7 research outputs found

    Survey: Local Consumer Sentiment is Stabilizing

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    In this paper a mathematical model describing small oscillations of a heterogeneous medium is considered. The medium consists of a partially perforated elastic material and a slightly viscous compressible fluid filling the pores. For the given model the corresponding homogenized problem is constructed by using the two-scale convergence method. The boundary conditions connecting equations of the homogenized model on the boundary between the continuous elastic material and the porous elastic material with fluid are foun

    Spectrum of One-dimensional Vibrations of a Layered Medium Consisting of a Kelvin-Voigt Material and a Viscous Incompressible Fluid

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    The paper considers a mathematical model for natural vibrations of a periodic layered medium. The medium consists of a viscoelastic Kelvin-Voigt material and a viscous incompressible fluid. For the given model, two homogenized models are derived. They correspond to the cases of transverse and longitudinal vibrations of the layered medium. It is shown that the spectrum of each homogenized model is the union of roots of the corresponding quadratic equations.РассмотрСна матСматичСская модСль, ΠΎΠΏΠΈΡΡ‹Π²Π°ΡŽΡ‰Π°Ρ собствСнныС колСбания пСриодичСской слоистой срСды, составлСнной ΠΈΠ· вязкоупругого ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π° КСльвина-Π€ΠΎΠΉΠ³Ρ‚Π° ΠΈ вязкой нСсТимаСмой Тидкости. Для Π΄Π°Π½Π½ΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ построСны Π΄Π²Π΅ усрСднСнныС ΠΌΠΎΠ΄Π΅Π»ΠΈ, ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΠ΅ ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½Ρ‹ΠΌΠΈΠΏΡ€ΠΎΠ΄ΠΎΠ»ΡŒΠ½Ρ‹ΠΌΠΊΠΎΠ»Π΅Π±Π°Π½ΠΈΡΠΌΡΠ»ΠΎΠΈΡΡ‚ΠΎΠΉΡΡ€Π΅Π΄Ρ‹. Показано,чтоспСктркаТдойусрСднСнноймодСли Π΅ΡΡ‚ΡŒ объСдинСниС ΠΊΠΎΡ€Π½Π΅ΠΉ ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΡ… ΠΊΠ²Π°Π΄Ρ€Π°Ρ‚Π½Ρ‹Ρ… ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ

    Spectrum of One-dimensional Vibrations of a Layered Medium Consisting of a Kelvin-Voigt Material and a Viscous Incompressible Fluid

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    The paper considers a mathematical model for natural vibrations of a periodic layered medium. The medium consists of a viscoelastic Kelvin-Voigt material and a viscous incompressible fluid. For the given model, two homogenized models are derived. They correspond to the cases of transverse and longitudinal vibrations of the layered medium. It is shown that the spectrum of each homogenized model is the union of roots of the corresponding quadratic equations.РассмотрСна матСматичСская модСль, ΠΎΠΏΠΈΡΡ‹Π²Π°ΡŽΡ‰Π°Ρ собствСнныС колСбания пСриодичСской слоистой срСды, составлСнной ΠΈΠ· вязкоупругого ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π° КСльвина-Π€ΠΎΠΉΠ³Ρ‚Π° ΠΈ вязкой нСсТимаСмой Тидкости. Для Π΄Π°Π½Π½ΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ построСны Π΄Π²Π΅ усрСднСнныС ΠΌΠΎΠ΄Π΅Π»ΠΈ, ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΠ΅ ΠΏΠΎΠΏΠ΅Ρ€Π΅Ρ‡Π½Ρ‹ΠΌΠΈΠΏΡ€ΠΎΠ΄ΠΎΠ»ΡŒΠ½Ρ‹ΠΌΠΊΠΎΠ»Π΅Π±Π°Π½ΠΈΡΠΌΡΠ»ΠΎΠΈΡΡ‚ΠΎΠΉΡΡ€Π΅Π΄Ρ‹. Показано,чтоспСктркаТдойусрСднСнноймодСли Π΅ΡΡ‚ΡŒ объСдинСниС ΠΊΠΎΡ€Π½Π΅ΠΉ ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΡ… ΠΊΠ²Π°Π΄Ρ€Π°Ρ‚Π½Ρ‹Ρ… ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ

    УсрСднСниС ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ акустики для частично ΠΏΠ΅Ρ€Ρ„ΠΎΡ€ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡƒΠΏΡ€ΡƒΠ³ΠΎΠ³ΠΎ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π° со слабовязкой ΠΆΠΈΠ΄ΠΊΠΎΡΡ‚ΡŒΡŽ

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    In this paper a mathematical model describing small oscillations of a heterogeneous medium is considered. The medium consists of a partially perforated elastic material and a slightly viscous compressible fluid filling the pores. For the given model the corresponding homogenized problem is constructed by using the two-scale convergence method. The boundary conditions connecting equations of the homogenized model on the boundary between the continuous elastic material and the porous elastic material with fluid are foundРассмотрСна матСматичСская модСль, ΠΎΠΏΠΈΡΡ‹Π²Π°ΡŽΡ‰Π°Ρ ΠΌΠ°Π»Ρ‹Π΅ колСбания Π³Π΅Ρ‚Π΅Ρ€ΠΎΠ³Π΅Π½Π½ΠΎΠΉ срСды, состо- ящСй ΠΈΠ· частично ΠΏΠ΅Ρ€Ρ„ΠΎΡ€ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡƒΠΏΡ€ΡƒΠ³ΠΎΠ³ΠΎ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π° ΠΈ слабовязкой сТимаСмой Тидкости, Π·Π°ΠΏΠΎΠ»Π½ΡΡŽΡ‰Π΅ΠΉ ΠΏΠΎΡ€Ρ‹. Для Π΄Π°Π½Π½ΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽ ΠΌΠ΅Ρ‚ΠΎΠ΄Π° Π΄Π²ΡƒΡ…ΠΌΠ°ΡΡˆΡ‚Π°Π±Π½ΠΎΠΉ сходимости постро- Π΅Π½Π° ΡΠΎΠΎΡ‚Π²Π΅Ρ‚ΡΡ‚Π²ΡƒΡŽΡ‰Π°Ρ усрСднСнная модСль ΠΈ Π½Π°ΠΉΠ΄Π΅Π½Ρ‹ Π³Ρ€Π°Π½ΠΈΡ‡Π½Ρ‹Π΅ условия, ΡΠ²ΡΠ·Ρ‹Π²Π°ΡŽΡ‰ΠΈΠ΅ уравнСния усрСднСнной ΠΌΠΎΠ΄Π΅Π»ΠΈ Π½Π° Π³Ρ€Π°Π½ΠΈΡ†Π΅ ΠΌΠ΅ΠΆΠ΄Ρƒ ΡΠΏΠ»ΠΎΡˆΠ½Ρ‹ΠΌ ΡƒΠΏΡ€ΡƒΠ³ΠΈΠΌ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠΌ ΠΈ пористым ΡƒΠΏΡ€ΡƒΠ³ΠΈΠΌ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠΌ с ΠΆΠΈΠ΄ΠΊΠΎΡΡ‚ΡŒ

    УсрСднСниС ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ акустики для частично ΠΏΠ΅Ρ€Ρ„ΠΎΡ€ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡƒΠΏΡ€ΡƒΠ³ΠΎΠ³ΠΎ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π° со слабовязкой ΠΆΠΈΠ΄ΠΊΠΎΡΡ‚ΡŒΡŽ

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    In this paper a mathematical model describing small oscillations of a heterogeneous medium is considered. The medium consists of a partially perforated elastic material and a slightly viscous compressible fluid filling the pores. For the given model the corresponding homogenized problem is constructed by using the two-scale convergence method. The boundary conditions connecting equations of the homogenized model on the boundary between the continuous elastic material and the porous elastic material with fluid are foun

    Π­Ρ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½Ρ‹Π΅ уравнСния акустики для слоистого ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π°, описываСмого Π΄Ρ€ΠΎΠ±Π½ΠΎΠΉ модСлью КСльвина-Π€ΠΎΠΉΠ³Ρ‚Π°

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    The paper is devoted to the construction of effective acoustic equations for a two-phase layered viscoelastic material described by the Kelvin–Voigt model with fractional time derivatives. For this purpose, the theory of two-scale convergence and the Laplace transform with respect to time are used. It is shown that the effective equations are partial integro-differential equations with fractional time derivatives and fractional exponential convolution kernels. In order to find the coefficients and the convolution kernels of these equations, several auxiliary cell problems are formulated and solvedΠ‘Ρ‚Π°Ρ‚ΡŒΡ посвящСна ΠΏΠΎΡΡ‚Ρ€ΠΎΠ΅Π½ΠΈΡŽ эффСктивных ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ акустики для Π΄Π²ΡƒΡ…Ρ„Π°Π·Π½ΠΎΠ³ΠΎ слоистого вязкоупругого ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π°, описываСмого модСлью ΠšΠ΅Π»ΡŒΠ²ΠΈΠ½Π°β€“Π€ΠΎΠΉΠ³Ρ‚Π° с Π΄Ρ€ΠΎΠ±Π½Ρ‹ΠΌΠΈ ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹ΠΌΠΈ ΠΏΠΎ Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ. Для этой Ρ†Π΅Π»ΠΈ ΠΈΡΠΏΠΎΠ»ΡŒΠ·ΡƒΠ΅Ρ‚ΡΡ тСория Π΄Π²ΡƒΡ…ΠΌΠ°ΡΡˆΡ‚Π°Π±Π½ΠΎΠΉ сходимости ΠΈ ΠΏΡ€Π΅ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½ΠΈΠ΅ Лапласа ΠΏΠΎ Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ. Показано, Ρ‡Ρ‚ΠΎ эффСктивныС уравнСния ΡΠ²Π»ΡΡŽΡ‚ΡΡ ΠΈΠ½Ρ‚Π΅Π³Ρ€ΠΎΠ΄ΠΈΡ„Ρ„Π΅Ρ€Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹ΠΌΠΈ уравнСниями Π² частных ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹Ρ… с Π΄Ρ€ΠΎΠ±Π½Ρ‹ΠΌΠΈ ΠΏΡ€ΠΎΠΈΠ·Π²ΠΎΠ΄Π½Ρ‹ΠΌΠΈ ΠΏΠΎ Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ ΠΈ Π΄Ρ€ΠΎΠ±Π½ΠΎ-ΡΠΊΡΠΏΠΎΠ½Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹ΠΌΠΈ ядрами свСртки. Для Ρ‚ΠΎΠ³ΠΎ Ρ‡Ρ‚ΠΎΠ±Ρ‹ Π½Π°ΠΉΡ‚ΠΈ коэффициСнты ΠΈ ядра свСрток этих ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ, сформулированы ΠΈ Ρ€Π΅ΡˆΠ΅Π½Ρ‹ нСсколько Π²ΡΠΏΠΎΠΌΠΎΠ³Π°Ρ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… Π·Π°Π΄Π°
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