Geodesic on a sphere and on a plane in 2D

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Homework Help Overview

The discussion revolves around finding geodesics on a sphere and a plane in a 2D context, utilizing calculus of variations. Participants explore the mathematical formulation of curves connecting two points and the implications of their lengths.

Discussion Character

  • Exploratory, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Some participants attempt to derive the shortest distance between points on a plane and relate it to geodesics on a sphere. Questions arise about specific equations and their derivations, particularly concerning the transition from one equation to another.

Discussion Status

Participants are actively engaging with the problem, sharing their attempts and questioning the validity of their equations. Some express uncertainty about specific steps in their reasoning, while others provide insights into the relationships between different formulations.

Contextual Notes

There are mentions of specific equations and references to external resources, indicating that some participants are working from established texts. The discussion also reflects a mix of familiarity with the subject matter, as some participants express uncertainty about foundational concepts in Lagrangian mechanics.

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 …
 
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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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