Optimizing Tunnel Design: Calculus of Variations on a Spherical Earth

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Homework Help Overview

The discussion revolves around optimizing the design of a tunnel on a spherical Earth to minimize travel time for a particle between two surface points. The problem is situated within the context of calculus of variations.

Discussion Character

  • Exploratory, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to derive the travel time using both polar and Cartesian coordinates, expressing velocity in terms of gravitational parameters and formulating a functional. They express uncertainty about the correctness of their functional and seek guidance on completing the problem.
  • Some participants suggest calculating the Euler-Lagrange differential equation and mention the possibility of using polar coordinates to simplify the problem, hinting at a known solution involving hypocycloids.
  • Others question the assumptions made, such as neglecting Coriolis effects, indicating a need for clarity on the problem's constraints.

Discussion Status

The discussion is ongoing, with participants exploring different methods and interpretations. Some guidance has been offered regarding the use of the Euler-Lagrange equation and the potential for simplification through polar coordinates. However, there is no explicit consensus on the approach to take.

Contextual Notes

Participants are navigating the complexities of a functional that depends on both x and y coordinates, which is noted as a challenge for the original poster. There is also mention of differing assumptions regarding the effects of gravity and frame of reference in the problem.

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Presume the Earth is spherical, homogeneous and of radius R. What should be the shape of a tunnel connecting two points on the surface in order to minimize the time it takes for a particle to travel between the two points.

I have had a go at doing it in both polar and cartesian co-ordinates but am getting stuck. I'm fairly sure we are supposed to do it in cartesian but this way is proving particularly tricky.

What i have done is this;

Using some basic physics and energy conservation I have found that

\displaystyle{v(r) = \sqrt{\frac{g}{R}(R^2 - r^2)}}

or

\displaystyle{v = \sqrt{\frac{g}{R}(R^2 - x^2 - y^2)}}

ds^2 = dx^2 + dy^2

ds = \sqrt{1 + (y')^2} \; dx

So \displaystyle{\int t = \frac{ds}{v} = \sqrt{\frac{R}{g}} \int \frac{\sqrt{1 + (y')^2}}{\sqrt{R^2 - x^2 - y^2} \; dx}

The functional is

\displaystyle{T[x, y, y'] = \sqrt{\frac{R}{g}} \frac{\sqrt{1 + (y')^2}}{\sqrt{R^2 - x^2 - y^2}}

This is the problem, I've never dealt with a functional like this before. Up until now, any functional has had a cyclic coordinate which has made it nice and simple. This fuctional depends explicitly on both x and y.

Is what I've done so far correct? How can I go about finishing the problem


The question also gives the answer that should be obtained

\displaystyle{x(\theta) = (R - r) \cos \left(\frac{R}{r}\theta \right) + r \cos \left(\frac{R - r}{R} \theta \right)}

and

\displaystyle{y(\theta) = (R - r) \sin \left(\frac{R}{r}\theta \right) - r \sin \left(\frac{R - r}{R} \theta \right)}
 
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bump... any ideas anyone?
 
Assuming your functional is correct, why don't you proceed with calculating the Euler-Lagrange differential equation. If you do it in polar coordiantes with the correct functional, the ELDE can be integrated once giving the equation for a hypocycloid in polar coordiantes. It can then be written parametrically giving you the answer your book provided. I don't know why your professor would have a bias towards either method, generally they like to see the simplest solution.
 
So you get to neglect Coriolis effects?

Carl
 
I found I a cool link on a GR brachistrone problem. It becomes an interesting problem in that there are then 2 distinct frames from which to minimize the travel time.
 

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