554 research outputs found

    Interior error estimate for periodic homogenization

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    In a previous article about the homogenization of the classical problem of diff usion in a bounded domain with su ciently smooth boundary we proved that the error is of order Ο΅1/2\epsilon^{1/2}. Now, for an open set with su ciently smooth boundary C1,1C^{1,1} and homogeneous Dirichlet or Neuman limits conditions we show that in any open set strongly included in the error is of order Ο΅\epsilon. If the open set Ξ©βŠ‚Rn\Omega\subset R^n is of polygonal (n=2) or polyhedral (n=3) boundary we also give the global and interrior error estimates

    Strain Hardening in Polymer Glasses: Limitations of Network Models

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    Simulations are used to examine the microscopic origins of strain hardening in polymer glasses. While traditional entropic network models can be fit to the total stress, their underlying assumptions are inconsistent with simulation results. There is a substantial energetic contribution to the stress that rises rapidly as segments between entanglements are pulled taut. The thermal component of stress is less sensitive to entanglements, mostly irreversible, and directly related to the rate of local plastic arrangements. Entangled and unentangled chains show the same strain hardening when plotted against the microscopic chain orientation rather than the macroscopic strain.Comment: 4 pages, 3 figure

    Particle dynamics inside shocks in Hamilton-Jacobi equations

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    Characteristics of a Hamilton-Jacobi equation can be seen as action minimizing trajectories of fluid particles. For nonsmooth "viscosity" solutions, which give rise to discontinuous velocity fields, this description is usually pursued only up to the moment when trajectories hit a shock and cease to minimize the Lagrangian action. In this paper we show that for any convex Hamiltonian there exists a uniquely defined canonical global nonsmooth coalescing flow that extends particle trajectories and determines dynamics inside the shocks. We also provide a variational description of the corresponding effective velocity field inside shocks, and discuss relation to the "dissipative anomaly" in the limit of vanishing viscosity.Comment: 15 pages, no figures; to appear in Philos. Trans. R. Soc. series

    ΠŸΡ€ΠΎΠ±Π»Π΅ΠΌΠ° ΠΈΠ½Π΅Ρ€Ρ†ΠΈΠΈ ΠΈ антигравитация

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    The main aim of the present paper is to prove the possibility of the phenomenon of antigravity: as is shown by the example of plane curvilinear motion, the material bodies moving by inertia can repel each other. According to the criterion of antigravity obtained, the necessary condition for antigravity is the motion of a body by inertia along such a curvilinear trajectory on which the energy of the body is transferred from the rotational degree of freedom to the translational one. A control parameter is introduced with the change of which the character of particles motion changes: when the control parameter passes through some critical value, the force of attraction between particles is replaced by the repulsive force. Thus, the possibility to control the character of interaction between the particles of a physical system by redistributing the energy of the system between its degrees of freedom is unclosed. It is shown that the extension of the Newtonian scheme of mechanics by taking into consideration a broad class of curvilinear motions by inertia demands the refinement of the standard notion of inertia of the material body. The concept of inertia property should reflect the presence of dialectically opposite components of motion, associated with conservation of two characteristics of body motion β€” momentum and kinetic energy representing, accordingly, the force and energy measures of motion, mutually supplementing each other. The inertia property of body is that any body opposes to changing both momentum and kinetic energy. The tendency of the body to the conservation of momentum leads to the uniform and rectilinear motion (i.Β e. to translational inertia), and the tendency to kinetic energy conservation β€” to the curvilinear (accelerated) motion by inertia. Both types of inertial motion have a general feature β€” they can continue unrestrictedly long. The material bodies, moving along a curvilinear trajectory by inertia, are shown to generate electromagnetic field in environment. This field can be considered as a special physical medium which is created by bodies when they curvilinearly move by inertia and is capable to exert back action upon bodies. The results of the investigation presented in this paper allow one to make a guess that electromagnetism, as well as gravitation, is not a special kind of interaction. Electromagnetism is the interaction of material particles with mass that are in such states of curvilinear motion by inertia in which energy is transferred from some degrees of freedom to others.Π“Π»Π°Π²Π½Ρ‹ΠΉ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ настоящСй Ρ€Π°Π±ΠΎΡ‚Ρ‹ состоит Π² Π΄ΠΎΠΊΠ°Π·Π°Ρ‚Π΅Π»ΡŒΡΡ‚Π²Π΅ возмоТности явлСния Π°Π½Ρ‚ΠΈΠ³Ρ€Π°Π²ΠΈΡ‚Π°Ρ†ΠΈΠΈ: Π½Π° ΠΏΡ€ΠΈΠΌΠ΅Ρ€Π΅ плоского ΠΊΡ€ΠΈΠ²ΠΎΠ»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠ³ΠΎ двиТСния ΠΏΠΎ ΠΈΠ½Π΅Ρ€Ρ†ΠΈΠΈ ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, Ρ‡Ρ‚ΠΎ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΡŒΠ½Ρ‹Π΅ Ρ‚Π΅Π»Π°, ΠΎΠ±Π»Π°Π΄Π°ΡŽΡ‰ΠΈΠ΅ массой, ΠΌΠΎΠ³ΡƒΡ‚ ΠΎΡ‚Ρ‚Π°Π»ΠΊΠΈΠ²Π°Ρ‚ΡŒΡΡ Π΄Ρ€ΡƒΠ³ ΠΎΡ‚ Π΄Ρ€ΡƒΠ³Π°. УстановлСн ΠΊΡ€ΠΈΡ‚Π΅Ρ€ΠΈΠΉ Π°Π½Ρ‚ΠΈΠ³Ρ€Π°Π²ΠΈΡ‚Π°Ρ†ΠΈΠΈ, согласно ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΌΡƒ Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΡ‹ΠΌ условиСм Π°Π½Ρ‚ΠΈΠ³Ρ€Π°Π²ΠΈΡ‚Π°Ρ†ΠΈΠΈ являСтся ΠΏΠ΅Ρ€Π΅ΠΌΠ΅Ρ‰Π΅Π½ΠΈΠ΅ Ρ‚Π΅Π»Π° ΠΏΠΎ ΠΈΠ½Π΅Ρ€Ρ†ΠΈΠΈ ΠΏΠΎ Ρ‚Π°ΠΊΠΎΠΌΡƒ ΠΊΡ€ΠΈΠ²ΠΎΠ»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠΌΡƒ ΠΏΡƒΡ‚ΠΈ, Π½Π° ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΌ происходит ΠΏΠ΅Ρ€Π΅ΠΊΠ°Ρ‡ΠΊΠ° энСргии Ρ‚Π΅Π»Π° ΠΈΠ· Π²Ρ€Π°Ρ‰Π°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ стСпСни свободы Π² ΠΏΠΎΡΡ‚ΡƒΠΏΠ°Ρ‚Π΅Π»ΡŒΠ½ΡƒΡŽ. Π’Π²Π΅Π΄Π΅Π½ ΡƒΠΏΡ€Π°Π²Π»ΡΡŽΡ‰ΠΈΠΉ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€, с ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ΠΌ Π²Π΅Π»ΠΈΡ‡ΠΈΠ½Ρ‹ ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠ³ΠΎ измСняСтся Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ двиТСния Ρ‚Π΅Π»: ΠΏΡ€ΠΈ ΠΏΠ΅Ρ€Π΅Ρ…ΠΎΠ΄Π΅ ΡƒΠΏΡ€Π°Π²Π»ΡΡŽΡ‰Π΅Π³ΠΎ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Π° Ρ‡Π΅Ρ€Π΅Π· Π½Π΅ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠ΅ критичСскоС Π·Π½Π°Ρ‡Π΅Π½ΠΈΠ΅ сила притяТСния ΠΌΠ΅ΠΆΠ΄Ρƒ Ρ‚Π΅Π»Π°ΠΌΠΈ смСняСтся силой отталкивания. ΠžΡ‚ΠΊΡ€Ρ‹Π²Π°Π΅Ρ‚ΡΡ, Ρ‚Π°ΠΊΠΈΠΌ ΠΎΠ±Ρ€Π°Π·ΠΎΠΌ, Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡ‚ΡŒ управлСния Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ΠΎΠΌ взаимодСйствия ΠΌΠ΅ΠΆΠ΄Ρƒ частицами физичСской систСмы ΠΏΡƒΡ‚Π΅ΠΌ пСрСраспрСдСлСния энСргии систСмы ΠΌΠ΅ΠΆΠ΄Ρƒ Π΅Π΅ стСпСнями свободы. Показано, Ρ‡Ρ‚ΠΎ Ρ€Π°ΡΡˆΠΈΡ€Π΅Π½ΠΈΠ΅ Π½ΡŒΡŽΡ‚ΠΎΠ½ΠΎΠ²ΡΠΊΠΎΠΉ схСмы ΠΌΠ΅Ρ…Π°Π½ΠΈΠΊΠΈ ΠΏΡƒΡ‚Π΅ΠΌ Π²ΠΊΠ»ΡŽΡ‡Π΅Π½ΠΈΡ Π² рассмотрСниС ΠΎΠ±ΡˆΠΈΡ€Π½ΠΎΠ³ΠΎ класса ΠΊΡ€ΠΈΠ²ΠΎΠ»ΠΈΠ½Π΅ΠΉΠ½Ρ‹Ρ… Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΉ ΠΏΠΎ ΠΈΠ½Π΅Ρ€Ρ†ΠΈΠΈ Ρ‚Ρ€Π΅Π±ΡƒΠ΅Ρ‚ уточнСния общСпринятых прСдставлСний ΠΎ свойствС ΠΈΠ½Π΅Ρ€Ρ†ΠΈΠΈ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΡŒΠ½ΠΎΠ³ΠΎ Ρ‚Π΅Π»Π°. ΠŸΠΎΠ½ΡΡ‚ΠΈΠ΅ «свойство ΠΈΠ½Π΅Ρ€Ρ†ΠΈΠΈΒ» Π΄ΠΎΠ»ΠΆΠ½ΠΎ ΠΎΡ‚Ρ€Π°ΠΆΠ°Ρ‚ΡŒ Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ диалСктичСски ΠΏΡ€ΠΎΡ‚ΠΈΠ²ΠΎΠΏΠΎΠ»ΠΎΠΆΠ½Ρ‹Ρ… ΡΠΎΡΡ‚Π°Π²Π»ΡΡŽΡ‰ΠΈΡ… двиТСния, связанных с сохранСниСм Π΄Π²ΡƒΡ… характСристик двиТСния Ρ‚Π΅Π»Π° β€” ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ° ΠΈ кинСтичСской энСргии, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ ΠΏΡ€Π΅Π΄ΡΡ‚Π°Π²Π»ΡΡŽΡ‚ собой, соотвСтствСнно, ΡΠΈΠ»ΠΎΠ²ΡƒΡŽ ΠΈ ΡΠ½Π΅Ρ€Π³Π΅Ρ‚ΠΈΡ‡Π΅ΡΠΊΡƒΡŽ ΠΌΠ΅Ρ€Ρ‹ двиТСния, Π²Π·Π°ΠΈΠΌΠ½ΠΎ Π΄ΠΎΠΏΠΎΠ»Π½ΡΡŽΡ‰ΠΈΠ΅ Π΄Ρ€ΡƒΠ³ Π΄Ρ€ΡƒΠ³Π°. Бвойство ΠΈΠ½Π΅Ρ€Ρ†ΠΈΠΈ Ρ‚Π΅Π»Π° Π·Π°ΠΊΠ»ΡŽΡ‡Π°Π΅Ρ‚ΡΡ Π² Ρ‚ΠΎΠΌ, Ρ‡Ρ‚ΠΎ всякоС Ρ‚Π΅Π»ΠΎ сопротивляСтся измСнСнию ΠΊΠ°ΠΊ ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ°, Ρ‚Π°ΠΊ ΠΈ кинСтичСской энСргии. Π‘Ρ‚Ρ€Π΅ΠΌΠ»Π΅Π½ΠΈΠ΅ Ρ‚Π΅Π»Π° ΠΊ ΡΠΎΡ…Ρ€Π°Π½Π΅Π½ΠΈΡŽ ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ° ΠΏΡ€ΠΈΠ²ΠΎΠ΄ΠΈΡ‚ ΠΊ Ρ€Π°Π²Π½ΠΎΠΌΠ΅Ρ€Π½ΠΎΠΌΡƒ ΠΈ прямолинСйному двиТСнию (Ρ‚.Β Π΅. ΠΊ ΠΏΠΎΡΡ‚ΡƒΠΏΠ°Ρ‚Π΅Π»ΡŒΠ½ΠΎΠΉ ΠΈΠ½Π΅Ρ€Ρ†ΠΈΠΈ), Π° стрСмлСниС ΠΊ ΡΠΎΡ…Ρ€Π°Π½Π΅Π½ΠΈΡŽ кинСтичСской энСргии β€” ΠΊ ΠΊΡ€ΠΈΠ²ΠΎΠ»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠΌΡƒ (ускорСнному) двиТСнию ΠΏΠΎ ΠΈΠ½Π΅Ρ€Ρ†ΠΈΠΈ. Оба Ρ‚ΠΈΠΏΠ° двиТСния ΠΏΠΎ ΠΈΠ½Π΅Ρ€Ρ†ΠΈΠΈ Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ΠΈΠ·ΡƒΡŽΡ‚ΡΡ Ρ‚Π΅ΠΌ, Ρ‡Ρ‚ΠΎ ΠΎΠ½ΠΈ ΠΌΠΎΠ³ΡƒΡ‚ ΠΏΡ€ΠΎΠ΄ΠΎΠ»ΠΆΠ°Ρ‚ΡŒΡΡ сколь ΡƒΠ³ΠΎΠ΄Π½ΠΎ Π΄ΠΎΠ»Π³ΠΎ. Показано, Ρ‡Ρ‚ΠΎ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΡŒΠ½Ρ‹Π΅ частицы, двиТущиСся ΠΏΠΎ ΠΊΡ€ΠΈΠ²ΠΎΠ»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠΌΡƒ ΠΏΡƒΡ‚ΠΈ ΠΏΠΎ ΠΈΠ½Π΅Ρ€Ρ†ΠΈΠΈ, Π³Π΅Π½Π΅Ρ€ΠΈΡ€ΡƒΡŽΡ‚ элСктромагнитноС ΠΏΠΎΠ»Π΅ Π² ΠΎΠΊΡ€ΡƒΠΆΠ°ΡŽΡ‰Π΅ΠΌ пространствС. Π­Ρ‚ΠΎ ΠΏΠΎΠ»Π΅ ΠΌΠΎΠΆΠ½ΠΎ Ρ€Π°ΡΡΠΌΠ°Ρ‚Ρ€ΠΈΠ²Π°Ρ‚ΡŒ ΠΊΠ°ΠΊ ΠΎΡΠΎΠ±ΡƒΡŽ Ρ„ΠΈΠ·ΠΈΡ‡Π΅ΡΠΊΡƒΡŽ срСду, которая пороТдаСтся Ρ‚Π΅Π»Π°ΠΌΠΈ ΠΏΡ€ΠΈ ΠΈΡ… ΠΊΡ€ΠΈΠ²ΠΎΠ»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠΌ Π΄Π²ΠΈΠΆΠ΅Π½ΠΈΠΈ ΠΏΠΎ ΠΈΠ½Π΅Ρ€Ρ†ΠΈΠΈ ΠΈ способна ΠΎΠΊΠ°Π·Ρ‹Π²Π°Ρ‚ΡŒ ΠΎΠ±Ρ€Π°Ρ‚Π½ΠΎΠ΅ воздСйствиС Π½Π° Ρ‚Π΅Π»Π°. ΠŸΡ€Π΅Π΄ΡΡ‚Π°Π²Π»Π΅Π½Π½Ρ‹Π΅ Π² Ρ€Π°Π±ΠΎΡ‚Π΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ исслСдования ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‚ ΠΏΡ€Π΅Π΄ΠΏΠΎΠ»ΠΎΠΆΠΈΡ‚ΡŒ, Ρ‡Ρ‚ΠΎ элСктромагнСтизм, ΠΊΠ°ΠΊ ΠΈ гравитация, Π½Π΅ являСтся особым Π²ΠΈΠ΄ΠΎΠΌ взаимодСйствия. Π­Π»Π΅ΠΊΡ‚Ρ€ΠΎΠΌΠ°Π³Π½Π΅Ρ‚ΠΈΠ·ΠΌ β€” это взаимодСйствиС ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΡŒΠ½Ρ‹Ρ… частиц, ΠΎΠ±Π»Π°Π΄Π°ΡŽΡ‰ΠΈΡ… массой ΠΈ находящихся Π² особых состояниях ΠΊΡ€ΠΈΠ²ΠΎΠ»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠ³ΠΎ двиТСния ΠΏΠΎ ΠΈΠ½Π΅Ρ€Ρ†ΠΈΠΈ, Π² ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… происходит ΠΏΠ΅Ρ€Π΅ΠΊΠ°Ρ‡ΠΊΠ° энСргии ΠΈΠ· ΠΎΠ΄Π½ΠΈΡ… стСпСнСй свободы Π² Π΄Ρ€ΡƒΠ³ΠΈΠ΅

    Homogenization of Maxwell's equations in periodic composites

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    We consider the problem of homogenizing the Maxwell equations for periodic composites. The analysis is based on Bloch-Floquet theory. We calculate explicitly the reflection coefficient for a half-space, and derive and implement a computationally-efficient continued-fraction expansion for the effective permittivity. Our results are illustrated by numerical computations for the case of two-dimensional systems. The homogenization theory of this paper is designed to predict various physically-measurable quantities rather than to simply approximate certain coefficients in a PDE.Comment: Significantly expanded compared to v1. Accepted to Phys.Rev.E. Some color figures in this preprint may be easier to read because here we utilize solid color lines, which are indistinguishable in black-and-white printin

    Muon pair creation from positronium in a circularly polarized laser field

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    We study elementary particle reactions that result from the interaction of an atomic system with a very intense laser wave of circular polarization. As a specific example, we calculate the rate for the laser-driven reaction e+eβˆ’β†’ΞΌ+ΞΌβˆ’e^+e^- \to \mu^+\mu^-, where the electron and positron originate from a positronium atom or, alternatively, from a nonrelativistic e+eβˆ’e^+e^- plasma. We distinguish accordingly between the coherent and incoherent channels of the process. Apart from numerical calculations, we derive by analytical means compact formulas for the corresponding reaction rates. The rate for the coherent channel in a laser field of circular polarization is shown to be damped because of the destructive interference of the partial waves that constitute the positronium ground-state wave packet. Conditions for the observation of the process via the dominant incoherent channel in a circularly polarized field are pointed out

    Somatoform disorders in the family doctor's practice.

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    Somatoform disorders – psychoΒ­genic diseases are characterized by pathological physical symptoms that resemble somatic illness. Thus, any organic manifestations, which can be attributed to known diseases are not detected, but there are non-specific functional impairments. Somatoform disorders include somatization disorder, undifferentiated somatoform disorder, hypochoΒ­nΒ­driacal disorder, somatoform dysfunction of the autonomic nervous system and stable somatoform pain disorder. The first part of the article reviewes features of the clinical manifestations of somatization disorder and undifferentiated somatoform disorder. Role of non-benzodiazepine tranquilizers (ADAPTOL) and metabolic drugs (VASONAT) in the treatment of patients with somatoform disorders is discussed. In review article data of neurologists and cardiologists on the effectiveness of anxiolytic drug ADAPTOL and metabolic drug VASONAT in different clinical groups of patients (coronary artery disease, chronic ischemia of the brain), which can significantly improve quality of life, increase exercise tolerance, improve cognitive function and correct mental and emotional disorders are presented

    NUMERICAL STUDY OF OIL SPILL IN THE PATOS LAGOON ESTUARY REGION

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    The consumption pattern of the world population is based on petroleum derivatives, which despite contributing to the improvement of the quality of life, has negative aspects, mainly in the environmental scope. The number of oil spills in water slide has increased significantly in recent years. Considering the complexity of the marine environment, the present work aims to apply a identification system of the dynamics and dispersion of oil, using the numerical modeling in the region of Franceses Bridge, near to Patos Lagoon-RS, Brazil. The study of hypothetical events of oil leakage in the region is of fundamental importance, since the Riograndense Petroleum Refinery is located inside of the Patos Lagoon estuary. A data structure of atmospheric and oceanic circulation was organized and inserted in the coupling between the hydrodynamic module Telemac-3D and the ECOS oil model, during the period between 2010 and 2013. The coupling of these models provided satisfactory results, requiring a level of computational effort favorable to obtaining of results capable of giving technical and scientific support to studies such as those of environmental impacts and contingency plans
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