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91.
92.
Thermal conductivity, viscosity, and self-diffusion coefficient data for liquid n-alkanes are satisfactorily correlated simultaneously by a method based on the hard-sphere theory of transport properties. Universal curves are developed for the reduced transport properties *, *, and D * as a function of the reduced volume. A consistent set of equations is derived for the characteristic volume and for the parameters R , R , and R D, introduced to account for the nonsphericity and roughness of the molecules. The temperature range of the above scheme extends from 110 to 370 K, and the pressure range up to 650 MPa.  相似文献   
93.
A compact finite-difference scheme to solve one-phase Stefan problems in one dimension is described. Numerical experiments indicate that the moving interface is obtained withO(t) accuracy when 3–4 iterations per time step are used to solve the nonlinear implicit scheme. The scheme can be adapted to ADI methods in higher dimensions.  相似文献   
94.
A new method for experimental determination of the thermal diffusion factor T for binary gas mixtures with a thermal diffusion column (TDC) is developed, based on A. M. Rozen's equation of TDC. The experimental results for T are obtained in a reduced form in this approximation. An experimental reference point, determined in the same TDC with a standard gas mixture, is used for the transformation of the results for T in absolute units. The proposed method is applicable for arbitrary gas mixtures, irrespective of the mass difference of the components.  相似文献   
95.
It has been shown that the acoustic response of imperfect interfaces may be described by a quasi-static spring model. In the present paper, experimental data on the geometry of the contacts between two diffusion-bonded blocks have been used to determine the spring stiffness of such interfaces which have been correlated with experimentally determined ultrasonic reflection coefficients. The correlation between the theoretical reflection coefficient and the spring stiffness was found to be in excellent agreement with experimentally-observed values, if the disbonds are of infinitesimally small thickness. For disbonds of finite thickness, the agreement is less satisfactory. Reasons for the discrepancy in the latter case are unknown at the present time.  相似文献   
96.
In an earlier paper, Heisenberg's uncertainty principle was invoked at the melting point T m of crystalline solids to provide fundamental justification for Lindemann's melting law and to compute diffusion coefficients of several alkali halides. The uncertainty principle defines breakdown of Debye zone boundary (ZB) phonons as valid collective excitations when phonon energies and line widths due to anharmonicity become comparable at T m. Upon breakdown, random, high-frequency single-particle motion or partial decoupling of crystal ions sets in. Lifetimes of these single-particle ZB motions are determined from the minimum-uncertainty product inequality by assuming that it becomes an equality at T m for ZB phonons. The present paper addresses improved formulation of that work and extended application to ionic electrical conductivities of 18 molten alkali halides at T m. It is shown that use of the Debye model produces an approximate lower bound to the mean free time, not the unconstrained direct estimate previouslu implied. This feature is generally reflected in results for ionic conductivities and alkali halide diffusion coefficients for which comparison experimental data were found. However, in spite of this lower-bound formulation and the simple nature of the computation, the results compare favorably with experiment. A model of random single-particle harmonic motion superimposed on the lower-frequency collective motion is proposed to account for volume expansion accompanying the partial decoupling for hard-sphere ions. Experimental comparisons for 15 alkali halides show the decoupling volume change to account largely for the total volume change of melting (in the hard-sphere approximation), yielding a closer agreement with experiment than recent calculations aimed explicitly at the total volume change.Paper presented at the Tenth Symposium on Thermophysical Properties, June 20–23, 1988, Gaithersburg, Maryland, U.S.A.  相似文献   
97.
Recent accurate measurements of the self-diffusion coefficient for n-hexadecane and n-octane and of the viscosity coefficient for n-heptane, n-nonane, and n-undecane over wide pressure ranges have been used to provide a critical test of a previously described method, based on consideration of hard-sphere theory, for the correlation of transport coefficient data. It is found that changes are required to the universal curve for the reduced viscosity coefficient as a function of reduced volume and, also, to the parameters R D, R , and R which were introduced to account for effects of nonspherical molecular shape. The scheme now accounts most satisfactorily for the self-diffusion, viscosity, and thermal conductivity coefficient data for all n-alkanes from methane to hexadecane at densities greater than the critical density.  相似文献   
98.
基于人类视觉模型的各向异性扩散滤波方法   总被引:2,自引:2,他引:0       下载免费PDF全文
针对各向异性扩散模型中扩散系数的梯度阈值确定问题进行了研究,提出了一种基于人类视觉模型的各向异性扩散滤波器。首先在PM方程的基础上研究了各向异性扩散系数中梯度阈值的取值问题。根据仿生学原理,分析了韦伯比曲线,将图像根据背景亮度划分为不同的区域,分别采用不同的公式计算梯度阈值。然后讨论了改进后算法在8邻域内的离散实现问题。仿真结果表明,与传统的恒常梯度阈值扩散模型相比,改进后的算法在有效保留图像重要信息的同时对噪声的抑制效果更为理想。  相似文献   
99.
The electrochemical behaviour of LaNi3.55Mn0.4Al0.3Co0.75−xFex (x = 0, 0.15, 0.55, 0.75) intermetallic compounds has been studied and presented [C. Khaldi, H. Mathlouthi, J. Lamloumi, A. Percheron-Guégan, Int. J. Hydrogen Energy 29 (2004) 307–311; C. Khaldi, H. Mathlouthi, J. Lamloumi, A. Percheron-Guégan, J. Alloys Compd. 360 (2003) 266–271; C. Khaldi, H. Mathlouthi, J. Lamloumi, A. Percheron-Guégan, J. Alloys Compd. 384 (2004) 249–253]. It has been deduced that the LaNi3.55Mn0.4Al0.3Co0.4Fe0.35 compound has interesting electrochemical properties. In this paper we present the electrochemical study of LaNi3.55Mn0.4Al0.3Co0.4Fe0.35 compound properties compared with the parent LaNi3.55Mn0.4Al0.3Co0.75 compound. Several techniques, such as, the chronopotentiometry, the constant potential discharge (CPD), the cyclic voltammetry (CV) and the linear polarization (LP) were applied to characterize these electrochemical properties. The electrochemical discharge capacity of the LaNi3.55Mn0.4Al0.3Co0.75 alloy increases to reach 294 mAh g−1 after few cycles only (five cycles). However, the activation of the LaNi3.55Mn0.4Al0.3Co0.4Fe0.35 alloy takes more than 20 cycles to be achieved and the obtained maximum discharge capacity is 194 mAh g−1. The hydrogen diffusion coefficient DH was determined by constant potential discharge and cyclic voltammetry techniques. The obtained values of the LaNi3.55Mn0.4Al0.3Co0.75 and LaNi3.55Mn0.4Al0.3Co0.4Fe0.35 compounds are 6.29 × 10−11 and 7.62 × 10−11, and 2 × 10−8 and 7.5 × 10−8 cm2 s−1 by CPD and CV techniques, respectively. The exchange current density values, determined by a linear polarization technique, are 44 and 27 mA g−1, respectively, for LaNi3.55Mn0.4Al0.3Co0.75 and LaNi3.55Mn0.4Al0.3Co0.4Fe0.35 alloys.  相似文献   
100.
Ni-Fe-Cr-B-Si涂层超塑扩散焊接的强化效应及耐磨性   总被引:1,自引:0,他引:1  
研究了Ni-Fe-Cr-B-Si合金涂层超塑性扩散焊接及焊接后的强化效应。通过对涂层的组织结构分析、硬度及耐磨性能的测试表明,当基材(5CrMnMo钢)与涂层产生协调超塑变形时,涂层原颗粒间、涂层与基材结合界面完全焊合。超塑焊合后的涂层比高频重熔及火焰重熔涂层硬度(HV)提高100-150,耐摩擦磨损性能提高30%。指出,沉淀强化、细晶强化及晶内位错密度增加是引起涂层强化效应和提高耐磨性的主要因素。  相似文献   
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