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TURBULENT STRUCTURE OF WATER AND CLAY SUSPENSIONS WITH BED LOAD

机译:床荷载作用下水和粘土悬浮液的湍流结构

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摘要

The discusser wishes to congratulate the authors for their excellent paper. He would like to discuss some possible drag reduction effects. The discusser has reanalyzed the authors' data assuming quasi-uniform flows at the end of the channel. For the clear-water flow experiments (runs C-1 and C-2), the data suggest an equivalent roughness height k_s of the flume (smooth plexiglass) between 0.15 mm and 0.19 mm. With these values, it is possible to compute the clear-water friction factors f for the clay-mud-flow experiments (M-1 and M-2), and to compare these values with the mudflow friction factor f_s. It is interesting to note that the clay-mud flow (runs M-1 and M-2) exhibits smaller flow resistance f_s than the clear-water flow: i.e. f_s/f < 1 (Fig. 18). Other researchers observed similarly some drag reduction caused by the presence of suspended sediments (Table 4). Fig. 18 presents model and prototype data of friction factor reduction as a function of the mean volumetric sediment concentration C_υ. Most data were obtained with suspended sediments without depositing material. The data of Buckley (1923) must be considered with great care as the changes in friction factor due to variation in bed configuration might be important.
机译:讨论者希望对作者的出色论文表示祝贺。他想讨论一些可能的减阻效果。讨论者重新分析了作者的数据,并假设在通道末端存在准均匀流。对于清水流动实验(运行C-1和C-2),数据表明水槽(光滑的有机玻璃)的等效粗糙度高度k_s在0.15 mm和0.19 mm之间。利用这些值,可以计算出泥浆流实验(M-1和M-2)的清水摩擦系数f,并将这些值与泥流摩擦系数f_s进行比较。有趣的是,粘土-泥浆流(M-1和M-2)比清水流具有较小的流阻f_s:即f_s / f <1(图18)。其他研究人员类似地观察到由于悬浮沉积物的存在而导致的阻力减小(表4)。图18给出了摩擦系数降低与平均体积沉积物浓度C_υ的函数关系的模型和原型数据。大多数数据是在没有沉积物质的情况下使用悬浮沉积物获得的。必须非常仔细地考虑Buckley(1923)的数据,因为床构造的变化引起的摩擦系数的变化可能很重要。

著录项

  • 来源
    《Journal of Hydraulic Engineering》 |1995年第7期|p.562-563|共2页
  • 作者

    Hubert Chanson;

  • 作者单位

    Sr. Lect., Dept. of Civ. Engrg., Univ. of Queensland, Brisbane QLD 4072, Australia;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 水利工程;建筑科学;
  • 关键词

  • 入库时间 2022-08-18 00:22:56

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