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首页> 外文期刊>Journal of Hydraulic Engineering >Subelement Form-Drag Parameterization in Rough-Bed Flows
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Subelement Form-Drag Parameterization in Rough-Bed Flows

机译:粗糙流中的子元素形式-拖动参数化

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Spatial averaging of the Reynolds-averaged Navier-Stokes equations gives the double-averaged Navier-Stokes equations, for which boundary drag appears naturally and explicitly in momentum conservation equations. Increasing use of the double-averaged equations, e.g., for relating flows to three-dimensional bed roughness, for evaluation of profiles of flow stresses and velocities in ecologically significant regions below roughness tops, and for modeling purposes, requires parameterization of boundary drag at subele-ment scales. Based on seven flows over repeated square-rib roughness and ten flows over repeated fixed simulated sand waves, with measured velocities and bed pressures, expressions for form-drag coefficient C_D=f (elevation below roughness top, relative roughness submergence, roughness steepness) are obtained for each of the two-dimensional roughness types. Using these equations, form drag variation with elevation below roughness tops can be calculated using either the double average of the square of local velocity (preferred based on conceptual considerations, trends in coefficient prediction, and also overall drag prediction) or the squared local double-averaged velocity, the roughness area being normal to the flow in each case. Integration of subelement drag given by these expressions is shown to give form-drag coefficient magnitudes and trends for complete individual elements comparable to those obtained by other authors based on measurements or numerical simulations. The ranges of roughness steepness and relative roughness submergence upon which the present equations have been derived need to be noted in consideration of application of the equations. In addition, effective application of the expressions is limited in regions of strongly negative double-averaged velocity. Further work remains to determine drag parameterization for alternative roughness geometries.
机译:雷诺平均Navier-Stokes方程的空间平均给出了双平均Navier-Stokes方程,其边界阻力在动量守恒方程中自然而明确地出现。越来越多地使用双平均方程式,例如,将流量与三维床粗糙度联系起来,评估粗糙度顶下以下重要生态区域中的流动应力和速度分布图,以及出于建模目的,需要对子元素处的边界阻力进行参数化量表。根据重复的方肋粗糙度下的七次流动和固定的重复模拟砂波下的十次流动,在测得的速度和床压的情况下,形变系数C_D = f的表达式(低于粗糙度顶部的高度,相对粗糙度浸没,粗糙度陡度)为二维粗糙度类型中的每一个都获得。使用这些方程式,可以使用局部速度平方的两倍平均值(基于概念上的考虑,系数预测的趋势以及整体阻力预测的首选)或局部平方倍的平方来计算高度在粗糙度以下的形状阻力变化。平均速度,在每种情况下,粗糙度区域均垂直于流动。这些表达式给出的子元素阻力积分显示出完整的单个元素的形式阻力系数幅度和趋势,可与其他作者基于测量或数值模拟获得的结果进行比较。考虑到方程的应用,需要注意已经在其上推导出本方程的粗糙度陡度和相对粗糙度浸没的范围。另外,表达式的有效应用受到严重负双倍平均速度区域的限制。确定替代粗糙度几何形状的阻力参数化还有进一步的工作。

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