• 제목/요약/키워드: bottom velocity

검색결과 628건 처리시간 0.025초

해저면 광각 탄성파 탐사자료를 이용한 BSR 부근의 P파 속도 분석 (P-wave Velocity Analysis Around the BSR Using Wide-angle Ocean-bottom Seismic Data)

  • 김병엽;변중무
    • 지구물리와물리탐사
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    • 제12권2호
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    • pp.173-182
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    • 2009
  • 2008년 4월, 한국지질자원연구원은 동해 울릉분지 내에 있는 가스하이드레이트 유망지역을 대상으로 OBS를 이용하여 광각 탄성파 탐사를 실시하였다. 이 탐사는 광각 탄성파 자료를 통해 가스하이드레이트 부존 심도에서의 2차원 탄성파 속도 분포를 규명하기 위한 것으로서, 탐사지역의 층서구조와 기본 속도구조 도출을 위해 64채널 스트리머를 사용한 2차원 탄성파 반사법 탐사도 동시에 수행하였다. 취득한 광각 반사파 자료는 $\tau$-p 분석을 통해 각각의 OBS가 위치한 지점에서의 1차원 구간속도를 구하고 이렇게 구한 속도모델은 최종 속도 분포를 도출하기위해 사용된 탄성파 주시 역산법을 적용하는데 있어서 빠른 수렴을 위한 초기 속도 모델로 활용하였다. 초기 층서 모델은 2차원 반사법 탐사에서 얻은 중합자료를 바탕으로 작성하였고 최상위층에서부터 하위층으로 순차적으로 모델링 및 역산을 수행하는 layer stripping 방식으로 최종 속도 모델을 도출하였다. 본 연구를 통해 탐사지역의 가스하이드레이트 존재로 인한 BSR 위아래 층의 속도 역전현상 뿐만 아니라 컬럼/침니 구조에서의 속도가 주변보다 높음을 확인할 수 있었다.

천해파와 해류에 의한 해저면 마찰력 (Bottom Friction of Surface Waves and Current Flow)

  • 유동훈;김지웅
    • 한국해안해양공학회지
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    • 제12권3호
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    • pp.130-138
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    • 2000
  • 일방향흐름에 의한 해류의 마찰력 계산을 위하여 Prandtl의 혼합길이 이론을 수심 전구간에 적용하고 난류의 세기와 수리조건에 따라 완난류와 전난류로 분류하여 마찰계수를 산정하는 개수로 마찰계수 산정방법을 제시하였다. 파랑과 해류의 합성류에 의한 해저마찰력을 계산하기 위하여 두 유속의 연직분포를 고려한 BYO 모형을 이러한 흐름특성을 반영하여 개선하였다. BYO 모형은 모든 유속의 연직분포가 해저면으로부터의 직선과 접선으로 만나는 점(Bijker point)을 도출하여 파운동 유속과 해류유속의 합성을 이 점에서 시행하여 일주기의 평균갑을 구하는 모형이다. 일방향흐름의 해류나 천해파에 의한 파운동이나 해저면 가까이 경계층흐름은 완난류, 천이난류, 전난류 등 세가지 종류로 대별된다. 그 중 완난류로 대별하여 두 경우에 대한 합성류 마찰력 산정방법을 제시하였다.

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바닥면이 움직이는 이차원 채널 내 액적의 특성 연구 (Study on Characteristics of a Droplet in Two-dimensional Channel with Moving Bottom Wall)

  • 김형락;윤현식;정해권;하만영
    • 설비공학논문집
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    • 제23권2호
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    • pp.103-110
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    • 2011
  • A two-dimensional immiscible droplet deformation phenomena on moving wall in a channel has been investigated by using lattice Boltzmann method involving two-phase model. The dependence of the deformation of the droplet with different sizes on the contact angle and the velocity of bottom wall has studied. When the bottom wall starts to move, the deformation of the droplet occurs. For the largest bottom wall velocity, eventually, the deformation of the droplet is classified into the three patterns according to the contact angle.

Design of Ship Thruster and Seabed Scouring due to Effects of Water Velocity

  • Choi, Byoung-Yeol;Lee, Sang-Gil
    • Journal of Advanced Research in Ocean Engineering
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    • 제3권3호
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    • pp.102-111
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    • 2017
  • This study considered the effects on the seabed of a harbor and quay wall from ship maneuvers in relation to the thruster jet flow and initial velocity. This study also included the engine capacity, RPM, and diameter and pitch of a ship's thruster for a required speed. The impact of a scour hole on the environment of a quay wall was investigated. Based on these results, a risk based analysis was conducted to evaluate different strategies and their consequences. There has been an increase in the loads on the bottom of a harbor during ship maneuvering. This increase is caused by the propeller loads of mooring and unmooring vessels. This indicates a greater number of arrivals and departures of vessels with larger drafts, larger thruster diameters, and larger available thruster power capacities. Another important cause could be an increase in the maneuverability of vessels from the use of bow thrusters. The increasing loads, which cause a higher jet flow above the bottom, can lead to undesirable scour holes.

전난류에서의 파마찰계수 (Wave Friction Factor far Rough Turbulent Flow)

  • 유동훈
    • 한국해안해양공학회지
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    • 제5권2호
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    • pp.51-57
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    • 1993
  • 포텐셜 이론으로 구해지는 해저면 유속은 일반적으로 난류경계층에서의 파유속과 같다고 가정한다. 해저면 가까이에서 파운동에 의한 유속분포를 해석하기 위한 최근의 이론과 수치모형에서 발견되는 실험결과와의 오차는 주로 이 가정의 문제점으로부터 연유하는 것으로 사료된다. 경계층 최상점에서의 유속에 대한 이론치와 실유속치와의 관계식을 본고에서 제의하였다. 이 관계식을 이용하여 Jonsson(1967)과 Fredsoe(1984)가 각각 개발한 기존 이론식을 수정하였으며, 수정된 이론을 이용하여 파마찰계수를 산정한 결과, 발표된 실험치들과 비교하여 상당한 향상을 얻을 수 있었다.

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선수부 선저 슬래밍 충격에 대비한 설계압력의 산출 (Computation of Design Pressure against the Bow Bottom Slamming Impact)

  • 김용직;이승철;하영록;홍사영
    • 대한조선학회논문집
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    • 제55권3호
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    • pp.187-195
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    • 2018
  • Ship's bottom slamming has been studied by many researchers for a very long time. But still some ships suffer structure damages caused by the bottom slamming impacts. This paper presents a practical computation method of the design impact pressure due to ship's bow bottom slamming. Large heave and pitch motions of a rigid hull ship are simulated by the nonlinear strip method in time domain and the relative colliding velocity between the bow bottom and the water surface is calculated using the simulated ship motions. The bottom slamming impact pressure is calculated as a product of the relative colliding velocity squared and the bottom slamming pressure coefficient that is obtained by modification of the SNAME pressure coefficients based on Ochi's slamming experiments. Not only the bottom slamming pressures but also the required bottom plate thicknesses are calculated and compared with those of the classification society rules. The comparisons show good agreements and it is confirmed that the present method is practically very useful for the bottom structure design against ship's bow bottom slamming impacts.

A finite element based approach to observe hydrodynamic pressure in reservoir adjacent to concrete gravity dam

  • Santosh Kumar, Das;Kalyan Kumar, Mandal;Arup Guha, Niyogi
    • Ocean Systems Engineering
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    • 제12권4호
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    • pp.385-402
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    • 2022
  • This paper deals with the study of hydrodynamic pressure in reservoir adjacent to the concrete gravity dam subjected to dynamic excitation. Widely famous finite element method is used to discretize the reservoir domain for modelling purpose. Pressure is considered as nodal variable following Eulerian approach. A suitable nonreflecting boundary condition is applied at truncated face of reservoir to make the infinite reservoir to finite one for saving the computational cost. Thorough studies have been done on generation of hydrodynamic pressure in reservoir with variation of different geometrical properties. Velocity profile and hydrodynamic pressure are observed due to harmonic excitation for variation of inclination angle of dam reservoir interface. Effect of bottom slope angle and inclined length of reservoir bottom on hydrodynamic pressure coefficient of reservoir are also observed. There is significant increase in hydrodynamic pressure and distinct changes in velocity profile of reservoir are noticeable for change in inclination angle of dam reservoir interface. Change of bottom slope and inclined length of reservoir bottom are also governing factor for variation of hydrodynamic pressure in reservoir subjected to dynamic excitation.

난류채널유동에서 움직이는 벽면에 대한 수치연구 (Numerical Investigation of the Moving Wall Effects in Turbulent Channel Flows)

  • 황준혁;이재화
    • 한국가시화정보학회지
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    • 제15권3호
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    • pp.27-33
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    • 2017
  • Direct numerical simulations of turbulent channel flows with moving wall conditions on the top wall are performed to examine the effects of the moving wall on the turbulent characteristics. The moving wall velocity only applied to the top wall with the opposite direction to the main flow is systematically varied to reveal the sustained-mechanism for turbulence. The turbulence statistics for the Couette-Poiseuille flow, such as mean velocity, root mean square of the velocity fluctuations, Reynolds shear stress and pre-multiplied energy spectra of the velocity fluctuations, are compared with those of canonical turbulent channel flows. The comparison suggests that although the turbulent activity on the top wall increases with increasing the Reynolds number, that on the bottom wall decreases, contrary to the previous finding for the canonical turbulent channel flows. The increase of the turbulent energy on the top wall is attributed to not only the increase of the Reynolds number but also elongation of the logarithmic layer due to increase of the wall layer on the top wall. However, because the logarithmic layer is shortened on the bottom wall due to the decrease of the wall layer, the turbulence energy on the bottom wall decreases despite of the increase of the Reynolds number.

인공어초 주변의 흐름장에 관한 수치해석 (Numerical Analysis of the Flow Field around Artificial Reefs)

  • 정칠훈;김헌태
    • 한국수산과학회지
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    • 제40권1호
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    • pp.31-38
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    • 2007
  • This study investigated the fluid force acting on an artificial reef and the scour pattern at the bottom of the artificial reef in a steady-flow field using the finite difference method (Flow-3D). The structure was tetragonal in shape, like similar objects found in nature. The numerical analysis showed that the hydrodynamic characteristics and incipient scouring pattern matched natural phenomena. The velocity distribution around the tetragon was symmetric and wake occurred inside the tetragon and behind the bottom of the tetragon. The length of the recirculation flow behind the tetragon for each velocity was about 4-5 cm and the magnitude of the recirculation flow inside the tetragon generally increased with the Reynolds' number, although it decreased slightly for Reynolds' numbers from 11,000 to 12,000. In addition, the total fluid force acting on the tetragon increased with the inflow velocity, although the increment was smaller when the velocity exceed 18 cm/sec. The incipient pattern for the scouring of sediment matched the natural phenomenon.

Vertical distribution of suspended sediment concentration - A case study in Cu Lao Dung Coastal Areas (Vietnam)

  • Tien H. Le Nguyen;Phuoc H. Vo Luong
    • Ocean Systems Engineering
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    • 제13권3호
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    • pp.313-324
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    • 2023
  • The vertical distribution of suspended sediments in the mangrove-mud coast is complicated due to the characterization of cohesive sediment properties, and the influence of hydrodynamic factors. In this study, the time-evolution of suspended sediment concentration (SSC) in water depth is simulated by a one-dimensional model. The model applies in-situ data measured in October 2014 at the outer station in Cu Lao Dung coastal areas, Soc Trang, Vietnam. In the model, parameters which have influence on vertical distribution of SSC include the settling velocity Ws and the diffusion coefficient Kz. The settling velocity depends on the cohesive sediment properties, and the diffusion coefficient depends on the wave-current dynamics. The settling velocity is determined by the settling column experiment in the laboratory, which is a constant of 1.8 × 10-4 ms-1. Two hydrodynamic conditions are simulated including a strong current condition and a strong wave condition. Both simulations show that the SSC near the bottom is much higher than ones at the surface due to higher turbulence at the bottom. At the bottom layer, the SSC is strongly influenced by the current.