Geodesic on a sphere and on a plane in 2D

Click For Summary
The discussion centers on deriving geodesics on both a 2D plane and a sphere using calculus of variations. The user successfully demonstrates that the shortest distance between two points on a plane is a straight line, applying Euler's equation to derive the necessary equations. For the sphere, they seek clarification on transitioning between specific equations and confirm that all geodesics are great circles due to rotational symmetry. Participants provide insights and corrections, particularly regarding the application of Lagrangian mechanics and the interpretation of variables. The conversation emphasizes the importance of understanding the mathematical foundations behind geodesics in different geometries.
MatinSAR
Messages
673
Reaction score
204
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.
 

Attachments

  • 1711129875931.png
    1711129875931.png
    12.7 KB · Views: 75
Physics news on Phys.org
The image sends me to the PF black hole …
 
Solve algebraically for ##1/\theta’##?
 
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 ...
 
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.
 
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.
 
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*}
 
  • #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.
 
  • Like
Likes MatinSAR and docnet
  • #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.
 
  • Like
Likes Orodruin and MatinSAR
  • #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: