141 resultados para Estadística -- Mecànica


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Onsager's symmetry theorem for transport near equilibrium is extended in two directions. A corresponding symmetry is obtained for linear transport near nonequilibrium stationary states, and the class of transport laws is extended to include nonlocality in both space and time. The results are formally exact and independent of any specific model for the nonequilibrium state.

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We continue our study of classical mechanics using the methods of quantum mechanics. A Hilbert space is introduced, new conservation laws deduced, and the possibility of representing by new methods the many body classical problem discussed.

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To understand the origin of the dynamical transition, between high-temperature exponential relaxation and low-temperature nonexponential relaxation, that occurs well above the static transition in glassy systems, a frustrated spin model, with and without disorder, is considered. The model has two phase transitions, the lower being a standard spin glass transition (in the presence of disorder) or fully frustrated Ising (in the absence of disorder), and the higher being a Potts transition. Monte Carlo results clarify that in the model with (or without) disorder the precursor phenomena are related to the Griffiths (or Potts) transition. The Griffiths transition is a vanishing transition which occurs above the Potts transition and is present only when disorder is present, while the Potts transition which signals the effect due to frustration is always present. These results suggest that precursor phenomena in frustrated systems are due either to disorder and/or to frustration, giving a consistent interpretation also for the limiting cases of Ising spin glass and of Ising fully frustrated model, where also the Potts transition is vanishing. This interpretation could play a relevant role in glassy systems beyond the spin systems case.

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In this paper we address the problem of consistently constructing Langevin equations to describe fluctuations in nonlinear systems. Detailed balance severely restricts the choice of the random force, but we prove that this property, together with the macroscopic knowledge of the system, is not enough to determine all the properties of the random force. If the cause of the fluctuations is weakly coupled to the fluctuating variable, then the statistical properties of the random force can be completely specified. For variables odd under time reversal, microscopic reversibility and weak coupling impose symmetry relations on the variable-dependent Onsager coefficients. We then analyze the fluctuations in two cases: Brownian motion in position space and an asymmetric diode, for which the analysis based in the master equation approach is known. We find that, to the order of validity of the Langevin equation proposed here, the phenomenological theory is in agreement with the results predicted by more microscopic models

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A simple model of diffusion of innovations in a social network with upgrading costs is introduced. Agents are characterized by a single real variable, their technological level. According to local information, agents decide whether to upgrade their level or not, balancing their possible benefit with the upgrading cost. A critical point where technological avalanches display a power-law behavior is also found. This critical point is characterized by a macroscopic observable that turns out to optimize technological growth in the stationary state. Analytical results supporting our findings are found for the globally coupled case.

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In this Contribution we show that a suitably defined nonequilibrium entropy of an N-body isolated system is not a constant of the motion, in general, and its variation is bounded, the bounds determined by the thermodynamic entropy, i.e., the equilibrium entropy. We define the nonequilibrium entropy as a convex functional of the set of n-particle reduced distribution functions (n ? N) generalizing the Gibbs fine-grained entropy formula. Additionally, as a consequence of our microscopic analysis we find that this nonequilibrium entropy behaves as a free entropic oscillator. In the approach to the equilibrium regime, we find relaxation equations of the Fokker-Planck type, particularly for the one-particle distribution function.

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We study the static properties of the Little model with asymmetric couplings. We show that the thermodynamics of this model coincides with that of the Sherrington-Kirkpatrick model, and we compute the main finite-size corrections to the difference of the free energy between these two models and to some clarifying order parameters. Our results agree with numerical simulations. Numerical results are presented for the symmetric Little model, which show that the same conclusions are also valid in this case.

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We study the relaxational dynamics of the one-spin facilitated Ising model introduced by Fredrickson and Andersen. We show the existence of a critical time which separates an initial regime in which the relaxation is exponentially fast and aging is absent from a regime in which relaxation becomes slow and aging effects are present. The presence of this fast exponential process and its associated critical time is in agreement with some recent experimental results on fragile glasses.

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A study of a stable front propagating in a turbulent medium is presented. The front is generated through a reaction-diffusion equation, and the turbulent medium is statistically modeled using a Langevin equation. Numerical simulations indicate the presence of two different dynamical regimes. These regimes appear when the turbulent flow either wrinkles a still rather sharp propagating interfase or broadens it. Specific dependences of the propagating velocities on stirring intensities appropriate to each case are found and fitted when possible according to theoretically predicted laws. Different turbulent spectra are considered.

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The diffusion of passive scalars convected by turbulent flows is addressed here. A practical procedure to obtain stochastic velocity fields with well¿defined energy spectrum functions is also presented. Analytical results are derived, based on the use of stochastic differential equations, where the basic hypothesis involved refers to a rapidly decaying turbulence. These predictions are favorable compared with direct computer simulations of stochastic differential equations containing multiplicative space¿time correlated noise.

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A més de realitzar una estadística mèdica dels trastorns i perills que afecten els treballadors de dita companyia, el document reivindica la necessitat d'aquest tipus de treball per tal de posar sobre la taula els problemes presents i les solucions a buscar.

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Introducción: Hay poco conocimiento sobre la similitud de la mecánica entre la lactancia materna y la artificial. Evaluamos la mecánica de la succión en neonatos con lactancia materna exclusiva, lactancia artificial exclusiva y lactancia mixta. Nuestra hipótesis fue que el patrón fisiológico de los movimientos de succión varía según el tipo de alimentación. Según esta hipótesis, los niños con lactancia materna exclusiva realizan unos movimientos al mamar distintos a los de la succión de una tetina, realizados por niños con lactancia artificial. Los niños con lactancia mixta mezclan ambos tipos de movimientos de succión. Métodos: Estudio transversal de neonatos de 21-28 días de edad con lactancia materna o artificial exclusiva (124 parejas madre-hijo), y ensayo de campo, abierto, cruzado y aleatorizado, realizado en neonatos de 21-28 días (110 parejas madre-hijo) y en lactantes de 3-5 meses de edad (125 parejas madre-hijo) con lactancia mixta. Las variables principales fueron los movimientos de succión y las pausas. Resultados: Los neonatos de 21-28 días de edad alimentados con lactancia artificial exclusiva mostraron un menor número de movimientos de succión y el mismo número de pausas, pero de mayor duración, que los neonatos con lactancia materna exclusiva. Entre los niños que recibieron lactancia mixta, el número de movimientos de succión al recibir alimentación con biberón fue similar y las pausas menos numerosas y de menor duración respecto a lo observado al amamantar, tanto a los 21-28 días como a los 3-5 meses de edad. En este grupo de lactancia mixta, la cifra media de tomas de lactancia materna fue de 5,83 ± 1,93 a los 21-28 días de vida y de 4,42 ± 1,67 a los 3-5 meses de edad. En el análisis de equivalencia, realizado sobre los niños que recibieron lactancia mixta, el intervalo de confianza del 95% de la razón de movimientos con lactancia artificial y con lactancia materna se situó fuera del rango de equivalencia, indicó un número de movimientos de succión menor en un 5,9-8,7% al tomar el biberón, así como un menor número de pausas y una duración más breve de ellas en este mismo grupo. Conclusiones: En la lactancia mixta, la comparación entre las tomas de biberón y las de pecho se situó fuera del rango de equivalencia, aunque las diferencias fueron pequeñas. Los niños con lactancia mixta mezclan ambos tipos de movimientos (lactancia materna y lactancia artificial) durante la fase de aprendizaje y adoptan su propio patrón.

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El objetivo del presente trabajo consistió en analizar la valoración que realizan los alumnos de la asignatura Análisi de Dades en Psicologia de los diferentes materiales puestos a su disposición para el proceso de enseñanza-aprendizaje de esta materia, con el fin último de poder facilitar al alumnado el material más adecuado para el fomento de su trabajo autónomo. Para ello se administró un cuestionario elaborado ad-hoc en el que se preguntó sobre el diferente tipo de material que tenían a su disposición los alumnos matriculados en esta asignatura en el primer semestre del curso académico 2008-09; en concreto se trabajó con una muestra de 391 estudiantes. Los resultados mostraron que el material mejor evaluado fue el tradicional, es decir, el formulario de la asignatura, el dossier de problemas junto con sus soluciones y las clases, tanto las magistrales como prácticas; en tanto que el material más basado en las nuevas tecnologías fue el peor valorado (CD-Roms interactivos, páginas Web, glosario generado por los alumnos en el campus virtual de la asignatura).