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Molecular dynamics simulations of high-energy twist and tilt bicrystals of fcc palladium reveal a universal, liquid-like, isotropic high-temperature diffusion mechanism, characterized by a rather low self-diffusion activation energy that is independent of the boundary type or misorientation. Medium-energy grain boundaries exhibit the same behavior at the highest temperatures; however, at lower temperatures the diffusion mechanism becomes anisotropic, with a higher, misorientation-dependent activation energy. Our simulations demonstrate that the lower activation energy at elevated temperatures is caused by a structural transition, from a solid boundary structure at low temperatures to a liquid-like structure at high temperatures. We demonstrate that the existence of such a transition has important consequences for diffusion creep in nanocrystalline fcc metals. In particular, our simulations reveal that in the absence of grain growth, nanocrystalline microstructures containing only high-energy grain boundaries exhibit steady-state diffusion creep with a creep rate that agrees quantitatively with that given by the Coble-creep formula. Remarkably, the activation energy for the high-temperature creep rate is the same as that characterizing the universal high-temperature diffusion in high-energy energy bicrystalline grain boundaries. 相似文献
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We consider a system of random walks or directed polymers interacting weakly with an environment which is random in space and time. In spatial dimensionsd>2, we establish that the behavior is diffusive with probability one. The diffusion constant is not renormalized by the interaction. 相似文献
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Molecular-dynamics (MD) simulations are used, for the first time, to study grain-boundary diffusion creep of a model polycrystalline silicon microstructure. Our fully dense model microstructures, with a grain size of up to 7.5 nm, were grown by MD simulations of a melt into which small, randomly oriented crystalline seeds were inserted. In order to prevent grain growth and thus to enable steady-state diffusion creep to be observed on a time scale accessible to MD simulations (of typically 10-9s), our input microstructures were tailored to (i) have a uniform grain shape and a uniform grain size of nm dimensions and (ii) contain only high-energy grain boundaries which are known to exhibit rather fast, liquid-like self-diffusion. Our simulations reveal that under relatively high tensile stresses these microstructures, indeed, exhibit steady-state diffusion creep that is homogenous (i.e., involving no grain sliding), with a strain rate that agrees quantitatively with that given by the Coble-creep formula. 相似文献
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Summary Diffusion of MgCl2 through six different types of nuclepore membranes of polycarbonate has been studied. The change of concentration with time
was determined by a conductivitymeter on line with a microcomputer. The measurements were carried out at temperatures between
20 and 50°C at 10°C intervals and at different concentrations in the range 2·10−4÷10−1 equiv l−1. The salt permeabilityP
ms of the membrane system, formed by the membrane itself and the two adjacent layers of diffusion, is obtained through methematical
treatment of the concentrationvs. time results. We have studied the variation ofP
ms with concentration of solutions, the characteristics of the membrane and the temperature. Finally, we have estimated the
activation energy of the diffusion process by using a kinetic model of the permeation.
Riassunto Si è studiata la diffusione di MgCl2 attraverso sei diversi tipi di membrane Nuclepore di policarbonato. Il cambiamento di concentrazione nel tempo è stato determinato da un misuratore di conduttività collegato con un microcomputer. Le misurazioni sono state effettuate a temperatura tra 20 e 50°C ad intervalli di 10°C e a differenti concentrazioni nell’intervallo 2·10−4÷10−1 equiv l−1. La permeabilità al saleP ms del sistema membrana, formato dalla membrana stessa e da due strati adiacenti di diffusione è ottenuta attraverso la trattazione matematica dei risultati di concentrazionivs. il tempo. Si sono studiate la variazioneP ma con la concentrazione delle soluzioni, le caratteristiche della membrana e la temperatura. Infine si è stimata l’energia di attivazione del processo di diffusione usando un modello cinetico di permeazione.
Резюме Исследуется диффузия MgCl2 через шесть различных типов ядерных мембран из поликарбоната. Изменение концентрации со временем определяется с помощью измерения проводимости в линию с микрокомпьютером. Измерения проводятся при температурах от 20 до 50°C с интервалом 10°C и при различных концентрациях в области 2.10−4÷10−1. Проницаемость солиP ms через мембранную систему, образованную самой мембраной и двумя соседними слоями диффузии, получается с помощью математической обработки зависимости концентрации от времени. Мы исследовали изменениеP ms в зависимости от концентрации растворов, характеристик мембран и температуры. Б заключение, мы оцениваем энергию активации процесса диффузии, используя кинетическую модель проникновения.相似文献
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We study tracer diffusion in the continuous-time asymmetric random average process which is an interacting particle system on generalizing the Hammersley process. From the equations of motion for the particle-position correlations we obtain the exact tracer diffusion coefficient which is in agreement with a recent heuristic result by Krug and Garcia. 相似文献
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为了阐明相位编码光学加密算法的扩散及混淆特性,基于傅里叶变换位移定理,从分组密码设计准则出发,以双随机相位光学加密算法为研究对象,分析了采用单个随机相位模板的2 f系统的扩散和混淆特性。将单随机相位加密过程分解为2个相互关联的过程,结果表明,傅里叶变换在加密算法中引入了混淆操作,而傅里叶变换结合随机相位模板实现了扩散操作。通过数值模拟对上述理论分析进行了验证,引入信息熵来评价加密图像的统计分布特性,进一步分析了菲涅尔域及分数阶傅里叶变换域随机相位加密算法的扩散混淆特性。研究表明,单随机相位加密和双随机相位加密图像的信息熵分布为7.038和7.157,而随机振幅加密图像信息熵为4.521。因而,随机相位加密算法比随机振幅加密算法能实现对信息更好地扩散。 相似文献
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J.H. Harding 《Interface Science》2003,11(1):81-90
This article discusses grain boundary diffusion in ceramics. It gives a brief review of the experimental data available for ionic oxides and the problems of interpretation associated with it. The fundamental differences between grain boundary diffusion in metals and ceramics are noted. Calculations of the segregation of defects and impurities to grain boundaries are discussed together with methods of calculating diffusion coefficients in these boundaries. New results for alumina and chromia are presented. The problem of defining a grain boundary width is discussed with respect to new calculations on nickel oxide. 相似文献
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《Journal of Electrostatics》2014,72(6):437-440
Sessile droplets of an ionic liquid with contact angles close to 90° were subjected to an electric field E = V/w inside a capacitor with plate separation w and potential difference V. For small field induced deformations of the droplet shape the change in maximum droplet height, Δh = h(E) – h(0), was found to be virtually independent of the plate separation provided that w > 3h(0). In this regime a scaling law obtains Δh α E2r2, where r is the constant droplet radius, in agreement with the asymptotic predictions of Basaran and Scriven (J. Coll. Int. Sci. 140, 10, 1990). 相似文献
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Diffusion of particles in porous media often shows subdiffusive behavior. Here, we analyze the dynamics of particles exhibiting an orientation. The features we focus on are geometrical restrictions and the dynamical consequences of the interactions between the local surrounding structure and the particle orientation. This interaction can lead to particles getting temporarily stuck in parts of the structure. Modeling this interaction by a particular random walk dynamics on fractal structures we find that the random walk dimension is not affected while the diffusion constant shows a variety of interesting and surprising features. 相似文献
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Hassan Ebadi-Dehaghani 《Journal of Macromolecular Science: Physics》2016,55(3):310-318
Diffusion of 1,2,3-benzotriazole (BT), as one of the volatile corrosion inhibitors (VCI) for copper and steel, through several polymers was investigated using molecular dynamics simulation (MD). MD were performed by employing the COMPASS force field to estimate the diffusivity of BT through polyethylene (PE), polypropylene (PP), polyvinyl chloride (PVC), and Nylon 6 as potential hosts for anticorrosion film packaging purposes. The diffusion coefficients (D) of BT in these polymers were calculated by constructing an amorphous cell, each containing BT and one of these polymers. After constructing the cell, a molecular dynamics simulation was performed to calculate the mean square displacement of the BT molecule. Simulation results showed that BT can diffuse through PVC easier than the other polymers. Among these hosts the Nylon 6 had the lowest D value, implying that this polymer can maintain BT for a long time. The temperature dependence of diffusion through PE, as the most common VCI film, was studied and the activation energy (Qd) and pre-exponential diffusion coefficient (D0) in Arrhenius equation were calculated. 相似文献
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The evolution of the understanding of the mass transport phenomena in solids and liquids allows for the unification of phenomenological models. The central Darken problem is considered from the choice of the coordinate axes for diffusion, i.e. the definition of this mode of motion and the method of diffusion displacement is defined and measured. Euler's and Liouville theorems are used extensively in the analysis. The formula is derived for volume density conservation, i.e. the volume continuity equation. This fundamental formula defines the volume-fixed frame of reference in the multicomponent solid, gas and liquid solutions. The volume-fixed frame of reference is self-consistent with the foundations of linear irreversible thermodynamics, except that is recognises the need to add volume density to the usual list of extensive physical properties undergoing transport in every continuum. Proposed modifications are self-consistent with the literature dating back to Onsager, the experiments of Kirkendall, their interpretation by Darken and recent generalized formulations. It will be shown that the method can be used in mechano-chemistry and electro-mechano-chemistry. 相似文献
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The effect of diffusion of silver through Se thin films, on the visibility of two and multiple beam interference fringes has
been studied. For thickness measurements, Al has been found to be a suitable overcoating metallic layer as it does not diffuse
through Se. The thickness was measured by multiple beam fringes at reflection. 相似文献
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We study the deterministic diffusion coefficient of the two-dimensional periodic Lorentz gas as a function of the density of scatterers. Based on computer simulations, and by applying straightforward analytical arguments, we systematically improve the Machta–Zwanzig random walk approximation [Phys. Rev. Lett.
50:1959 (1983)] by including microscopic correlations. We furthermore, show that, on a fine scale, the diffusion coefficient is a non-trivial function of the density. On a coarse scale and for lower densities, the diffusion coefficient exhibits a Boltzmann-like behavior, whereas for very high densities it crosses over to a regime which can be understood qualitatively by the Machta–Zwanzig approximation. 相似文献
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We investigate the dynamics of the number of particles diffusing in a multiplicative medium. We show that the typical behaviour
of the growth process is different from the average. We develop a new formalism to study the average growth process and extend
it to the calculation of higher moments and finally of the probability distribution. We show that the fluctuations of the
growth process increase exponentially with time. We describe the interesting features of the distribution. 相似文献
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We solve analytically the problem of a biased random walk on a finite chain of ‘sites’ (1,2,…,N) in discrete time, with ‘myopic boundary conditions’—a walker at 1 (orN) at timen moves to 2 (orN − 1) with probability one at time (n + 1). The Markov chain has period two; there is no unique stationary distribution, and the moments of the displacement of
the walker oscillate about certain mean values asn → ∞, with amplitudes proportional to 1/N. In the continuous-time limit, the oscillating behaviour of the probability distribution disappears, but the stationary distribution
is depleted at the terminal sites owing to the boundary conditions. In the limit of continuous space as well, the problem
becomes identical to that of diffusion on a line segment with the standard reflecting boundary conditions. The first passage
time problem is also solved, and the differences between the walks with myopic and reflecting boundaries are brought out. 相似文献