Classical Mechanics (Kibble & Berkshire) · Problem 13.14

Hamilton's equations and phase space — T.W.B. Kibble, F.H. Berkshire

Physics — Mechanics · geodesics-calculus-of-variations

Problem

Geodesics on a paraboloid Solve the problem of finding the shortest path between two points P(0,1,1)P(0, 1, 1) and Q(0,−1,1)Q(0, -1, 1) on the surface of the paraboloid z=x2+y2z = x^2 + y^2. Let C\mathcal{C} be a path lying in the surface that connects PP and QQ. Show that the length of C\mathcal{C} is given by L[r]=∫−π/2π/2[r2+(1+4r2)r˙2]1/2dθ,L[r] = \int_{-\pi/2}^{\pi/2} \left[r^2 + \left(1 + 4r^2\right)\dot{r}^2\right]^{1/2} d\theta, where r=r(θ)r = r(\theta) is the polar equation of the projection of C\mathcal{C} on to the plane z=0z = 0, and r˙\dot{r} means dr/dθdr/d\theta. Now find the function r(θ)r(\theta) that minimises LL. It is easier to work directly with the second order E-L equation (which can be found with computer assistance). Solve the E-L equation numerically with the initial conditions r(0)=λr(0) = \lambda, r˙(0)=0\dot{r}(0) = 0 and choose λ\lambda so that the path passes through PP (and, by symmetry, QQ). Plot the shortest path using 3D graphics.

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