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81.
Transportation of passive scalar in inhomogeneous turbulence 总被引:3,自引:0,他引:3
Cui Guixiang Chen Yuguang Zhang Zhaoshun Xu Chunxiao L. Shao J. P. Bertoglio 《Acta Mechanica Sinica》2000,16(1):21-28
The paper studies the transportation of passive scalar in the inhomogeneous turbulence by means of large eddy simulation.
The prediction accuracy is verified by the well-known Comte-Bellot spectrum of the homogeneous turbulence. The mean transportation
properties are predicted with satisfaction and the underestimation of the thermal flux by the phenomenological models has
been disclosed. The high intermittence of the temperature fluctuations has been found in the inhomogeneous turbulence and
it is the reason for the underestimation of turbulent thermal flux by the phenomenological model.
The project supported by the National Natural Science Foundation of China (19732005), National Climbing Project and LIAMA 相似文献
82.
A. N. Terentiev H. J. Lee C. -J. Kim G. W. Hong 《Physica C: Superconductivity and its Applications》1997,290(3-4):291-296
By measuring the quality factor of the mechanical oscillator with an attached magnet we investigated the amplitude dependence of the energy loss in a permanent magnet-YBCO superconductor system. When a non-conducting ferrite magnet is used the energy loss is proportional to the amplitude to the 2.79 power. This value is close to the value of 3 expected for the hysteretic motion of flux lines from the Bean model. When a conducting magnet is used the exponent decreased to the value of 2.5. This reflects the contribution of eddy current dissipation in a conducting magnet to the overall loss. We identified a novel mechanism of ac loss in the magnet-superconductor system. According to this mechanism the eddy current in a magnet is induced by the ac field generated by the ac supercurrent in response to the motion of a magnet. This mechanism would take place in a rotary bearing if circumferential inhomogeneity of the rotor magnetization occurred. 相似文献
83.
The Large Eddy Simulation (LES) / Conditional Moment Closure (CMC) model with detailed chemistry is used for modelling spark ignition and flame propagation in a turbulent methane jet in ambient air. Two centerline and one off-axis ignition locations are simulated. We focus on predicting the flame kernel formation, flame edge propagation and stabilization. The current LES/CMC computations capture the three stages reasonably well compared to available experimental data. Regarding the formation of flame kernel, it is found that the convection dominates the propagation of its downstream edge. The simulated initial downstream and radial flame propagation compare well with OH-PLIF images from the experiment. Additionally, when the spark is deposited at off-centerline locations, the flame first propagates downstream and then back upstream from the other side of the stoichiometric iso-surface. At the leading edge location, the chemical source term is larger than others in magnitude, indicating its role in the flame propagation. The time evolution of flame edge position and the final lift-off height are compared with measurements and generally good agreement is observed. The conditional quantities at the stabilization point reflect a balance between chemistry and micro-mixing. This investigation, which focused on model validation for various stages of spark ignition of a turbulent lifted jet flame through comparison with measurements, demonstrates that turbulent edge flame propagation in non-premixed systems can be reasonably well captured by LES/CMC. 相似文献
84.
在聚变堆中,包层是真空室内的核心部件之一,它直接面对等离子体,工作环境十分恶劣。利用ANSYS 软件的矢量电磁法,计算了中国聚变工程实验堆(CFETR)包层在离子体破裂和垂直位移事件中感应的涡电流和电磁力。介绍了建模、电流源加载、边界条件的设置、求解和计算结果。这为今后包层组件结构的详细设计和优化提供了必要的参考数据和方法。 相似文献
85.
86.
The Reynolds-averaged Navier–Stokes (RANS) equations were solved along with turbulence models, namely k–ε, k–ω, Reynolds stress models (RSM), and filtered Navier–Stokes equations along with Large Eddy Simulation (LES) to study the fully-developed turbulent flows in circular pipes roughened by repeated square ribs with various spacings. Solutions of these flows were obtained using the commercial computational fluid dynamics (CFD) software Fluent. The numerical results were validated against experimental measurements and other numerical data published in literature. The performance of the turbulence models was compared and discussed. All the RANS models and LES model were observed to perform equally well in predicting the time-averaged flow statistics. However no instantaneous information can be obtained from the RANS results. Therefore, when a rough overview of the flow process in a pipe roughened by repeated ribs is needed, any one of the RANS models can be of value. On the other hand, the instantaneous as well as time-averaged flows could be studied with more insight using LES, albeit at a cost of CPU effort at least one order higher. 相似文献
87.
A new displacement modulation based dynamic indentation method is demonstrated and shown to be effective for viscoelastic
characterization of a glassy polymer. The analysis of dynamic experiments requires a complete understanding of the measuring
system’s dynamic characteristics especially the damping. Accordingly, an improved method, based on the use of a wire spring,
is developed for determining the damping characteristics. In general, damping in an indentation instrument is contributed
by two elements: the eddy current damping from the electromagnetic loading coil and the squeeze film damping from the capacitive
displacement transducer. Therefore, a method to determine the relative contribution from the different damping elements present
in the system is demonstrated and the results are compared with the calibration obtained from the wire spring method. Finally,
dynamic indentation tests are carried out on a glassy polymer to obtain the complex modulus; the values of which are compared
with those obtained from bulk dynamic mechanical analysis (DMA) tests. Storage modulus values are found to be in good agreement
with bulk data but some divergence in the case of loss modulus is observed. The calibration procedure of the measuring instrument
is critically examined in view of these observations. Overall, displacement modulation based dynamic indentation is shown
to be a promising method for viscoelastic characterization at the micron length scales.
An erratum to this article can be found at 相似文献
88.
Yan Zhang 《Journal of Computational and Applied Mathematics》2010,234(2):593-250
In this paper, we assess two kinds of subgrid finite element methods for the two-dimensional (2D) incompressible Naver-Stokes equations (NSEs). These methods introduce subgrid-scale (SGS) eddy viscosity terms which do not act on the large flow structures. The eddy viscous terms consist of the fluid flow fluctuation strain rate stress tensors. The fluctuation tensor can be calculated by a elliptic projection or a simple L2 projection (projective filter) in finite element spaces. The finite element pair P2/P1 is adopted to numerically implement analysis and computation. We give a complete error analysis based on the assumptions of some regularity conditions. On the part of numerical tests, the numerical computations for the stationary flows show that the numerical results agree with some benchmark solutions and theoretical analysis very well. Furthermore, the given SGS models are applied to the non-stationary fluid flows. 相似文献
89.
This paper presents residual‐based turbulence models for problems with moving boundaries and interfaces. The method is developed via a hierarchical application of variational multiscale ideas and the models are cast in an arbitrary Lagrangian–Eulerian (ALE) frame to accommodate the deformation of domain boundaries. An overlapping additive decomposition of velocity and pressure fields into coarse and fine scale components leads to coarse and fine scale mixed‐field problems. The problem governing fine scales is subjected to a further decomposition of the fine scale velocity into overlapping components termed as fine scales level I and level II. In turn, in the bottom‐up integration of scales, the model for level II fine scales serves to stabilize the problem governing level I fine scales, and model for level I fields yields the turbulence models. From the computational perspective, the coarse scales are represented in terms of the standard Lagrange shape functions, whereas level I and level II scales are represented via quadratic and fourth order polynomial bubbles, respectively. Because of the bubble functions approach employed in the consistently derived fine scale models, the resulting method is free of any embedded or tunable parameters. The proposed turbulence models share a common feature with the LES models in that the largest scales in the flow are numerically resolved, whereas the subgrid scales are modeled. The method is applied to flow around a plunging airfoil at Re = 40,000, and results are compared with experimental and numerical data published in the literature. Also presented are the results for the plunging airfoil at Re = 60,000 to show the robustness and range of applicability of the method. Copyright © 2013 John Wiley & Sons, Ltd. 相似文献
90.
NORA OKONG'O DOYLE D. KNIGHT GANG ZHOU 《International Journal of Computational Fluid Dynamics》2013,27(4):303-326
Large Eddy Simulation (LES) of the decay of isotropic turbulence and of channel flow has been performed using an explicit second-order unstructured grid algorithm for tetrahedral cells. The algorithm solves for cell-averaged values using the finite volume form of the unsteady compressible Jittered Navier-Stokes equations. The inviscid fluxes are obtained from Godunov's exact Riemann solver. Reconstruction of the flow variables to the left and right sides of each face is performed using least squares or Frink's method. The viscous fluxes and heat transfer are obtained by application of Gauss' theorem. LES of the decay of nearly incompressible isotropic turbulence has been performed using two models for the SGS stresses: the Monotone Integrated Large Eddy Simulation (MILES) approach, wherein the inherent numerical dissipation models the sub-grid scale (SGS) dissipation, and the Smagorinsky SGS model. The results using the MILES approach with least squares reconstruction show good agreement with incompressible experimental data. The contribution of the Smagorinsky SGS model is negligible. LES of turbulent channel flow was performed at a Reynolds number (based on channel height and bulk velocity) of 5600 and Mach number of 0.5 (at which compressibility effects are minimal) using Smagorinsky's SGS model with van Driest damping. The results show good agreement with experimental data and direct numerical simulations for incompressible channel flow. The SGS eddy viscosity is less than 10% of the molecular viscosity, and therefore the LES is effectively MILES with molecular viscosity. 相似文献