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Распространение волн в нелокальной среде с нелинейными источниками энергии
source is a nonlinear function of temperature. An example of a nonclassical material is a medium
New equations of convolution type obtained by replacing the integral by its maximumWe study the nonlinear equation max g(γ)|cos(γ - α)| = f(α), γεℝ where f(α) is a given function
Exponentially convergent galerkin method for numerical modeling of lasing in microcavities with piercing holes of microring lasers. The original problem is reduced to a nonlinear eigenvalue problem for a system of Muller
SINUSOIDAL VELAROIDAL SHELL - NUMERICAL MODELLING OF THE NONLINEAR BUCKLING RESISTANCE shells of complex geometry, many things remained to do. Four different sources of nonlinearity exist
Generalized interpolating polynomial operator An which puts into correspondence an arbitrary 2π - periodic function with zero mean trigonometric
New equations of convolution type obtained by replacing the integral by its maximumWe study the nonlinear equation max g(γ)|cos(γ - α)| = f(α), γεℝ where f(α) is a given function
Диффузионно-кинетические процессы в неравновесных теплофизических системах с источниками энергии Часть 1. Дисперсия нелинейных тепловых волн. The nonlinear properties of these thermophysical systems are driven by the fact that volume energy sources
On justification of general polynomial projection method for solving periodic fractional integral equationstrigonometric approximation
About the convergence of the general projection polynomial method for a class of periodic fractional-integral equationstrigonometric approximation
A GCD-weighted Trigonometric SumA GCD-weighted Trigonometric Sum
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