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Investigation of flow structure with moat acting as a water cushion at the toe of an overflowing levee
Environmental Fluid Mechanics ( IF 2.2 ) Pub Date : 2022-04-29 , DOI: 10.1007/s10652-022-09861-6
Fakhar Muhammad Abbas , Norio Tanaka

The principle theme of this study is to introduce a novel countermeasure to reduce the energy of the overflowing floodwater by utilization of a water cushion. For this purpose, laboratory experiments including “LW” cases (levee with water cushion) and “OL” cases (only levee) were conducted to elucidate the role of a water cushion in the flow structure variation after a levee is overflowed and to reduce energy. A moat (a deep and wide trench) with varying non-dimensional length (Lm* = Lm/hL; Lm is the length of the moat where hL is the levee height) and depth (Dm* = Dm/hL; Dm is the moat depth) acting as a water cushion was provided at the toe of a levee with varied landward slopes (SL). The energy reductions in the LW and OL systems were found to be very close to each other at lower overflow water depths, while it was 25% greater in the LW system than in the OL system at higher overflow water depths. Changes in the landward slope (SL) of the levee, non-dimensional length (Lm*), and depth (Dm*) of moat significantly changed the flow structure and created six different flow structures. However, 1–6%, 1–3%, and 1–5% differences in energy reduction rate were observed by varying SL, Lm*, and Dm*, respectively, in LW cases. All flow structures contributed greatly to energy reduction, but the energy reduction rate was maximum in flow structure named as T-2. Flow structures named as T-2 and T-6 are preferable due to increased water depth inside the moat and presence of submerged hydraulic jump which can be achieved during landward slopes SL = 1:1, 1:2 and by decreasing Lm* Dm*, of moat during Landward slope SL = 1:3.



中文翻译:

溢流大堤前端护城河作为水垫的水流结构研究

本研究的主要主题是介绍一种利用水垫降低溢流洪水能量的新对策。为此,进行了包括“LW”案例(带水垫的堤坝)和“OL”案例(仅堤坝)在内的实验室实验,以阐明水垫在堤坝溢流后水流结构变化中的作用,并降低能量. 护城河(深而宽的沟渠)具有不同的无量纲长度(L m *  =  L m / h LL m是护城河的长度,其中h L是堤坝高度)和深度(D m *  =  D/小时;D m是护城河深度)作为水垫提供在具有不同向陆坡度( S L)的堤坝的脚趾处。LW 和 OL 系统中的能量减少在较低溢流水深时非常接近,而 LW 系统中的能量减少比 OL 系统在较高溢流水深度时高 25%。大堤向陆坡度 ( S L )、无量纲长度 ( L m * ) 和深度 ( D m * ) 的变化) 的护城河显着改变了流动结构,创造了六种不同的流动结构。然而,在 LW 情况下,通过改变 S L 、L m * 和 D m * 分别观察1-6 % 1-3 %1-5 %能量降低率差异。所有流动结构对能量降低的贡献都很大,但能量降低率在T-2流动结构中最大。命名为 T-2 和 T-6 的流动结构更可取,因为护城河内的水深增加,并且存在水下水力跃迁,这可以在向陆斜坡S L  = 1:1、1:2 和通过减小L m *时实现_* , 向陆坡S L  = 1:3 期间的护城河。

更新日期:2022-04-29
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