Showing 50 of 634 papers

The number of periodic solutions of the second kind to the differential equation $\ddot{\varphi}-f_1(\varphi)\dot{\varphi}-f_0(\varphi)=0$

G. I. Shilova
1967-01-01 RussiaRxiv: ru-196701.23975

The equation \begin{equation} \ddot{\varphi}-f_1(\varphi)\dot{\varphi}-f_0(\varphi)=0\tag{1} \label{1} \end{equation} is considered in the case where $f_0(\varphi)$ and $f_1(\varphi)$ are trigonometric polynomials of degree no higher than $n$, where $n$ is a fixed natural number. Equation (1) is equ…

Dynamical systems close to Hamiltonian ones

K. S. Sibirskii
1967-01-01 RussiaRxiv: ru-196701.25002

In problems related to determining the number of limit cycles bifurcating from a singular point of the second group, it is sometimes (RZhMat, 1965, 7B199) essential to establish the fact that for a system close to a Hamiltonian one, depending on a parameter $\mu$, under certain additional conditions…

Two-point and multi-point Taylor formulas

O. N. Litvin, V. L. Rvachev
1967-01-01 RussiaRxiv: ru-196701.31809

A formula is considered by which the value of the function $f(x)\in C^n$ on a given interval is determined through its values and the values of its derivatives at $m$ points ($m\ge2$) of the given interval. The considered examples demonstrate the possibility of effectively using the obtained general…

On the existence of an upper and a lower solution of a boundary value problem for a system of ordinary differential equations

A. N. Vityuk
1967-01-01 RussiaRxiv: ru-196701.34450

Under certain conditions imposed on the right-hand sides of the system of equations, the existence of upper and lower solutions to the boundary value problem for finite and countable systems of ordinary differential equations on an interval of a specific length is proven. Bibliography 2.

The structure of a solution of the equation $u'=U_0(\nu)u+\sum_{n=1}^\infty(\nu)u^{1+\alpha_n}\equiv U(u,\nu)$ in a small neighborhood of the origin

A. N. Erugin
1967-01-01 RussiaRxiv: ru-196701.35573

The article constructs a solution to the equation \begin{equation} u'=U_0(\nu)u+\sum_{n=1}^\infty(\nu)u^{1+\alpha_n}\equiv U(u,\nu)\tag{1} \label{1} \end{equation} where $u$ and $\nu$ are polar coordinates. At the same time, there is one case where the solution to equation \eqref{1} cannot be obtain…

The existence and uniqueness theorem for the Cauchy problem of a hyperbolic equation with self-regulating delay

D. G. Korenevskij, S. F. Feshchenko
1967-01-01 RussiaRxiv: ru-196701.43279

For a hyperbolic equation of the form $$U_{tx}=f(t,x,U(t,x),U(t-\tau,x),U_t(t,x),U_t(t-\tau,x),U_x(t,x)U_x(t-\tau,x))$$ with an initial function $\varphi(t,x)$ defined for $(t,x)\in[t_0-\tau_0,t_0]\times\Omega$ and with a delay $\tau=\tau(t,x,U,U_t,U_x)$ that depends not only on the independent vari…

The asymptotic representation of the solution of a boundary value problem for a system of ordinary differential equations with a complex parameter

M. Z. Ibragimkhalilov
1967-01-01 RussiaRxiv: ru-196701.46175

In connection with the study of one-dimensional mixed problems for second-order parabolic systems containing time derivatives in the boundary conditions, this paper provides an asymptotic representation of the solution to the spectral problem (1)–(2) for a system of ordinary differential equations o…

A problem on a pairing of equations of parabolic and hyperbolic types when time derivatives occur in the boundary conditions

E. A. Ostrovskii
1967-01-01 RussiaRxiv: ru-196701.57121

We consider the problem of finding a solution to the following system of equations: $$\frac{\partial u^{(1)}}{\partial t}=\sum_{l=0}^2C_{0l}^{(1)}(x)\frac{\partial^lu^{(1)}}{\partial x^l}+f^{(1)}(x,t),\quad x\in(a_1,b_1),\quad t\in(0,T),$$ $$\frac{\partial^2 u^{(2)}}{\partial t^2}=\sum_{\substack{{k…

The completeness of certain function systems

M. A. Aleksidze
1967-01-01 RussiaRxiv: ru-196701.60052

Linearly independent systems \begin{equation} {\ln r(x_i,y)},\quad\biggl{\frac{\partial}{\partial n_y}\ln r(x_i,y)\biggr}\quad(i=1,2,\dots), \label{1} \end{equation} are considered, where $x_i$ are uniformly distributed on the circle $S_1$, and $y \in S$; here, $S$ and $S_1$ are concentric circles. …

On the smoothness of thermal potentials. IV

L. I. Kamynin
1967-01-01 RussiaRxiv: ru-196701.69261

The paper considers an application of the theory of Panya’s special heat potential of a simple layer to a boundary value problem for a system of parabolic equations with discontinuous coefficients, arising in the study of the distribution of concentrations of substances involved in the vital process…