987 resultados para MD simulation


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利用自行研制的含热传导、冲击动力学大、变形有限元程序,模拟了小尺寸梁在脉冲激光加热条件下的变形过程。在此基础上,利用商用程序模拟了冷却及残余应力的产生,研究了激光参数(强度及分布)等对于微弯曲的影响。数值模拟结果与文献中的实验观察相吻合。

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Barnacle cement is an underwater adhesive that is used for permanent settlement. Its main components are insoluble protein complexes that have not been fully studied. In present article, we chose two proteins of barnacle cement for study, 36-KD protein and Mrcp-100K protein. In order to investigate the characteristic of above two proteins, we introduced the method of molecular modeling. And the simulation package GROMACS was used to simulate the behavior of these proteins. In this article, before the simulations, we introduce some theories to predict the time scale for polymer relaxation. During the simulation, we mainly focus on two properties of these two proteins: structural stability and adhesive force to substrate. First, we simulate the structural stability of two proteins in water, and then the stability of 36-KD protein in seawater environment is investigated.We find that the stability varies in the different environments. Next, to study adhesive ability of two proteins, we simulate the process of peeling the two proteins from the substrate (graphite). Then, we analyze the main reasons of these results. We find that hydrogen bonds in proteins play an important role in the protein stability. In the process of the peeling, we use Lennard–Jones 12-6 potential to calculate the van der Waals interactions between proteins and substrate.

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基于伪随机数生成技术促生白噪声扰动,以高精度迎风/对称紧致混合差分算法求解二维/三维非定常可压Navier-Stokes方程,揭示了可压自由剪切层初始剪切过程中扰动的线性演化特征,以及该过程对扰动波数和方向的内在选择性.验证了所用算法的有效性,表明线性理论同数值模拟相结合是可压剪切层研究的合理途径之一.

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An algebraic unified second-order moment (AUSM) turbulence-chemistry model of char combustion is introduced in this paper, to calculate the effect of particle temperature fluctuation on char combustion. The AUSM model is used to simulate gas-particle flows, in coal combustion in a pulverized coal combustor, together with a full two-fluid model for reacting gas-particle flows and coal combustion, including the sub-models as the k-epsilon-k(p) two-phase turbulence niodel, the EBU-Arrhenius volatile and CO combustion model, and the six-flux radiation model. A new method for calculating particle mass flow rate is also used in this model to correct particle outflow rate and mass flow rate for inside sections, which can obey the principle of mass conservation for the particle phase and can also speed up the iterating convergence of the computation procedure effectively. The simulation results indicate that, the AUSM char combustion model is more preferable to the old char combustion model, since the later totally eliminate the influence of particle temperature fluctuation on char combustion rate.

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The sensor scheduling problem can be formulated as a controlled hidden Markov model and this paper solves the problem when the state, observation and action spaces are continuous. This general case is important as it is the natural framework for many applications. The aim is to minimise the variance of the estimation error of the hidden state w.r.t. the action sequence. We present a novel simulation-based method that uses a stochastic gradient algorithm to find optimal actions. © 2007 Elsevier Ltd. All rights reserved.

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This paper performed a numerical simulation on temperature field evolution for the surface layer of a metallic alloy subjected to pulsed Nd:YAG laser treatment. The enthalpy method was adopted to solve the moving boundary problem, I.e. Stefan problem. Computational results were obtained to show the temperature field evolution. Effects of latent heat and mushy zone width on the temperature field were investigated. The results also show very high values of temperature gradient and cooling rate, which are typical characteristics during the solidification process.

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A rectangular structural unit cell of a-Al2O3 is generated from its hexagonal one. For the rectangular structural crystal with a simple interatomic potential [Matsui, Mineral Mag. 58A, 571 (1994)], the relations of lattice constants to homogeneous pressure and temperature are calculated by using Monte-Carlo method at temperature 298K and 0 GPa, respectively. Both numerical results agree with experimental ones fairly well. By comparing pair distribution function, the crystal structure of a-Al2O3 has no phase transition in the range of systematic parameters. Based on the potential model, pressure dependence of isothermal bulk moduli is predicted. Under variation of general strains, which include of external and internal strains, elastic constants of a-Al2O3 in the different homogeneous load are determined. Along with increase of pressure, axial elastic constants increase appreciably, but nonaxial elastic constants are slowly changed.

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For understanding the correctness of simulations the behaviour of numerical solutions is analysed, Tn order to improve the accuracy of solutions three methods are presented. The method with GVC (group velocity control) is used to simulate coherent structures in compressible mixing layers. The effect of initial conditions for the mixing layer with convective Mach number 0.8 on coherent structures is discussed. For the given initial conditions two types of coherent structures in the mixing layer are obtained.

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A new method to study collapsing process of fluidized bed was proposed. The method is based on the analysis of the pressure variation during collapse. A model is proposed to describe the pressure variation on any location of the bed during collapse. Three kind of particles were fluidized by air and the pressure variation after shutting down the gas supply was measured by pressure transducers and simulated by the proposed model. The simulated results were in good agreement with the experimental data. The parameters of the fluidized bed, such as bubble fraction alpha(b), particle fraction in dense phase alpha(p), bubble velocity u(b) and slip velocity of particle u(i), can be estimated from the measured pressure data by using the proposed model. The model was also used to calculate the pressure variation in pulsed fluidized beds with low frequency.

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In this paper, TASCflow3D is used to solve inner and outer 3D viscous incompressible turbulent flow (R-e = 5.6 X 10(6)) around axisymmetric body with duct. The governing equation is a RANS equation with standard k-epsilon turbulence model. The discrete method used is a finite volume method based on the finite element approach. In this method, the description of geometry is very flexible and at the same time important conservative properties are retained. The multi-block and algebraic multi-grid techniques are used for the convergence acceleration. Agreement between experimental results and calculation is good. It indicates that this novel approach can be used to simulate complex flow such as the interaction between rotor and stator or propulsion systems containing tip clearance and cavitation.

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Rarefied gas flows through micro-channels are simulated using particle approaches, named as the information preservation (IP) method and the direct simulation Monte Carlo (DSMC) method. In simulating the low speed flows in long micro-channels the DSMC method encounters the problem of large sample size demand and the difficulty of regulating boundary conditions at the inlet and outlet. Some important computational issues in the calculation of long micro-channel flows by using the IP method, such as the use the conservative form of the mass conservation equation to guarantee the adjustment of the inlet and outlet boundary conditions and the super-relaxation scheme to accelerate the convergence process, are addressed. Stream-wise pressure distributions and mass fluxes through micro-channels given by the IP method agree well with experimental data measured in long micro-channels by Pong et al. (with a height to length ratio of 1.2:3000), Shih et al. (l.2:4800), Arkilic et al. and Arkilic (l.3:7500), respectively. The famous Knudsen minimum of normalized mass flux is observed in IP and DSMC calculations of a short micro-channel over the entire flow regime from continuum to free molecular, whereas the slip Navier-Stokes solution fails to predict it.

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El presente estudio se realizó en el laboratorio de cultivo de tejidos de la Universidad Nacional Agraria de abril del 2007 a marzo del 2008, con el objetivo de mejorar la eficiencia de producción de piña (Ananas comosus (L.) Merr.) en diferentes fases de la micropropagación. En establecimiento, enraizamiento y aclimatización se evaluaron medios de cultivos con difere ntes concentraciones de reguladores de crecimiento. En la multiplicación se estudió el tipo de consistencia del medio, frasco y número de explantes por frasco. En la fase de establecimiento los medios de cultivo que contenían las sales de Murashige y Skoog, (1962) con 1 mg/l BAP y 0.1 mg/l AIA ó ANA favorecieron la separación de los primordios de hojas; el color verde se presentó en los medios con ANA y BAP. En la fase de multiplicación los mejores medios de cultivo contenían 2 y 3 mg/l BAP de consistencia líquida, con brotes de 0.96 y 1.20. Los medios de cultivo que contenían las sales MS de consistencia semi sólida fueron superiores en número de hojas y raíces. La formación de brotes fue superior al usar frascos de 220 ml con 8 ex plantes en medio semisólido con un promedio de 3.43. La longitud de planta y el número de hojas presentaron promedios superiores en medio semisólido con 5 explantes y en frascos de 220 m l y 430 ml, respectivamente. La inducción de raíces fue favorecida en los medios de cultivo que contenían 1 mg/l de BAP con 40 g/l de sacarosa. Para la variable número de brotes, hojas y longitud de planta no hubo diferencia significativa entre los tratamientos. Las vitroplantas provenientes de plantas enteras presentaron 100% de sobrevivencia. El promedio de espinas fue más acentuado en los tratamientos de plantas partidas longitudinalmente. El número de hoja resultó similar estadísticamente en los medios con diferentes niveles de sacarosa en combinación con 0.1 y 1 mg/l de AIA. La longitud de planta obtuvo el mejor promedio en el medio que contenía 0.5 mg/l de AIA con 30 g/l de sacarosa.

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La piña es reconocida como una de las frutas más finas de las re giones tropicales y se denomina la reina de todas las frutas. En Nicaragua se consume principalmente como frut a fresca, refresco y otros productos derivados de la industrialización de la piña. Para el estudio de embriogénesis somática en piña cultivar MD - 2 se realizaron diferentes variantes de medios de cultivo en las fases de inducción, multiplicación, formación de plantas , enraizamiento y aclimatación de plantas. En la fase de inducción de callo s con el empleo de explante s de hojas no se produjo iniciación de callos, pero con explantes de ápices meristemáticos se obtuvieron los mejores resultados en los medios qu e contenían 1 mg/l de 2,4 - D y 0 y 0.2 mg/l 6 - B encil - amino - purina . La multiplicación de callos fue mejor en los medios de cultivos que se le suministraron 2 mg/l de Ácido Indolacético y 1.8 mg/l de A cido - naftaleno - acético con agua de coco al 1 5% y 400 mg/ l de carbón activado . La formaci ón de pla n tas se favoreció en el medio de cultivo que contenía 0.38 mg/l de Ácido Indolbutírico y dos mg/l de 6 - Bencil - Amino - Purina. En l a fase de enraizamiento de las plantas resultó ser mejor el medio de cultivo que con tenía 0.5 mg/l de Ácido Indolacé tico y 40 g/l de sacarosa . En la fase de aclimat iz ación de plantas los medios que previamente se desarrollaron en las cinco variantes de medios en la fase de en raizamiento presentaron los mejores resultados con respecto al po rcen taje de sobrevivencia.