• Proceedings of the Korean Society of Coastal and Ocean Engineers Conference
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• 2008.09a
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• pp.164-167
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• 2008

• Proceedings of the Korean Society of Coastal and Ocean Engineers Conference
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• 2008.09b
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• pp.164-167
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• 2008

• Journal of Korean Society of Coastal and Ocean Engineers
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• v.13 no.2
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• pp.149-157
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• 2001

From the weakly nonlinear mild-slope wave equations introduced by Nadaoka et al.(1994, 1997), a set of weakly nonlinear wave equations for rapidly varying topography are derived by including the bottom curvature and slope-squared tenns ignored in the original equations ofNadaoka et al. To solve the linear version of extended wave equations derived in this study one-dimensional finite difference numerical model is con¬structed. The perfonnance of the model is tested for the case of wave reflection from a plane slope with various inclination. The numerical results are compared with the results calculated using other numerical models reported earlier. The comparison shows that the accuracy of the numerical model is improved significantly in comparison with that of the original equations ofNadaoka et al. by including a complete set of bottom curva1w'e and slope¬squared terms for a rapidly varying topography.

• Proceedings of the Korea Water Resources Association Conference
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• 2016.05a
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• pp.338-338
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• 2016

준설은 흙 또는 모래, 자갈을 파내는 작업을 말하는 것으로, 준설의 목적은 수로, 하천, 항만공사에서 수심의 증가 및 수심을 유지하기 위함이다(산업안전대사전, 2004). 이러한 준설은 하천의 흐름 특성 및 제반 여건 변화를 수반하기도 한다. 준설 직후 낮아진 하상으로 인하여 수위가 감소되는 경우가 있으며, 반면에 수위 저하를 동반하지 않는 경우(저수지와 연결된 준설), 준설 부근에 퇴적이 발생하며 이는 하천의 수위 상승으로 연결될 수 있다. 이러한 수위 상승은 홍수 시 제방의 월류 가능성을 높이는 등 하천의 치수 안전성에 문제를 야기할 수 있다. 본 연구에서는 준설로 인한 하천의 수위 상승에 초점을 맞추었다. 기존 연구에서는 대부분 이러한 현상분석을 위해 수치해석을 이용하였으며, HEC-6, CCHE2D, GSTARS 등의 1, 2차원 수치해석 프로그램을 이용하였다. 그러나 1, 2 차원 수치모형은 수심에 따른 흐름특성을 충분히 반영하지 못하는 한계점을 가진다. 이에 본 연구에서는 3차원 수치해석 모형인 SCHISM을 이용하였다. SCHISM은 하구역의 흐름특성을 분석하기 위해 개발된 프로그램으로, 본 연구와 같이 단면의 급 확대부의 수치해석에 적합한 프로그램이라고 판단된다. 기존연구를 바탕으로 하상변동에 영향을 주는 인자를 산정하여 무차원화 하였으며, 하상 변동량 및 수위상승 영향의 민감도 분석을 수행하였다. 무차원인자는 준설깊이/상류수심(H/hu), 하류하폭/상류하폭($W_d/W_u$), 하류수심/상류수심($h_d/h_u$), 유량(Q)으로 결정하였다. 수치해석에 이용된 지형은 1: 2 경사의 제방을 가진 직선수로이며, 준설 구간을 기준으로 상 하류 각각 1,000 m의 길이를 확보하였다. SCHISM 수치모의를 통하여 민감도 분석을 수행한 결과 모든 수치해석 case에서 퇴적으로 인한 상류수위의 증가를 확인 할 수 있었다. 또한 하류수심/상류수심은 준설부 퇴적 및 상류 수위 상승에 가장 큰 영향을 주는 인자로 나타났다. 본 연구는 하천 준설 계획 시 참고자료로 활용이 가능할 것이며, 준설로 인한 하천수리특성 변화의 선행연구로써 의미가 있다고 판단된다.

• Proceedings of the Korea Water Resources Association Conference
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• 2007.05a
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• pp.1353-1357
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• 2007

국내에서 홍수 범람과 농지침수 분석에 이용되는 FLUMEN 모형은 원형섬 주변 처오름 현상과 급변류 해석만이 검증되어 소개되었다. 따라서 FLUMEN 모형의 만곡부나 합류부 등 개수로에서 적용가능성을 파악하기 위해서 하상경사 급변화, 원형 교각 주변 흐름변화, $180^{\circ}$ 만곡부 및 $90^{\circ}$ 합류부 실험 결과와 비교 검토를 수행하였다. FLUMEN 모형은 유한 체적법을 이용한 수치 계산으로 천이구간에서 발생하는 불연속점에서도 수치 모의가 잘 이루어지며, 만곡 수로와 합류 수로에서 전체적인 수심 분포가 최대 6%미만의 오차를 보이고 있어 매우 양호한 수치 모의를 할 수 있다. 또한 임의의 기하학적 형상을 원하는 위치에 반영한 지형 격자망 생성이 가능하다. 따라서 FLUMEN은 교각 주변, 만곡부 및 합류부 흐름 특성을 비교적 정확한 모의가 가능하며, 실제 하천에 적용하기에 충분한 수치 모의 능력을 지닌 모형이라 판단된다.

• Journal of Korean Society of Coastal and Ocean Engineers
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• v.13 no.2
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• pp.122-138
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• 2001

It is well known that whcn waves propagating on a shallow water suddenly encounter a much deeper water they do not propagate further but are reflected. If we apply this phenomenon to a harbor by making the harbor depth much greater than outside, we could improve the harbor tranquillity by making the waves impinging into the harbor be reflected at the harbor entrance. In the present paper, first we apply the numerical models based' on the mild-slope equation and extended mild-slope equation to calculate the long wave resonances in a rectangular harbor with a very large depth discontinuity at its entrance to find that the difference between the models is almost negligible. By applying the numerical model to a realistic model harbor whose inside is entirely dredged, it is found that the effect of dredging is insignificant when the inside depth is twice the outside one but tripled inside depth significantly reduces the long waves of period of one to five minutes whieh may exert a bad influence on ship motion. Moreover, even when only a portion of the harbor basin is dredged, the cffect of dredging in the dredged area is found to be comparable to that of entire dredging, showing that the dredging of harbor basin can be a countenncasure for harbor resonance.

• Journal of Korean Society of Coastal and Ocean Engineers
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• v.13 no.3
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• pp.254-261
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• 2001

It is well known that when long waves propagate from deep ocean onto a continental shelf with a very steep continental slope, the waves reflected from the shore can not propagate offshore and are re-reflected from the continental slope so that large water level fluctuations are induced near the shore. Liu(1986) has analyzed this phenomenon by assuming a topography which has a depth discontinuity along a semicircular offshore boundary, but his solution is erroneous. In the present paper, we correct his analytical solutions for a straight shoreline and a rectangular harbor. The corrected solution is then compared with the numerical results of the Galerkin finite element model of Jeong et al.(1998), which is based on the extended mild-slope equation.

• Journal of Korean Society of Coastal and Ocean Engineers
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• v.15 no.3
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• pp.159-166
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• 2003

In this study, we develop a finite element model to directly solve the Laplace equation while keeping the same computational efficiency as the models based on the extended mild-slope equation which has been widely used for calculation of wave transformation in shallow water. For this, the computational domain is discretized into finite elements with a single layer in the vertical direction. The velocity potential in the element is then expressed in terms of the potentials at the nodes located at water surface, and the Galerkin method is used to construct the numerical model. A common shape function is adopted in horizontal direction, and the cosine hyperbolic function in vertical direction, which describes the vertical behavior of progressive waves. The model was developed for vertical two-dimensional problems. In order to verify the developed model, it is applied to vertical two-dimensional problems of wave reflection and transmission. It is shown that the present finite element model is comparable to the models based on extended mild-slope equations in both computational efficiency and accuracy.

• 한국해양학회지
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• v.30 no.1
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• pp.13-26
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• 1995

In this paper three turbulence models including two-equation model by Blumberg and Mellor (1987), one-equation model with mixing length formula of Blackadar's (1962), and zero-equation model of Prandtl's (1925) were compared in homogeneous, unstratified channel flows. Steady flows which a steep-sided trapezoidal trench with uniform discharge, tidal flow and steady wind-driven flow in finite channels are considered in detail. Steady flows in a trench and tidal flows in a finite channel were reproduced fairly accurately and there was virtually no difference among results of three turbulence models. However, In case of steady wind-driven flow only two-equation model reproduced the important features of experimental data. the other two models underestimated the surface velocity. In tidal and wind-driven flows with negligibly small adjective and diffusive effects, the two-equation model gives rise to parabolic profile of eddy viscosity with maximum at the mid0depth, and the one and zero equation model based on Blackadar formula linear profile with maximum at the surface.

• Proceedings of the KSME Conference
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• 2002.08a
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• pp.209-212
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• 2002

Since Berkhoff proposed the mild-slope equation in 1972, it has widely been used for calculation of shallow water wave transformation. Recently, it was extended to give an extended mild-slope equation, which includes the bottom slope squared term and bottom curvature term so as to be capable of modeling wave transformation on rapidly varying topography. These equations were derived by integrating the Laplace equation vertically. In the present study, we develop a finite element model to solve the Laplace equation directly while keeping the same computational efficiency as the mild-slope equation. This model assumes the vertical variation of wave potential as a cosine hyperbolic function as done in the derivation of the mild-slope equation, and the Galerkin method is used to discretize . The computational domain was discretized with proper finite elements, while the radiation condition at infinity was treated by introducing the concept of an infinite element. The upper boundary condition can be either free surface or a solid structure. The applicability of the developed model was verified through example analyses of two-dimensional wave reflection and transmission. .