


Vol 240, No 3 (2019)
- Year: 2019
- Articles: 9
- URL: https://journal-vniispk.ru/1072-3374/issue/view/15013
Article
Anatolii Mykhailovych Samoilenko (On His 80th Birthday)



On One Singularly Perturbed System of Ordinary Differential Equations with Multiple Root of the Degenerate Equation
Abstract
We consider a boundary-value problem for a system of two ordinary differential equations of the second order with different powers of the small parameter as coefficients of the second derivatives in both equations. One equation of the degenerate system possesses a double root. This leads to qualitative differences between the asymptotics of the boundary-layer solution of the analyzed system and the known asymptotics in the case of simple roots of the equations of degenerate system, namely, the structure of the boundary-layer series changes, the boundary layers are multizone, and the standard algorithm used for the construction boundary-layer functions becomes inapplicable and requires significant modifications.






Asymptotic Behavior of the Solutions of Differential Equations with Double Singularity in a Conditionally Stable Case
Abstract
We consider a double singular perturbation of a boundary-value problem for a nonlinear system of ordinary differential equations. For a formal asymptotic solution constructed by the method of boundary functions and generalized inverse matrices and projectors, we prove an asymptotic property of the formal series.



On the Force Interaction in Problems of Dynamics of Elastic Reservoirs Partially Filled with Liquid
Abstract
We consider a nonlinear problem of determination of the forces of interaction between a moving reservoir with deformable walls and a liquid that partially fills the vessel. For the dynamics of the relative motion of mechanical systems in the gravity field, we establish theorems on variations of the principal vectors of momentum and angular momentum in the body–liquid system in the case where the center of mass of the system is unknown in advance. We formulate the principles of construction of the nonlinear mathematical models of motion of the analyzed mechanical systems as a whole in terms of nonlinear ordinary differential equations.



Exact and Approximate Solutions of the Spectral Problems for the Differential Schrödinger Operator with Polynomial Potential in ℝK, K ≥ 2
Abstract
We consider spectral problems for the Schrödinger operator with polynomial potentials in ℝK, K ≥ 2. By using a functional-discrete (FD-)method and the Maple computer algebra system, we determine a series of exact least eigenvalues for the potentials of special form. In the case where the traditional FD-method is divergent (the degree of the polynomial potential exceeds 2 at least in one variable), we propose a modification of the method, which proves to be quite efficient for the class of problems under consideration. The obtained theoretical results are illustrated by numerical examples.



Quasiperiodic Forced Oscillations of a Solid Body in the Field of a Quadratic Potential
Abstract
We consider a natural Lagrangian system that describes the motion of a solid body under the action of superposition of two potential force fields. The first field is a stationary field with quadratic potential, while the potential of the second field is linear in the space and depends on time as a quasiperiodic function. We establish sufficient conditions under which this system has a classical hyperbolic quasiperiodic solution, which locally minimizes the Lagrangian averaged over time.



Spread of Values of a Cantor-Type Fractal Continuous Nonmonotone Function
Abstract
By using the \( {Q}_5^{\ast } \)-representation of numbers
determined by the quinary alphabet A5 ≡ {0, 1, 2, 3, 4} and an infinite stochastic matrix ‖qik‖, i ∈ A5, k ∈ N, with positive elements (q0k + q1k + q2k + q3k + q4k = 1) such that \( {\prod}_{k=1}^{\infty}\underset{i}{\max}\left\{{q}_{ik}\right\}=0 \) and β0k = 0, βi + 1, k = βik + qik, \( i=\overline{0,4} \), we define a continuous Cantor-type function by the equality
where δ0n = 0, \( {\delta}_{1n}=\frac{2+{\varepsilon}_n}{4} \), \( {\delta}_{2n}=\frac{2}{4}={\delta}_{3n} \), and \( {\delta}_{4n}=\frac{2-{\varepsilon}_n}{4} \), i.e., δi + 1, n = δin + gin, n ∈ N, and (εn) is a given sequence of real numbers such that 0 ≤ εn ≤ 1. We prove that this function is well defined and continuous. Moreover, it does not have intervals of monotonicity, except the intervals where it is constant. A criterion of bounded variation of the function is also established. We are especially interested in the problem of level sets of the function and in the topological and metric properties of the images of Cantor-type sets.



Nonlinear Boundary-Layer Problems and Laminar Vortical Streams Generated by Resonant Sloshing in a Tank with Circular Base
Abstract
For a viscous incompressible liquid with laminar flows, we deduce nonlinear boundary-layer problems for the near-surface flows near wetted surfaces (wall and bottom) of a rigid tank with circular base partly filled with a liquid of finite depth. Under the assumption that the resonant steady-state inviscid liquid sloshing caused by the horizontal translational orbital motion of the tank with forcing frequency close to the lowest natural sloshing frequency is known, by adopting the Narimanov–Moiseev-type approximation of the above-mentioned inviscid sloshing, we construct an analytic asymptotic solution of the obtained boundary-layer problems. It is shown that the inviscid flows must contain a global stationary vortex component. A new nonlinear boundary-value problem governing this component is proposed.


