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121.
扩散质进入窄浅型河道后,通常采用有限差分法求解一维对流分散方程进行水质模拟,计算相对复杂。为简化计算,提出了根据河道断面特征等水力特性,将河道划分为若干单元,忽略不灵敏因子分散项对单元间扩散质交换的影响,并引入单元均匀混合假定,提出了基于均匀混合假设的天然河道水质模拟方法,建立相应的水质数学模型。算例表明,该模型运算稳定,与有限差分法模拟精度相当,但可大大简化并节省计算工作量。 相似文献
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123.
绿柱石通道中配合物的振动光谱和辐照裂解 总被引:2,自引:1,他引:2
以四川平武富碱型绿柱石为研究对象 ,采用 IR和 L RM测试方法 ,重点对通道中氢化物和多聚合离子的配位构型、辐照裂解及热致转型进行了较深入系统的研究。研究表明 ,在该区成矿作用条件下 ,绿柱石通道中的钠离子趋向与氢离子化合反应生成 Na H氢化物 ,并占据通道中的 C2 位。在垂直 c轴方向上 ,以 3165 cm-1,3114 cm-1及 30 31cm-1伸缩振动弱吸收谱带为特征。[Fe2 ( OH) 4 ] 2 多聚合离子占据通道中的 C1位 ,以 32 34 cm-1伸缩振动锐吸收谱带为特征 (∥ c轴 )。辐照作用导致上述多聚合离子的裂解 ,并形成不稳定的 [H0 ] i心和相对稳定的 [Fe3 ] OH心。与之对应的吸收谱带分别出现在 3110 cm-1(⊥ c轴 )和 335 5cm-1(∥c轴 )处。通道中 Na H和 [Fe2 ( OH) 4 ] 2 多聚合离子的存在 ,可视为该类型绿柱石的一个重要的成因标志。 相似文献
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Georges Matheron (1930–2000) and John Tukey (1915–2000) were among the most prominent mathematical statisticians of the 20th century. Both men produced numerous important new theoretical and practical results. This personal appreciation of their work concentrates on contributions to mineral-resources research and describes their influence on my work in mineral-resource evaluation studies at the Geological Survey of Canada (1966–1983). 相似文献
126.
H.J.B. Birks 《Journal of Paleolimnology》2001,25(1):111-115
A recently discovered error in the part of the computer program WACALIB that implements maximum likelihood (ML) calibration has been discovered and corrected. The new version of WACALIB has been re-run with all the data-sets from which results based on the earlier version of WACALIB had been published. The new results suggest that ML regression and calibration perform as well or even better than weighted averaging (WA), at least when judged by the apparent root mean squared error. Further work involving cross-validation is required to evaluate more fully the relative performance of WA and ML approaches. 相似文献
127.
长江口深水航道治理工程综述 总被引:3,自引:0,他引:3
文章概要地介绍长江口深水航道治理工程的规划、勘察、设计和施工情况,对整治方案及主要岩土工程问题略作讨论。 相似文献
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The flow pattern around a cylinder, installed in a scoured channel bed, was experimentally investigated. Detailed measurements of the instantaneous 3D velocities were performed by using an Acoustic Doppler Velocity Profiler (ADVP), from which the profiles of the time-averaged velocities and turbulence stresses were obtained. It is shown that the influence of the cylinder and of the scour hole alters the approach flow; this is essentially confined to the vicinity of the cylinder and to the inside of the scour hole. The horseshoe vortex is measured as a flow reversal inside the scour hole, formed by the downward flow along the cylinder face and the reversed flow at the scour bed. 相似文献
130.
A.P. Nicholas 《地球表面变化过程与地形》2001,26(4):345-362
Results from a series of numerical simulations of two‐dimensional open‐channel flow, conducted using the computational fluid dynamics (CFD) code FLUENT, are compared with data quantifying the mean and turbulent characteristics of open‐channel flow over two contrasting gravel beds. Boundary roughness effects are represented using both the conventional wall function approach and a random elevation model that simulates the effects of supra‐grid‐scale roughness elements (e.g. particle clusters and small bedforms). Results obtained using the random elevation model are characterized by a peak in turbulent kinetic energy located well above the bed (typically at y/h = 0·1–0·3). This is consistent with the field data and in contrast to the results obtained using the wall function approach for which maximum turbulent kinetic energy levels occur at the bed. Use of the random elevation model to represent supra‐grid‐scale roughness also allows a reduction in the height of the near‐bed mesh cell and therefore offers some potential to overcome problems experienced by the wall function approach in flows characterized by high relative roughness. Despite these benefits, the results of simulations conducted using the random elevation model are sensitive to the horizontal and vertical mesh resolution. Increasing the horizontal mesh resolution results in an increase in the near‐bed velocity gradient and turbulent kinetic energy, effectively roughening the bed. Varying the vertical resolution of the mesh has little effect on simulated mean velocity profiles, but results in substantial changes to the shape of the turbulent kinetic energy profile. These findings have significant implications for the application of CFD within natural gravel‐bed channels, particularly with regard to issues of topographic data collection, roughness parameterization and the derivation of mesh‐independent solutions. Copyright © 2001 John Wiley & Sons, Ltd. 相似文献