mathematics Article The Geometry of a Randers Rotational Surface with an Arbitrary Direction Wind Rattanasak Hama 1,*,† and Sorin V. Sabau 2,† 1 Faculty of Science and Industrial Technology, Surat Thani Campus, Prince of Songkla University, Surat Thani 84000, Thailand 2 Department of Biological Sciences, Sapporo Campus, Tokai University, Sapporo 005-8601, Japan;
[email protected] * Correspondence:
[email protected] † These authors contributed equally to this work. Received: 5 October 2020; Accepted: 11 November 2020; Published: 17 November 2020 Abstract: In the present paper, we study the global behaviour of geodesics of a Randers metric, defined on Finsler surfaces of revolution, obtained as the solution of the Zermelo’s navigation problem. Our wind is not necessarily a Killing field. We apply our findings to the case of the topological cylinder R × S1 and describe in detail the geodesics behaviour, the conjugate and cut loci. Keywords: geodesics; cut locus; Finsler manifolds 1. Introduction A Finsler surface (M, F) is a geometrical structure defined on a smooth 3-manifold S ⊂ TM whose the canonical projection p : S ! M is a surjective submersion such that for each x 2 M, the p-fiber −1 Sx = p (x) is a strictly convex curve including the origin Ox 2 Tx M. Here, we denote by TM the tangent bundle of M. This is actually equivalent to saying that (M, F) is a surface M endowed with a Minkowski norm in each tangent space Tx M that varies smoothly with the base point x 2 M all over the manifold. Obviously, S is the unit sphere bundle f(x, y) 2 TM : F(x, y) = 1g, also called the indicatrix bundle.