首页> 外文学位 >Interaction of pressure and momentum driven flows with thin porous media: Experiments and modeling.
【24h】

Interaction of pressure and momentum driven flows with thin porous media: Experiments and modeling.

机译:压力和动量驱动的流动与薄多孔介质的相互作用:实验和建模。

获取原文
获取原文并翻译 | 示例

摘要

Flow interaction with thin porous media arise in a variety of natural and man-made settings. Examples include flow through thin grids in electronics cooling, and NOx emissions reduction by means of ammonia injection grids, pulsatile aquatic propulsion with complex trailing anatomy (e.g., jellyfish with tentacles) and microbursts from thunderstorm activity over dense vegetation, unsteady combustion in or near porous materials, pulsatile jet-drying of textiles, and pulsed jet agitation of clothing for trace contaminant sampling. Two types of interactions with thin porous media are considered: (i) forced convection or pressure-driven flows, where fluid advection is maintained by external forces, and (ii) inertial or momentum-driven flows, in which fluid motion is generated but not maintained by external forces.; Forced convection analysis through thin permeable media using a porous continuum approach requires the knowledge of porous medium permeability and form coefficients, K and C, respectively, which are defined by the Hazen-Dupuit-Darcy (HDD) equation. Their determination, however, requires the measurement of the pressure-drop per unit of porous medium length. The pressure-drop caused by fluid entering and exiting the porous medium, however, is not related to the porous medium length. Hence, for situations in which the inlet and outlet pressure-drops are not negligible, e.g., for short porous media, the definition of Kand C via the HDD equation becomes ambiguous. This aspect is investigated analytically and numerically using the flow through a restriction in circular pipe and parallel plates channels as preliminary models. Results show that inlet and outlet pressure-drop effects become increasingly important when the inlet and outlet fluid surface fraction &phis; decreases and the Reynolds number Re increases for both laminar and turbulent flow regimes. A conservative estimate of the minimum porous medium length beyond which the core pressure-drop predominates over the inlet and outlet pressure-drop is obtained by considering a least restrictive porous medium core. Finally, modified K and C are proposed and predictive equations, accurate to within 2.5%, are obtained for both channel configurations with Re ranging from 10-2 to 102 and &phis; from 6% to 95%.; When momentum driven flows interact with thin porous media, the interaction of vortices with the media's complex structure gives way to a number of phenomena of fundamental and applied interest, such as unsteady flow separation. A special case that embodies many of the key features of these flows is the interaction of a vortex ring with a permeable flat surface. Although fundamental, this complex flow configuration has never been considered. The present investigation experimentally studies the fluid mechanics of the interaction of a vortex ring impinging directly on thin permeable flat targets. The vortex ring is formed in water using a piston-cylinder mechanism and visualized using planar laser-induced fluorescence (PLIF). The rings are formed for jet Reynolds numbers of 3000 and 6000, and piston stroke-to-diameter ratios of 1.0, 3.0, and 6.0. Thin screens of similar geometry having surface opening fractions of 44, 60, 69, and 79% are targeted by the rings. The flow that emerges downstream of the screens reforms into a new, "transmitted" vortex ring. For the lower porosity targets, features that are characteristic of vortex ring impingement on walls are also observed, such as primary vortex ring rebound and reversal, flow separation, formation of secondary vortices and mixing. As the interaction proceeds, however, the primary vortex ring and secondary vortices are drawn toward the symmetry axis of the flow by fluid passing through the permeable screen. Quantitative flow measurements using digital particle image velocimetry (DPIV), indicate the transmitted vortex ring has lower velocity and less (total) kinetic energy than the incident ring. Ring trajectories and total ki
机译:与薄多孔介质的流动相互作用在各种自然和人造环境中产生。例子包括通过电子冷却中的薄格栅流动,通过氨注入格栅减少NOx排放,具有复杂尾随解剖结构的脉动水生推进(例如,带有触手的水母)以及密集植被上的雷暴活动产生的微爆,在多孔体内或附近的不稳定燃烧材料,纺织品的脉冲喷射干燥以及衣服的脉冲喷射搅动以进行微量污染物采样。考虑了与薄多孔介质的两种相互作用:(i)强制对流或压力驱动流,其中流体对流由外力维持,(ii)惯性或动量驱动流,其中产生流体运动但不产生流体运动由外力维持。使用多孔连续介质方法通过薄渗透性介质进行强制对流分析需要了解多孔介质的渗透性,并分别形成由Hazen-Dupuit-Darcy(HDD)方程定义的系数K和C。然而,其确定需要测量每单位多孔介质长度的压降。然而,由流体进入和离开多孔介质引起的压降与多孔介质的长度无关。因此,对于入口和出口压降不可忽略的情况,例如,对于短的多孔介质,通过HDD方程对Kand C的定义变得模棱两可。通过使用圆形管道和平行板通道中的限制器的流动作为初步模型,对这一方面进行了分析和数值研究。结果表明,当入口和出口流体表面分数为φ时,入口和出口的压降效应变得越来越重要。对于层流和湍流状态,雷诺数减少,雷诺数Re增加。通过考虑最小限度的多孔介质芯,可以得到最小的多孔介质长度的保守估计,在该最小范围内,芯压降将超过入口和出口压降。最后,提出了修正的K和C,并针对Re范围为10-2至102和φ的两个信道配置,获得了精确到2.5%以内的预测方程。从6%到95%。当动量驱动的流动与稀薄的多孔介质相互作用时,涡旋与介质复杂结构的相互作用会被许多基本的和实用的现象所取代,例如不稳定的流动分离。体现这些流动的许多关键特征的特例是涡流环与可渗透平面的相互作用。尽管是基本的,但从未考虑过这种复杂的流配置。本研究实验性地研究了直接撞击在薄的可渗透平面目标上的涡流环相互作用的流体力学。涡流环使用活塞缸机制在水中形成,并使用平面激光诱导荧光(PLIF)可视化。形成的环用于雷诺数为3000和6000,活塞冲程直径比为1.0、3.0和6.0。环对准表面开口率分别为44、60、69和79%的相似几何形状的薄筛。滤网下游出现的气流重新形成一个新的“透射”涡流环。对于较低的孔隙率目标,还观察到涡旋环撞击壁的特征,例如一次涡旋环回弹和反转,流动分离,二次涡旋的形成和混合。然而,随着相互作用的进行,通过流过可渗透筛网的流体,初级涡流环和次级涡流被拉向流动的对称轴。使用数字粒子图像测速仪(DPIV)进行的定量流动测量表明,所传输的涡旋环具有比入射环低的速度和更少的(总)动能。圆环轨迹和总气

著录项

  • 作者

    Naaktgeboren, Christian.;

  • 作者单位

    Southern Methodist University.;

  • 授予单位 Southern Methodist University.;
  • 学科 Engineering Mechanical.; Physics Fluid and Plasma.
  • 学位 Ph.D.
  • 年度 2007
  • 页码 184 p.
  • 总页数 184
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 机械、仪表工业 ; 等离子体物理学 ;
  • 关键词

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号