise.
    $endgroup$
    – ggcg
    Dec 14 '18 at 20:45














0












0








0





$begingroup$


Consider a path on the surface of the sphere given by a function $phi(theta)$. The line element along the path $phi$ is given by
$$
mathrm{d}s=Rmathrm{d}thetasqrt{1+left (frac{ mathrm{d} phi}{mathrm{d} theta}right )^2sin^2theta}.
$$

Deriving the Euler-Lagrange equation for $phi(theta)$, they lead to the differential equation
$$
frac{mathrm{d} phi}{mathrm{d} theta}=frac{c}{sinthetasqrt{sin^2theta-c^2}}tag{1}
$$

with $c$ some constant. Now, there are two things I'd like to figure out. How do I show that Euler-Lagrange equation is solved by
$$
phi=arcsin(C_1cottheta),
$$

where $C_1$ is constant? Determining such an integral is difficult for me. I think I should apply the identites identites $(arcsin x)'=frac{1}{sqrt{1-x^2}}$ and $(cot x)'=-frac{1}{sin^2(x)}$. Secondly, I want to transform $(1)$ into cartesian coordinates, but I am not sure how to do it. Should I use the trigonometric addition formula here?










share|cite|improve this question











$endgroup$




Consider a path on the surface of the sphere given by a function $phi(theta)$. The line element along the path $phi$ is given by
$$
mathrm{d}s=Rmathrm{d}thetasqrt{1+left (frac{ mathrm{d} phi}{mathrm{d} theta}right )^2sin^2theta}.
$$

Deriving the Euler-Lagrange equation for $phi(theta)$, they lead to the differential equation
$$
frac{mathrm{d} phi}{mathrm{d} theta}=frac{c}{sinthetasqrt{sin^2theta-c^2}}tag{1}
$$

with $c$ some constant. Now, there are two things I'd like to figure out. How do I show that Euler-Lagrange equation is solved by
$$
phi=arcsin(C_1cottheta),
$$

where $C_1$ is constant? Determining such an integral is difficult for me. I think I should apply the identites identites $(arcsin x)'=frac{1}{sqrt{1-x^2}}$ and $(cot x)'=-frac{1}{sin^2(x)}$. Secondly, I want to transform $(1)$ into cartesian coordinates, but I am not sure how to do it. Should I use the trigonometric addition formula here?







integration mathematical-physics euler-lagrange-equation






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edited Dec 14 '18 at 21:07







UnknownW

















asked Dec 14 '18 at 20:34









UnknownWUnknownW

1,025922




1,025922




migrated from physics.stackexchange.com Dec 14 '18 at 21:05


This question came from our site for active researchers, academics and students of physics.









migrated from physics.stackexchange.com Dec 14 '18 at 21:05


This question came from our site for active researchers, academics and students of physics.














  • $begingroup$
    Would Mathematics be a better home for this question?
    $endgroup$
    – Qmechanic
    Dec 14 '18 at 20:41










  • $begingroup$
    Yes, this is a pure math question. If it were in the context of a physics problem, like geodesics in GR, or the path of a moving particle I'd say otherwise.
    $endgroup$
    – ggcg
    Dec 14 '18 at 20:45


















  • $begingroup$
    Would Mathematics be a better home for this question?
    $endgroup$
    – Qmechanic
    Dec 14 '18 at 20:41










  • $begingroup$
    Yes, this is a pure math question. If it were in the context of a physics problem, like geodesics in GR, or the path of a moving particle I'd say otherwise.
    $endgroup$
    – ggcg
    Dec 14 '18 at 20:45
















$begingroup$
Would Mathematics be a better home for this question?
$endgroup$
– Qmechanic
Dec 14 '18 at 20:41




$begingroup$
Would Mathematics be a better home for this question?
$endgroup$
– Qmechanic
Dec 14 '18 at 20:41












$begingroup$
Yes, this is a pure math question. If it were in the context of a physics problem, like geodesics in GR, or the path of a moving particle I'd say otherwise.
$endgroup$
– ggcg
Dec 14 '18 at 20:45




$begingroup$
Yes, this is a pure math question. If it were in the context of a physics problem, like geodesics in GR, or the path of a moving particle I'd say otherwise.
$endgroup$
– ggcg
Dec 14 '18 at 20:45










1 Answer
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$begingroup$

for your line element:



$left(frac{ds}{dt}right)^2=R^2,left(dot{vartheta}right)^2+
R^2,sin^2(vartheta)left(dot{varphi}right)^2
$



I get this differential equations :



$
ddot{vartheta}-frac{c^2cos(vartheta)}{R^4,m^2,sin^3(vartheta)}=0
$



and
$dot{varphi}=frac{c}{R^2,m,sin^2(vartheta)}$



There is no analytical solution ?






share|cite|improve this answer











$endgroup$













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    1 Answer
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    active

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    1 Answer
    1






    active

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    active

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    active

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    1












    $begingroup$

    for your line element:



    $left(frac{ds}{dt}right)^2=R^2,left(dot{vartheta}right)^2+
    R^2,sin^2(vartheta)left(dot{varphi}right)^2
    $



    I get this differential equations :



    $
    ddot{vartheta}-frac{c^2cos(vartheta)}{R^4,m^2,sin^3(vartheta)}=0
    $



    and
    $dot{varphi}=frac{c}{R^2,m,sin^2(vartheta)}$



    There is no analytical solution ?






    share|cite|improve this answer











    $endgroup$


















      1












      $begingroup$

      for your line element:



      $left(frac{ds}{dt}right)^2=R^2,left(dot{vartheta}right)^2+
      R^2,sin^2(vartheta)left(dot{varphi}right)^2
      $



      I get this differential equations :



      $
      ddot{vartheta}-frac{c^2cos(vartheta)}{R^4,m^2,sin^3(vartheta)}=0
      $



      and
      $dot{varphi}=frac{c}{R^2,m,sin^2(vartheta)}$



      There is no analytical solution ?






      share|cite|improve this answer











      $endgroup$
















        1












        1








        1





        $begingroup$

        for your line element:



        $left(frac{ds}{dt}right)^2=R^2,left(dot{vartheta}right)^2+
        R^2,sin^2(vartheta)left(dot{varphi}right)^2
        $



        I get this differential equations :



        $
        ddot{vartheta}-frac{c^2cos(vartheta)}{R^4,m^2,sin^3(vartheta)}=0
        $



        and
        $dot{varphi}=frac{c}{R^2,m,sin^2(vartheta)}$



        There is no analytical solution ?






        share|cite|improve this answer











        $endgroup$



        for your line element:



        $left(frac{ds}{dt}right)^2=R^2,left(dot{vartheta}right)^2+
        R^2,sin^2(vartheta)left(dot{varphi}right)^2
        $



        I get this differential equations :



        $
        ddot{vartheta}-frac{c^2cos(vartheta)}{R^4,m^2,sin^3(vartheta)}=0
        $



        and
        $dot{varphi}=frac{c}{R^2,m,sin^2(vartheta)}$



        There is no analytical solution ?







        share|cite|improve this answer














        share|cite|improve this answer



        share|cite|improve this answer








        edited Dec 15 '18 at 20:46

























        answered Dec 15 '18 at 16:00









        EliEli

        1234




        1234






























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