Vol 71, No 1 (2025): Nonlocal and nonlinear problems
- Year: 2025
- Articles: 13
- URL: https://journals.rudn.ru/CMFD/issue/view/1858
- DOI: https://doi.org/10.22363/2413-3639-2025-71-1
Full Issue
Articles
On the nonlocal boundary value problem for the elliptic differential equations with integral type Samarskii-Ionkin conditions
Abstract
The present paper is devoted to the study of the abstract nonlocal boundary value problem with integral type Samarskii–Ionkin conditions for the differential equation of elliptic type \[\hspace{-6em} -u''(t)+Au(t)=f(t)\quad (0\leq t\leq T),\quad u\left( 0\right) =\varphi,\quad u'\left( 0\right) =u'\left( T\right) +\int\limits_{0}^{T}\alpha \left( s\right) u(s)ds+\psi.\quad\] in an arbitrary Banach space \(E\) with the positive operator \(A\). The well-posedness of this problem in various Banach spaces is established. In applications, theorems on the well-posedness of several nonlocal boundary value problems for elliptic equations with integral type Samarskii–Ionkin conditions are proved.



Inverse initial-boundary value problem for systems of quasilinear evolution equations of odd order
Abstract
An inverse initial-boundary value problem on a bounded interval for systems of quasilinear evolution equations of odd order is considered. Integral conditions are chosen as overdeterminations, and boundary functions and right-hand sides of equations of a special type are chosen as controls. Results on the existence and uniqueness of solutions for small initial data or a small time interval are established.



Splines, biharmonic operator and approximate eigenvalue
Abstract
The biharmonic operator plays a central role in a wide array of physical models, such as elasticity theory and the streamfunction formulation of the Navier–Stokes equations. Its spectral theory has been extensively studied. In particular the one-dimensional case (over an interval) serves as the basic model of a high order Sturm-Liouville problem. The need for corresponding numerical simulations has led to numerous works. This review focuses on a discrete biharmonic calculus. The primary object of this calculus is a high-order compact discrete biharmonic operator (DBO). The DBO is constructed in terms of the discrete Hermitian derivative. The surprising strong connection between cubic spline functions (on an interval) and the DBO is recalled. In particular the kernel of the inverse of the discrete operator is (up to scaling) equal to the grid evaluation of the kernel of \( \Big[\Big(\frac{d}{dx}\Big)^4\Big]^{-1}. \) This fact entails the conclusion that the eigenvalues of the DBO converge (at an “optimal” \(O(h^4)\) rate) to the continuous ones. Another consequence is the validity of a comparison principle. It is well known that there is no maximum principle for the fourth-order equation. However, a positivity result is recalled, both for the continuous and the discrete biharmonic equation, claiming that in both cases the kernels are order preserving.



Asymptotic solutions of the Vlasov-Poisson-Landau kinetic equations
Abstract
The paper is devoted to analytical and numerical study of solutions to the Vlasov–Poisson–Landau kinetic equations (VPLE) for distribution functions with typical length L such that \(\varepsilon = r_D/L \ll 1\), where \(r_D\) stands for the Debye radius. It is also assumed that the Knudsen number \({\rm K\!n} = l/L = O(1)\), where \(l\) denotes the mean free pass of electrons. We use the standard model of plasma of electrons with a spatially homogeneous neutralizing background of infinitely heavy ions. The initial data is always assumed to be close to neutral. We study an asymptotic behavior of the system for small \(\varepsilon > 0\). It is known that the formal limit of VPLE at \(\varepsilon = 0\) does not describe a rapidly oscillating part of the electric field. Our aim is to study the behavior of the “true” electric field near this limit. We consider the problem with standard isotropic in velocities Maxwellian initial conditions, and show that there is almost no damping of these oscillations in the collisionless case. An approximate formula for the electric field is derived and then confirmed numerically by using a simplified Bathnagar–Gross–Krook (BGK-type) model of Vlasov–Poisson–Landau equation (VPLE). Another class of initial conditions that leads to strong oscillations having the amplitude of order \(O(1/\varepsilon)\) is also considered. Numerical solutions of that class are studied for different values of parameters \(\varepsilon\) and \({\rm K\!n}\).



On the variational principle for a system of ordinary differential equations
Abstract
Necessary and sufficient conditions for the direct representability of one system of ordinary differential equations in the form of Lagrange-Ostrogradsky equations are obtained and the corresponding variational principle (the Hamilton-Ostrogradsky action) is constructed.



Applications of the s-harmonic extension to the study of singularities of Emden’s equations
Abstract
We use the Caffarelli–Silvestre extension to \( \mathrm{R}_+\times\mathrm{R}^N \) to study the isolated singularities of functions satisfying the semilinear fractional equation \( (-\Delta)^sv+\epsilon v^p=0 \) in a punctured domain of \( \mathrm{R}^N \) where \(\epsilon=\pm 1\), \(0 and \(p>1\). We emphasise the obtention of a priori estimates and analyse the set of self-similar solutions. We provide a complete description of the possible behaviour of solutions near a singularity.



Existence of weak solutions of the stationary alpha model describing the motion of polymer solutions
Abstract
In this paper, we study a boundary-value problem for a mathematical model describing the motion of aqueous polymer solutions. Based on the approximation-topological method, we investigate the existence of weak solutions of the problem under study. We consider the case of medium motion both in a bounded domain of two-dimensional or three-dimensional space and in an unbounded domain.



On the stitching of analytical and numerical solutions of the problem on a virtual boundary with the dominance of flow geometry in a bounded domain
Abstract
We are studying the following inverse PDE problem: to find geometric parameter of the domain of the time-dependent problem that match numerical one. Important feature is that discretization box of the interest contains source (fractures) generating transport in the porous media. From industrial point of view, we are building a machinery of the sewing the simulated pressure in the reservoir with analytical one. The goal is to obtain the value of the pressure function on the fracture (or near fracture) depending on the distance between multiple fractures (cf. [14]). For that, we generalize Einstein’s probabilistic method (see [5]) for the Brownian motion to study the fluids transport in porous media. We generalize Einstein’s paradigm to relate the average changes in the fluid density with the velocity of fluid and derive an anisotropic diffusion equation in nondivergence form that contains a convection term. This is then combined with the Darcy and the constitutive laws for compressible fluid flows to yield a nonlinear partial differential equations for the density function. Bernstein’s transformation is used to reduce the original nonlinear problem to the linear one. The method which we employ allow us to use a steady state analytical solution to interpret the result of numerical time-dependent pressure function on the fracture which takes into account 1-D geometry of the flow towards “long” fracture.



Local renormalized solutions of elliptic equations with variable exponents in unbounded domains
Abstract
In this paper, we consider a second-order quasilinear elliptic equation with variable nonlinearity exponents and a locally summable right-hand side. The stability property is established and, as a consequence, the existence of a local renormalized solution of the Dirichlet problem in an arbitrary unbounded domain is proved.



On globally smooth oscillating solutions of nonstrictly hyperbolic systems
Abstract
A class of nonstrictly hyperbolic systems of quasilinear equations with oscillatory solutions of the Cauchy problem, globally smooth in time in some open neighborhood of the zero stationary state, is found. For such systems, the period of oscillation of solutions does not depend on the initial point of the Lagrangian trajectory. The question of the possibility of constructing these systems in a physical context is also discussed, and nonrelativistic and relativistic equations of cold plasma are studied from this point of view.



Determination of the parameters of the mathematical model of the immune response to HIV
Abstract
Human immunodeficiency virus of type 1 (HIV) attacks the immune system and thereby weakens the defense against other infections and some types of cancer that the immune system of a healthy person can cope with. Despite the use of highly active antiretroviral therapy (HAART), there are no methods yet to completely eliminate HIV from the body of an infected person. However, due to the expansion of access to HIV prevention, diagnosis and treatment with HAART, HIV infection has moved into the category of controllable chronic diseases. Mathematical modeling methods are actively used to study the kinetic mechanisms of HIV pathogenesis and the development of personalized approaches to treatment based on combined immunotherapy. One of the central tasks of HIV infection modeling is to determine the individual parameters of the immune system response during the acute phase of HIV infection by solving inverse problems. To study the kinetics of the pathogenesis of HIV infection, a mathematical model of eight ordinary differential equations formulated by Bank et al. [5] was used. The system of equations of the model describes the change in the number of four subpopulations of CD4+ T cells and two types of CD8+ T cells. A feature of this model is the consideration of latently infected CD4+ T cells, which serve as the main reservoir of the viral population. The viral load on the human body is determined by the combination of populations of infectious and noninfectious viral particles. The inverse problem of parameter identification based on the data of the acute phase of HIV infection was studied. In particular, the identifiability of the parameters was studied and sensitivity analysis from the input data was performed. The inverse problem was reduced to a minimization problem using the evolutionary centers method.



On well-posedness of the free boundary problem for ideal compressible MHD equations and Maxwell equations in vacuum
Abstract
We survey results on the well-posedness of the free interface problem when an interface separates a perfectly conducting inviscid fluid (e.g., plasma) from a vacuum. The fluid flow is governed by the equations of ideal compressible magnetohydrodynamics (MHD). Unlike the classical statement, when the vacuum magnetic field obeys the div-curl system of pre-Maxwell dynamics, we do not neglect the displacement current in the vacuum region and consider the Maxwell equations for electric and magnetic fields. With boundary conditions on the interface this forms a nonlinear hyperbolic problem with a characteristic free boundary. The statement of this free boundary problem comes from the relativistic setting where the displacement current in vacuum cannot be neglected. We also briefly discuss the recent result showing the stabilizing effect of surface tension.



On homogenization of the Lavrent’ev-Bitsadze equation in a partially perforated domain with the third boundary condition on the boundary of the cavities. Subcritical, critical and supercritical cases
Abstract
For the Lavrent’ev—Bitsadze equation in a partially perforated model domain with a characteristic size of microinhomogeneities \(\varepsilon,\) we consider the problem with the third-kind boundary condition on the boundary of the cavities (the Fourier condition), which has a small parameter \(\varepsilon^\alpha\) as a multiplier in the coefficients, and the Dirichlet condition on the outer part of the boundary. For this problem, we construct a homogenized problem and prove the convergence of the solutions of the original problem to the solution of the homogenized problem in three cases. The subcritical case with \(\alpha>1\) is characterized by the fact that dissipation at the boundary of the cavities is negligibly small, in the critical case with \(\alpha=1\) a potential appears in the equation due to dissipation, and in the supercritical case with \(\alpha<1\) the dissipation plays the major role, it leads to degeneracy of the solution of the entire problem.


