Geodesic on a sphere and on a plane in 2D

  • #1
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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  • #2
The image sends me to the PF black hole …
 
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  • #4
Solve algebraically for ##1/\theta’##?
 
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  • #5
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?
 
  • #6
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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  • #7
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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  • #8
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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  • #9
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 [tex]
L = (\dot x^2 + \dot y^2)^{1/2}[/tex] which also gets the [itex]x = \mbox{constant}[/itex] solution.
 
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  • #14
pasmith said:
For the plane, I would start from [tex]
L = (\dot x^2 + \dot y^2)^{1/2}[/tex] which also gets the [itex]x = \mbox{constant}[/itex] 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:

FAQ: Geodesic on a sphere and on a plane in 2D

What is a geodesic on a sphere?

A geodesic on a sphere is the shortest path between two points on the surface of the sphere. These paths are segments of great circles, which are circles that have the same center and radius as the sphere itself.

How is a geodesic different on a plane compared to a sphere?

On a plane, a geodesic is simply a straight line, since the shortest distance between two points in a flat, two-dimensional space is a straight line. On a sphere, however, the geodesic is a segment of a great circle, which accounts for the curvature of the sphere.

How do you calculate the geodesic distance between two points on a sphere?

The geodesic distance between two points on a sphere can be calculated using the haversine formula or the spherical law of cosines. These formulas take into account the spherical coordinates (latitude and longitude) of the two points and the radius of the sphere.

What is the significance of geodesics in navigation and geography?

Geodesics are crucial in navigation and geography because they represent the shortest path between two points on the Earth's surface. This is important for air and sea travel, where following a great circle route can save time and fuel compared to following a straight line on a map, which may not be the shortest path on the curved surface of the Earth.

Can geodesics be generalized to other surfaces beyond spheres and planes?

Yes, geodesics can be generalized to other surfaces, such as ellipsoids, hyperbolic surfaces, and more complex manifolds. The concept of a geodesic as the shortest path between two points applies to any surface, though the specific calculations and properties of the geodesics will depend on the geometry of the surface in question.

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