Geodesic on a sphere and on a plane in 2D

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SUMMARY

The discussion focuses on deriving the geodesic equations for a curve on a 2D plane and a sphere using calculus of variations. The participants utilize Euler's equation to establish that the shortest distance between two points on a plane is a straight line, represented by the equation \(y = Bx + C\). For the sphere, they discuss the relationship between the parameters \(\theta\) and \(\varphi\) and confirm that all geodesics are great circles due to rotational symmetry. The conversation also touches on the transition from equations (5.10.4) to (5.10.5) in a referenced text.

PREREQUISITES
  • Understanding of calculus of variations, specifically Euler's equation.
  • Familiarity with geodesics and their properties on different surfaces.
  • Knowledge of differential equations and their applications in physics.
  • Basic concepts of Lagrangian mechanics and motion in a plane.
NEXT STEPS
  • Study the derivation of geodesics on a sphere using Lagrangian mechanics.
  • Explore the implications of Euler's equation in calculus of variations.
  • Learn about the applications of geodesics in physics and engineering.
  • Investigate the transition between different forms of equations in calculus of variations.
USEFUL FOR

Students and professionals in mathematics, physics, and engineering who are interested in the principles of calculus of variations and geodesic equations. This discussion is particularly beneficial for those studying motion on curved surfaces and optimizing paths in various applications.

MatinSAR
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Homework Statement
Find the geodesic on a sphere and on a plane in 2D.
Relevant Equations
Calculus of variation.
I start with the 2D plane. Suppose y(x) is the curve that connects these two points. Its length is given by:
$$S=\int_1^2 \, ds=\int_1^2 (1+y'^2)^{\frac {1}{2}} \, dx$$ Applying Euler's equation we get:$$\frac {\partial f} {\partial y'}=A$$$$\dfrac {y'}{(1+y'^2)^{\frac {1}{2}}}=A$$ $$y'^{2}=\dfrac {A^2}{1-A^2}$$$$\dfrac {dy}{dx}=\pm (\dfrac {A^2}{1-A^2})^{\frac 1 2}=B$$$$dy=Bdx$$$$y=Bx+C$$
So the shortest distance is a line that connects the points. I know it is one of the easiest questions in calculus of variation, I just wanted to know If I learnt it correctly. Any suggustion would be appreciated.

For the sphere, My answer is completely similar to this:
1711129926847.png

My problem is that I don't know how to obtain 5.10.5 using 5.10.4 ...
Many thanks.
 

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The image sends me to the PF black hole …
 
  • Haha
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Solve algebraically for ##1/\theta’##?
 
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Orodruin said:
Solve algebraically for ##1/\theta’##?
1711130679017.png

I've done that before. I forget to post it.

Don't you have any idea for the 1st question @Orodruin?
 
docnet said:
$$\begin{align*}
\sin^2\theta &= a\sqrt{\theta'^2+\sin^2\theta}\\
\sin^4\theta &= a^2(\theta'^2+\sin^2\theta)
\end{align*}$$
Thanks, But I don't see any problem ...
 
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MatinSAR said:
Thanks, But I don't see any problem ...
That's because there isn't a problem.. I'm sorry I hit post before I was finished typing.
 
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MatinSAR said:
I've done that before. I forget to post it.
So where is the problem?

MatinSAR said:
Don't you have any idea for the 1st question @Orodruin?
What is the first question? The straight line equation? That looks fine to me so I don't see a problem there either.
 
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Orodruin said:
So where is the problem?


What is the first question? The straight line equation? That looks fine to me so I don't see a problem there either.
According to me:
$$\dfrac {1}{\theta'}=\dfrac {a\csc \theta}{(1-a^2 \csc^2 \theta)^{\frac 1 2}}$$
Which is not true.


I've just found my mistake in above equation.

Orodruin said:
What is the first question? The straight line equation?
Yes.
Orodruin said:
That looks fine to me so I don't see a problem there either.
Thanks.


Edit:
Many thanks @Orodruin and @docnet ...
 
  • #10
If you still wanted to know how to get (5.10.5) from (5.10.4):

\begin{align*}
\sin^2\theta&= a\sqrt{\theta'^2+\sin^2\theta} \\
\sin^4\theta &= a^2 (\theta'^2+\sin^2\theta) &\text{squared both sides} \\
\sin^4\theta &= a^2\theta'^2+a^2\sin^2\theta\\
\theta'^2 &= \frac{\sin^4\theta - a^2\sin^2\theta}{a^2} &\text{solved for } \theta'^2\\
\theta'^2 &= \frac{1-\frac{a^2}{\sin^2\theta}}{\frac{a^2}{\sin^4\theta}} &\text{divided numerator and denominator by } \sin^4\theta\\
\theta' &= \frac{\sqrt{1-\frac{a^2}{\sin^2\theta}}}{\frac{a}{\sin^2\theta}}& \text{square rooted both sides}\\
\theta' &= \frac{\sqrt{1-a^2\csc^2\theta}}{ a\csc^2\theta}\\
\frac{1}{\theta'}&= \frac{ a\csc^2\theta}{\sqrt{1-a^2\csc^2\theta}}.
\end{align*}
 
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  • #11
The easier way of doing the sphere:

Assume a curve parameter ##t##. It is then clear that ##\dot\theta## constant with ##\dot\varphi=0## solves the geodesic equations. By rotational symmetry, all geodesics are great circles.
 
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  • #12
docnet said:
If you still wanted to know how to get (5.10.5) from (5.10.4):
Thanks for your time.
Orodruin said:
The easier way of doing the sphere:

Assume a curve parameter ##t##. It is then clear that ##\dot\theta## constant with ##\dot\varphi=0## solves the geodesic equations. By rotational symmetry, all geodesics are great circles.
I'll try it. Many thanks.
 
  • #13
For the plane, I would start from <br /> L = (\dot x^2 + \dot y^2)^{1/2} which also gets the x = \mbox{constant} solution.
 
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  • #14
pasmith said:
For the plane, I would start from <br /> L = (\dot x^2 + \dot y^2)^{1/2} which also gets the x = \mbox{constant} solution.
Thank you @pasmith for your help. Is that ##L## lagrangian? And why ##x## and ##y## are functions of time? I haven't completed lagrangian and hamiltonian mechanics yet ...

I am currently reading calculus of variation and I wanted to solve using euler equation.

Edit:
I think you are dealing with the problem as motion of a particle in a plane. Then we should show that it is moving on a straight line with constant speed, right?
 
Last edited:

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