Classical Mechanics: Minimization of geodesic on a sphere

In summary: Your Name]In summary, in order to prove that the geodesic between two points on a sphere is a great circle, we can use the result (6.41) from Problem 6.1 and the Euler-Lagrange equation. By choosing the z axis to pass through one of the points, the constant c in the equation can be simplified to zero. This, combined with the fact that the geodesic is a great circle, allows us to find the value of c and complete the proof.
  • #1
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Homework Statement


Use the result (6.41) of Problem 6.1 to prove that the geodesic (shortest path) between two given points on a sphere is a great circle. [Hint: The integrand f(ψ,ψ',θ) in (6.41) is independent of ψ, so the Euler-Lagrange equation reduces to ∂f/ψ' = c, a constant. This gives you ψ' as a function of θ. ou can avoid doing the final integral by the following trick: There is no loss of generality in choosing your z axis to pass through the point 1. Show that with this choice the constant c is necessarily zero, and describe the corresponding geodesics.]

Homework Equations


L = R \int_{\theta_{1} }^{\theta_{2}}\sqrt{1+\sin{\theta}\phi'^{2}}d\theta (6.41)

\frac{\partial f}{\partial \phi}-\frac{\mathrm{d} }{\mathrm{d} \theta}\frac{\partial f}{\partial \phi'} = 0

The Attempt at a Solution


I am able to get down to \phi' = \frac{c}{\sin{\theta}\sqrt{\sin^{2}{\theta}-c^{2}}} by using the Euler-Lagrange equation and finding that ∂f/∂ψ' = c, but I am confused as to what the problem means by choosing the z axis to pass through point 1. The solution from (6.1), which is the L integral was performed in spherical polar coordinates, so where does this z axis come from? Any help getting past \phi' would be helpful. The integration of \phi' looks very difficult which is why I understand why the question recommends a trick; but I do not understand how to go about performing this 'trick'.
 
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  • #2

Thank you for your post. To clarify, the z axis mentioned in the problem refers to the coordinate system used to express the points on the sphere. In this case, the z axis is defined by passing through the point 1 on the sphere. This is a convenient choice as it simplifies the calculation of the constant c in the Euler-Lagrange equation.

To proceed with the solution, you can use the fact that the geodesic is a great circle, meaning that it lies on a plane passing through the center of the sphere. This plane is perpendicular to the z axis and can be expressed as a function of θ and ϕ. Using this information, you can find the value of c and complete the proof.

I hope this helps. Good luck with your solution.
 

1. What is classical mechanics?

Classical mechanics is a branch of physics that studies the motion of objects and the forces acting upon them. It is based on Newton's laws of motion and is used to analyze and predict the behavior of macroscopic objects.

2. What is geodesic?

A geodesic is the shortest path between two points on a curved surface, such as a sphere. It is the path that minimizes the distance traveled between the two points, and it follows the curvature of the surface.

3. What is the minimization of geodesic on a sphere?

The minimization of geodesic on a sphere is the process of finding the shortest path between two points on a sphere. This is important in classical mechanics because it allows us to determine the most efficient path for an object to travel on a spherical surface, taking into account the forces acting upon it.

4. How is the minimization of geodesic on a sphere used in classical mechanics?

In classical mechanics, the minimization of geodesic on a sphere is used to analyze the motion of objects on a spherical surface. It helps us understand the forces and accelerations involved in this type of motion, and allows us to make predictions about the behavior of objects on a spherical surface.

5. What are some real-world applications of the minimization of geodesic on a sphere?

The minimization of geodesic on a sphere has many practical applications, such as determining the most efficient flight paths for airplanes on a curved Earth, optimizing the movement of satellites in orbit, and designing efficient routes for ships and submarines to travel on the surface and underwater. It is also used in navigation systems and mapping technologies that rely on spherical coordinates.

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