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In this paper, we consider the motion of a particle on a surface of revolution under the influence of a central force field. We prove that there are at most two analytic central potentials for which all the bounded, nonsingular orbits are…

Dynamical Systems · Mathematics 2017-10-10 Manuele Santoprete

The generalization of Bertrand's theorem to the case of the motion of point particle on the surface of a cone is presented. The superintegrability of such models is discussed. The additional integrals of motion are analyzed for the case of…

Mathematical Physics · Physics 2015-06-17 Y. Brihaye , P. Kosiński , P. Maślanka

An elementary proof of Bertrand's theorem is given by examining the radial orbit equation, without needing to solve complicated equations or integrals.

Classical Physics · Physics 2015-06-23 Siu A. Chin

Bertrand's theorem in classical mechanics of the central force fields attracts us because of its predictive power. It categorically proves that there can only be two types of forces which can produce stable, circular orbits. In the present…

Classical Physics · Physics 2011-05-09 Prashant Kumar , Kaushik Bhattacharya

A celebrated result of Bertrand states that the only central force potentials on the plane with the property that all bounded orbits are periodic are the Kepler potential and the potential of the harmonic oscillator. In this paper, we…

Dynamical Systems · Mathematics 2024-08-27 Asselle Luca , Baranzini Stefano

We discuss an alternative non-perturbative proof of Bertrand's theorem that leads in a concise way directly to the two allowed fields: the newtonian and the isotropic harmonic oscillator central fields.

Classical Physics · Physics 2007-05-23 F C Santos , V Soares , A C Tort

A proof of the uniformization theorem of Riemann surface is given with only elementary properties of holomorphic functions and not using the paracompacity of the surface. This proof leans on an holomorphic version of the topological…

Complex Variables · Mathematics 2025-11-06 Alexis Marin , Dorothea Vienne-Pollak

The Bertrand theorem concluded that; the Kepler potential, and the isotropic harmonic oscillator potential are the only systems under which all the orbits are closed. It was never stressed enough in the physical or mathematical literature…

Classical Physics · Physics 2019-04-03 Munir Al-Hashimi

We give an explicit formula for singular surfaces of revolution with prescribed unbounded mean curvature. Using it, we give conditions for singularities of that surfaces. Periodicity of that surface is also discussed.

Differential Geometry · Mathematics 2018-04-12 Luciana F. Martins , Kentaro Saji , Samuel P. dos Santos , Keisuke Teramoto

In this paper, we prove a similar result to the fundamental theorem of regular surfaces in classical differential geometry, which extends the classical theorem to the entire class of singular surfaces in Euclidean 3-space known as frontals.…

Differential Geometry · Mathematics 2019-10-08 Tito Alexandro Medina Tejeda

It was known that if the Gaussian curvature function along each meridian on a surface of revolution $(R^2, dr^2+m(r)^2d\theta^2)$ is decreasing, then the cut locus of each point of $\theta^{-1}(0)$ is empty or a subarc of the opposite…

Differential Geometry · Mathematics 2022-08-12 Minoru Tanaka , Toyohiro Akamatsu , Robert Sinclair , Masaru Yamaguchi

The set of volumes of stable surfaces does have accumulation points. In this paper, we study this phenomenon for surfaces with one cyclic quotient singularity, towards answering the question under which conditions we can still have…

Algebraic Geometry · Mathematics 2021-07-06 Diana Torres

We derive an expression for the determination of the apsidal angles that holds good for arbitrary central potentials. Then we discuss under what conditions the apsidal angles remain independent of the mechanical energy and angular momentum…

Classical Physics · Physics 2013-04-18 Filadelfo C. Santos , Vitorvani Soares , Alexandre C. Tort

The Bertrand's theorem is extended, i.e. closed orbits still may exist for other central potentials than the power law Coulomb potential and isotropic harmonic oscillator. It is shown that for the combined potential $V(r)=W(r)+b/r^2$…

Quantum Physics · Physics 2009-10-31 Zuo-Bing Wu , Jin-Yan Zeng

In this work we obtain analytical expressions for the non-additivity effects in the dispersive interaction between two atoms and perfectly conducting surface of arbitrary shape in the non-retarded regime. We show that this three bodies…

Quantum Physics · Physics 2015-05-27 Reinaldo de Melo e Souza , W. J. M. Kort-Kamp , F. S. S. Rosa , C. Farina

We derive a generalized Stokes' theorem, valid in any dimension and for arbitrary loops, even if self intersecting or knotted. The generalized theorem does not involve an auxiliary surface, but inherits a higher rank gauge symmetry from the…

High Energy Physics - Theory · Physics 2008-02-03 N. Bralic

In this paper we prove explicit formulas for all Willmore surfaces of revolution and demonstrate their use in the discussion of the associated Dirichlet boundary value problems. It is shown by an explicit example that symmetric Dirichlet…

Differential Geometry · Mathematics 2017-09-22 Rainer Mandel

A procedure for constructing bound state potentials is given. We show that, under the natural conditions imposed on a radial eigenvalue problem, the only special cases of the general central potential, which are exactly solvable and have…

Quantum Physics · Physics 2011-07-19 N. Gurappa , Prasanta K. Panigrahi , T. Soloman Raju

An upper bound on the first S^1 invariant eigenvalue of the Laplacian for invariant metrics on the 2-sphere is used to find obstructions to the existence of isometric embeddings of such metrics in (R^3,can). As a corollary we prove: If the…

Differential Geometry · Mathematics 2007-05-23 Martin Engman

Existence and uniqueness of the scattering solutions is proved for a class of bounded rough obstacles which is much larger than the class of Lipschitz obstacles. Integral equations method is not used. The approach is based on the…

Mathematical Physics · Physics 2007-05-23 A. G. Ramm , M. Sammartino
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