• Title/Summary/Keyword: Densimetric Froude number

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Experimental Study on Downstream Local Scour of Free-Falling Jet (자유낙하수맥 하류부에서의 세굴에 관한 실험적 연구)

  • 윤세의;이종태
    • Water for future
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    • v.28 no.4
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    • pp.147-154
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    • 1995
  • Scour characteristics of noncohesive bed materials at the downstream of free-falling jet were analyzed through hydraulic experiments. It was assumed that the downstream had no special energy dissipators. Flow characteristics of free falling jet from rectangular section were studied, and scour characteristics with and without mounds, which were generated at the downstream of the scour hole, were comparatively analyzed for various bed materials, discharges and tailwater depths. Not only the equilibrium scour depth but also the height of mound could be expressed as a function of densimetric Froude number. Densimetric Froude number had closer relationship with the equilibrium dimensionless scour depth than other dimensionless parameters. It was suggested that the mound effects should be considered at the design stage of bed protection works.

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Negative Buoyant Flow into Rectangular Ponds (수평정지수역(水平靜止水域)으로 유입(流入)되는 음부력(陰浮力)흐름)

  • Yoon, Tae Hoon;Chun, Si Young
    • KSCE Journal of Civil and Environmental Engineering Research
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    • v.7 no.4
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    • pp.51-60
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    • 1987
  • A two dimensional negatively buoyant flow from a shallow channel into rectangular ponds is analysed numerically by a finite difference scheme in a stretched coordinate system. In rectangular ponds, the confuguration of plunge flow largely depends on the densimetric Froude number, $Fr_e$, of the inflow. The velocity of front of the plunging flow increases with increasing negative buoyanty(decrease of $Fr_e$). The location of stable plunge point and maximun travel distance of plunge point are found to be a function of dimensionless time and densimetric Froude number. Large vortices develop on the both sides of negative buoyant flow or plunge flow.

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Behavior of Two Dimensional Density Flow into a Reservoir with Sloping Bottom (경사정지수역으로 유입되는 2차원 밀도류의 거동)

  • 윤태훈;전시영
    • Water for future
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    • v.20 no.3
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    • pp.237-245
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    • 1987
  • The behavior of negative buoyant flow into a reservoir with sloping bottom is analysed by numerical solution technique of the governing equations composed of continuty, momentum and constituent transport equation. The stable plunge point and maximum travel distance are found to be dependent on the bottom slope of reservoir as well as inflow densimetric Froude number, $Fr_e$. They are also related closely to a vortex formed just downstream from the plunge point and above the underflow. The plunge depth was shown to be a function of th bottom slope and $Fr_e$. The plunge depths obtained in this numerical study agree relatively well with published data and theoretical studies, and its predictive equation is derived.

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ON Salinity of Comduit Discharge from Selective Withdrawal Apparatus (선정된 배수관의 유출수 감분농도에 관한 연구)

  • 서영재;김진규
    • Water for future
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    • v.25 no.2
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    • pp.99-110
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    • 1992
  • A problem of outlet salinity from a stratified fluid with a well developed interface thickness consisting of an upper and lower layer differing slightly in density is considered. Three kinds of apparatus were used for the experimental test and salinity differences between inlet layer and outlet discharge were estimated by the functional relationship using the dimensionless values. For the critical incipient condition of withdrawal of upper layer, Densimetric Froude number is correlated by the inlet diameter and depth ratio in the tank.

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The Physical Characteristics of the flow field and the Form of Arrested Salt Wedge (정상 염수쇄기의 형상과 흐름 장의 물리적 특성)

  • 이문옥
    • 한국해양학회지
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    • v.25 no.2
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    • pp.62-73
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    • 1990
  • An experimental study is performed in order to catch the characteristics of the flow field at arrested salt wedge, using a rectangular open channel. Arrested salt wedge is generally so stable that the observations are easy, but velocities and interfacial waves are measured with the aid of visualization method, by injection of fluorescent dyes. The density interface, which is defined as the zone of maximum density variation with depth, exists in about 0.5 cm below the visual interface, and vertical density profile is quite well satisfied with Homeborn model. Interfacial layer has high turbulent intensity and its thickness decreases as the overall Richardson number increases and has magnitude of roughly 17% of upper layer. Cross-sectional velocity distribution just shows the influence of a side-wall friction and in the upper layer vertical velocity profile also becomes uniformly as Reynolds number increases, but in the lower layer it shows nearly parabolic type. Supposes that we divide salt wedge into three domains, that is, river mouth, intermediate and tip zone, entertainment coefficient is small at the intermediate zone and large at the river mouth and the tip zone. River mouth or intermediate zone has comparatively stable interface and capillary wave therefore s produced and propagated downstream. On the other hand, tip zone is very unstable, cusping ripple or bursting ripple is then produced incessantly. Arrested salt wedge form is nearly linear and has no relation to densimetric Froude number and Reynolds number.

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Thermal Effluent through Extruded Side Channel

  • Yoon, Tae-Hoon;Yook, Woon-Soo;Yi, Young-Kon
    • Korean Journal of Hydrosciences
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    • v.6
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    • pp.67-79
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    • 1995
  • The reattachment of buoyant efflluent to a shore in a crossflow is investigated experimentally. The effluent is prodeced by discharging heated water through a projected side channel into a confined crossflow of the same depth. In the projecting effluent, the size of recirculating region, which is formed by deflected thermal plume on the lee of the effluent, tends to increase, but the maximum temperature decreases in the direction of the crossflow and it has more uniform transverse spreading compared to non-projected type. The heat flux across the crossflow is found to be independent of the projceted length of the side channel under relatively high buoyancy flux on the contrary to low buoyancy flux. The reattachment of th effluent can be specified by both velocity ratio and densimetric Froude number, whereas only the velocity ratio is governing factor to the reattachment of the effluent in the case of non-projecting type.

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The Form of Saltwater Wedge and Structural Characteristics of Interfacial Layer (염수쐐기의 형상과 경계층의 구조적 특성)

  • Shin, Hyun-Ho;Lyu, Si-Wan;Kim, Young-Do;Seo, Il-Won
    • Proceedings of the Korea Water Resources Association Conference
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    • 2008.05a
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    • pp.1838-1842
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    • 2008
  • 본 연구에서는 하구 유입 하천에서 발생하는 염수쐐기의 형상 및 거동특성을 구명하기 위하여 정상상태 염수쐐기 실험을 수행하였다. 길이에 비해 상대적으로 폭이 좁은 개수로의 상류부분에는 담수를 지속적으로 공급할 수 있는 담수공급장치를 설치하였고, 정상상태의 염수쐐기를 발생시키기 위하여 염수수조 측면에 지속적으로 염수를 공급할 수 있는 염수공급수조를 설치하였다. 실험조건은 담수 방류량과 이층류의 밀도차의 영향을 고려한 밀도프루드수(densimetric Froude number)를 기준으로 선정하였다. 실험결과 각 케이스별 염수쐐기의 형상은 중앙부에서 약간의 산포된 양상을 제외하고는 거의 선형을 이루는 것으로 관찰되었다. 경계층의 형상과 두께는 이층류의 농도장을 측정하고 밀도변동성분을 고려한 표준편차를 통하여 산정하였다. 그리고 염수쐐기의 선단부에 해당하는 리차드슨수와 경계층 두께와의 비교 등을 통해서 경계층의 양상을 파악하였다.

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Temperature Structure in Regulating Ponds (조정지에서의 수온구조)

  • 윤태훈;전시영
    • Water for future
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    • v.20 no.3
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    • pp.247-252
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    • 1987
  • The negative buoyant flow into and through a regulating pond is analysed by numerical scheme. The controlling parameter of density current in the pond is found to be the inflow densimetric Froude number, $Fr_e$. Two vortices are formed and notable at the right corner and above the sunken flow in th pond. For given inflow characteristics, the required outflow temperature, the combination of dimensions of the pond and the residence time of the inflow in the pond are determined.

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The Behavior and Circulation of Density Current in a Small Reservoir (소규모 저수지에서 밀도류의 거동 및 순환)

  • Yoon, Tae Hoon;Han, Woon Woo
    • KSCE Journal of Civil and Environmental Engineering Research
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    • v.11 no.2
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    • pp.27-37
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    • 1991
  • The behavior of a negative buoyant flow flowing into a small reservoir is analysed by experiments and dimensional analysis. The nondimensional plunge point, head velocity, head travel distance and the dilution of density current are dependent on the inflow densimetric Froude number, Fre. The thickness of density current, flow pattern and density difference are different from two cases as follows; before the front of head arrive at the downstream end and after. Before the arrival, the thickness of density current is dependent on Fre and after the arrival, time and Fre. It was found that they can be expressed as power laws.

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Variation of Inflow Density Currents with Different Flood Magnitude in Daecheong Reservoir (홍수 규모별 대청호에 유입하는 하천 밀도류의 특성 변화)

  • Yoon, Sung-Wan;Chung, Se-Woong;Choi, Jung-Kyu
    • Journal of Korea Water Resources Association
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    • v.41 no.12
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    • pp.1219-1230
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    • 2008
  • Stream inflows induced by flood runoffs have a higher density than the ambient reservoir water because of a lower water temperature and elevated suspended sediment(SS) concentration. As the propagation of density currents that formed by density difference between inflow and ambient water affects reservoir water quality and ecosystem, an understanding of reservoir density current is essential for an optimization of filed monitoring, analysis and forecast of SS and nutrient transport, and their proper management and control. This study was aimed to quantify the characteristics of inflow density current including plunge depth($d_p$) and distance($X_p$), separation depth($d_s$), interflow thickness($h_i$), arrival time to dam($t_a$), reduction ratio(${\beta}$) of SS contained stream inflow for different flood magnitude in Daecheong Reservoir with a validated two-dimensional(2D) numerical model. 10 different flood scenarios corresponding to inflow densimetric Froude number($Fr_i$) range from 0.920 to 9.205 were set up based on the hydrograph obtained from June 13 to July 3, 2004. A fully developed stratification condition was assumed as an initial water temperature profile. Higher $Fr_i$(inertia-to-buoyancy ratio) resulted in a greater $d_p,\;X_p,\;d_s,\;h_i$, and faster propagation of interflow, while the effect of reservoir geometry on these characteristics was significant. The Hebbert equation that estimates $d_p$ assuming steady-state flow condition with triangular cross section substantially over-estimated the $d_p$ because it does not consider the spatial variation of reservoir geometry and water surface changes during flood events. The ${\beta}$ values between inflow and dam sites were decreased as $Fr_i$ increased, but reversed after $Fr_i$>9.0 because of turbulent mixing effect. The results provides a practical and effective prediction measures for reservoir operators to first capture the behavior of turbidity inflow.