We show that on an open bounded smooth strongly pseudoconvex subset of C-n, there exists a Kahler-Einstein metric with positive Einstein constant, such that the metric restricted to the Levi distribution of the bounda...
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We show that on an open bounded smooth strongly pseudoconvex subset of C-n, there exists a Kahler-Einstein metric with positive Einstein constant, such that the metric restricted to the Levi distribution of the boundary is conformal to the Levi form. To achieve this, we solve an associated complex Monge-Ampere equation with Dirichlet boundary condition. We also prove uniqueness of the solution subject to additional restrictions.
For a linear boundaryvalue problem for a Fredholm integro-differential equation, we obtain necessary and sufficient conditions for the unique solvability in terms of a matrix Q (nu) (m) (h) formed on the basis of the...
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For a linear boundaryvalue problem for a Fredholm integro-differential equation, we obtain necessary and sufficient conditions for the unique solvability in terms of a matrix Q (nu) (m) (h) formed on the basis of the matrices of boundary conditions, the differential part, the integral term, and a partition with increment h > 0 of the interval on which the problem is defined.
We suggest a numerical method for solving systems of linear nonautonomous ordinary differential equations with nonseparated multipoint and integral conditions. By using this method, which is based on the operation of ...
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We suggest a numerical method for solving systems of linear nonautonomous ordinary differential equations with nonseparated multipoint and integral conditions. By using this method, which is based on the operation of convolution of integral conditions into local ones, one can reduce the solution of the original problem to the solution of a Cauchy problem for systems of ordinary differential equations and linear algebraic equations. We establish bounded linear growth of the error of the suggested numerical schemes. numerical experiments were carried out for specially constructed test problems.
This paper deals with the initial boundaryvalue problem for the nonlinear viscoelastic Petrovsky equation u(tt) + Delta(2)u - integral(t)(0)g(t - tau)Delta(2)u(x,tau)d tau - Delta u(t) - Delta u(u) + vertical bar u(t...
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This paper deals with the initial boundaryvalue problem for the nonlinear viscoelastic Petrovsky equation u(tt) + Delta(2)u - integral(t)(0)g(t - tau)Delta(2)u(x,tau)d tau - Delta u(t) - Delta u(u) + vertical bar u(t)vertical bar(m-1)u(t) = vertical bar u vertical bar(p-1)u. Under certain conditions on g and the assumption that m < p, we establish some asymptotic behavior and blow-up results for solutions with positive initial energy.
We discuss the existence of solution for the fully fourth-order boundaryvalue problem u((4)) = f(t, u, u', u '',u'''), 0 < t < 1, u(0) = u(1) = u ''(0) = u ''(1) = 0. A g...
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We discuss the existence of solution for the fully fourth-order boundaryvalue problem u((4)) = f(t, u, u', u '',u'''), 0 < t < 1, u(0) = u(1) = u ''(0) = u ''(1) = 0. A growth condition on f guaranteeing the existence of solution is presented. The discussion is based on the Fourier analysis method and Leray-Schauder fixed point theorem.
We consider the stationary incompressible Navier Stokes equations in the exterior of a disk B subset of R-2 with non-zero Dirichlet boundary conditions on the boundary of the disk and zero boundary conditions at infin...
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We consider the stationary incompressible Navier Stokes equations in the exterior of a disk B subset of R-2 with non-zero Dirichlet boundary conditions on the boundary of the disk and zero boundary conditions at infinity. We prove the existence of classical solutions for an open set of boundary conditions without symmetry. (C) 2013 Elsevier Inc. All rights reserved.
An algorithm for showing solution of systems of non-linear algebraic equations describing the steady-state behaviour of objects in the mechanics of a deformable solid is considered. The existence of limit points and s...
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An algorithm for showing solution of systems of non-linear algebraic equations describing the steady-state behaviour of objects in the mechanics of a deformable solid is considered. The existence of limit points and simple bifurcation points on the trajectory of the solution of the system is admitted and, at these points, the Jacobian matrix of the system, assumed to be real, symmetric and continuous, degenerates. The basis of the algorithm is a transformation of the space of the arguments of the solution of systems of non-linear algebraic equations using a rotation matrix formed from the eigenvectors of the Jacobian matrix. (C) 2013 Elsevier Ltd. All rights reserved.
A class of nonlinear fractional order differential equation D(0+)(alpha)u(t) + f (t, u(t)) = 0, 0 < t < 1, u(0) = 0, u(1) = 1/eta(alpha-1) u(eta) is investigated in this paper, where D-0+(alpha) is the standard ...
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A class of nonlinear fractional order differential equation D(0+)(alpha)u(t) + f (t, u(t)) = 0, 0 < t < 1, u(0) = 0, u(1) = 1/eta(alpha-1) u(eta) is investigated in this paper, where D-0+(alpha) is the standard Riemann-Liouville fractional derivative of order 1 < alpha <= 2, 0 < eta < 1, f is an element of C([0, 1] x R, R). Using intermediate value theorem, we obtain a sufficient condition for the existence of the solutions for the above fractional order differential equations.
We present numericalsolutions of the flow in precessing spheres and spherical shells with small (ri/ro=0.1) inner cores and either stress-free or no-slip inner boundary conditions. For each of these three cases we co...
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We present numericalsolutions of the flow in precessing spheres and spherical shells with small (ri/ro=0.1) inner cores and either stress-free or no-slip inner boundary conditions. For each of these three cases we consider the sequence of bifurcations as the Reynolds number Re=ro2Ω/ν is increased up to ∼1280, focusing particular attention on bifurcations that break the antipodal symmetry U(−r)=−U(r). All three cases have steady and time-periodic symmetric solutions at smaller Re, and quasiperiodic asymmetric solutions at larger Re, but the details of the transitions differ, and include also periodic asymmetric and quasiperiodic symmetric solutions in some of the cases.
Compressible momentum and energy equations were solved numerically for concentric micro annular tubes with slip velocity and temperature jump wall boundary conditions. The results were expressed in the form of the pro...
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Compressible momentum and energy equations were solved numerically for concentric micro annular tubes with slip velocity and temperature jump wall boundary conditions. The results were expressed in the form of the product of friction factor and Reynolds number (***) for a quasi-fully developed condition and for the ranges of Re < 1000 and Ma < 1. The numerical methodology was based on the Arbitrary-Lagrangian-Eulerian (ALE) method. The outer tube radius ranged from 5 to 40 mu m with radius ratios of 0.2, 0.5, and 0.8. The length to hydraulic diameter ratio was more than 100. The stagnation pressure was chosen in such a way that the exit Mach number ranged from 0.1 to 1.0, and the outlet pressure was fixed at the atmospheric pressure. For the case of incompressible slip flow, *** is calculated as a function of radius ratio and Knudsen number. For high speed flows, the values of *** for compressible slip flow were higher than those for incompressible slip flow due to compressibility effects. Also, *** correlation for compressible slip flow was obtained from compressible no-slip flow and incompressible slip flow as a function of Mach and Knudsen numbers and radius ratio. In addition, a correlation for microchannel, microtube, and micro annular tube was obtained from the authors' previous work.
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