On Schnabl solutions of string field equations

We clarify the relationship between Schnabl’s solution and pure gauge configurations. Both Schnabl’s and pure gauge solutions are obtained by means of an iterative procedure. We show that the pure gauge string field configuration that is used in the construction of a perturbation series for Schnabl’s solution diverges on a large subspace of string configurations, but it can be rendered convergent by adding a compensating term. The additional term ensures the fulfillment of the equations of motion in a weak sense. This compensating term coincides with the term necessary for obtaining an action consistent with Sen’s first conjecture.     

On cauchy's equations of motion

Zusammenfassung Cauchys Bewegungs- und Momentengleichungen der klassischen Kontinuumsmechanik werden, mit Hilfe von Invarianz-Bedingungen gegenüber starren Zusatzbewegungen, aus dem Energietheorem hergeleitet.     

Baryon string model. II. Special solutions of classical three-string equations of motion

Conclusions We have considered the simplest solutions of the three-string equations of motion; these are solutions with a finite number of excited degrees of freedom. It is of interest to construct the quantum theory of such motions of the relativistic three-string. Quantum theory of a meson string with finite number of degrees of freedom was constructed in [4]. Quantization of finite-mode solutions of the baryon string model will be considered in the third paper of the present work.Institute of High Energy Physics, Serpukhov. Translated from Teoreticheskaya i Matematicheskaya Fizika. Vol. 64, No. 2, pp. 245–258, August, 1985.     

On the breakdown of classical solutions of the planar motion of an elastic string

We prove a result of formation of singularities for the classical solutions of the planar motion of a nonlinear elastic string. In a particular, but physically relevant, case we give a characterization of the global C¹ solutions with positive tension.     

Pure gauge configurations and tachyon solutions for cubic fermionic string field theory equations of motion

Special perturbative pure gauge solutions parameterized by a pair of wedge states are parts of the nontrivial (not purely gauge) tachyon solutions of the cubic fermionic string field theory describing the non-BPS brane true vacuum. We demonstrate explicitly that for the large parameter of the perturbation expansion, these pure gauge configurations are no longer solutions of the equations of motion. We show that this problem is solved by adding an extra term that is just the term needed for the first Sen conjecture to hold.     

On the linearization of the equations of motion of a rotating disk

In this paper, we present a consistent approach to reduce the fully nonlinear equations of a rotating disk to the classical linear equation derived by Lamb and Southwell and the nonlinear equations derived by Nowinski. The approach recognizes the fact that the out-of-plane deflection and the in-plane deflections are of different orders of magnitude. By using the ratio between the plate thickness and the outer radius as a measurement and carefully examining the reasonable magnitudes of all the variables involved, the fully nonlinear equations can be non-dimensionalized with all the terms being sorted according to their orders of magnitude. It is found that the classical linear equation derived by Lamb and Southwell can be recovered if all the terms of the lowest order of magnitude in the fully nonlinear equations are retained. If all the terms of the lowest two orders of magnitude are retained, Nowinski’s equations can then be recovered. Furthermore, the terms arising from in-plane deformation and rotary inertia are of the highest order and can be ignored in most of the applications.     

On the asymptotic solutions of the equations of motion of mechanical systems

The existence of solutions of the equations of motion of non-natural mechanical systems of a certain form which tend to a position of equilibrium when the time increases without limit is proved by the methods described in /1, 2/. The corresponding instability theorem is proved.     

On the holomorphic solutions of Hamiltonian equations of motion of point charges

The Maxwell–Lorenz system of electromagnetic fields interacting with charged particles (point charges) is studied in the Darwin approximation in which the Lagrangian and Hamiltonian of the particles are not coupled with the field. The solution of the equation of motion of particles with approximate Darwin Hamiltonian is found in a finite time interval by using the Cauchy theorem. The components of this solution are represented as holomorphic functions of time.     

On the governing equations of motion of nonholonomic systems on Riemannian manifolds

We propose a geometric approach to formulate the governing equations of motion for a class of nonholonomic systems on Riemannian manifolds. We first present a coordinate-free geometric formulation of the D’Alembert–Lagrange equation. Then by explicating this geometric formulation with respect to an arbitrary frame, we obtain the governing equations of motion in generalized form. The governing equations so obtained directly eliminate the dependent variations without using undetermined multipliers. As examples, we apply the formulation to a rigid body and a system with general first-order nonholonomic constraints; we also demonstrate their equivalences to the known results.     

On the solution of the equations of perturbed motion of an object-parachute system

We propose a method of finding the solutions of the equations of perturbed motion of an object-parachute system in analytic form. We perform an analysis of the roots of the characteristic equation of the linearized system. On the basis of the analysis we determine all the solutions of the equations of perturbed motion of the object-parachute system. We exhibit conditions under which the unperturbed motion (descent with slipping) is asymptotically stable.Translated fromDinamicheskie Sistemy, No. 6, 1987, pp. 41–46.     

On motion of the point algebraic singularity for two-dimensional nonlinear equations of hydrodynamics

Translated from Matematicheskie Zametki, Vol. 55, No. 3, pp. 11–20, March, 1994.