• 한국지반공학회지:지반
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• 제12권4호
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• pp.157-178
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• 1996

기존의 보강토벽체에 주로 이용되어온 steel strict등 고강도 인장보강재는 주변 뒤채움흙에 비해 상대적으로 변형이 작기 때문에, 설계검토시 과강재 자체에서 유발되는 변형의 크기에 대해서는 크게 유의할 필요가 없었다. 그러나 비교적 저강도인 섬유보강재의 경우, 한계상태에서 예상되는 섬유보강재 자체의 변형량은 주변 뒤채움흙의 소성변형 유발에 필요시 되는 변형량을 종종 초과하게 되며, 이와같은 크기의 과도한 변형량은 보강토벽체 구조체 자체의 안정성 확보 측면에서 허용할 수 없는 경우가 대부분이다. 결국 보증토벽체 구조체의 전면부 발생변위에 대한 일반적인 허용조건을 충족하기 위해서는, 극한강도 보다 훨씬 작은 크기의 강도가 섬유보강재의 경우 발휘하는 것으로 보아야 할 것이며, 따라서 최종적인 구조체 안정검토를 위해서는 보강재 자체의 예상변형량에 대한 평가가 섬유보강재의 경우 특히 중요시 된다. 보강재의 인장응력 -변형률 관계는 강보강재의 경우 선형탄성거동으로 가정할 수 있으나, 섬 유보강재의 경우에는 일반적으로 비 선형거동을 나타낸다. 본 연구에서는 쌍곡선 함수를 이용하여 섬유보강재의 비선형 거동특성을 모델링하였으며,또한 뒤채움흙 다짐으로 인한 유발응력등을 고려하기 위해 Ehrlich SE Mitchell, Duncan등이 제안한 방법을 수정하여 섬유 보강토벽체의 안정 해석법을 제시하였다. 본 안정 해석법 에서는 침투수압의 영향 및 뒤채움흙의 구속효과에 따른 섬유보강재의 부분적인 상대강성 변화 등을 고려하였으며, 이를 토대로 깊이별 각 섬유보 강재의 최대인장력 및 변형량 등의 예측이 가능하다. 본 연구에서는 제시하리라 하는 안정해석법의 적용성을 위해, paraweb polyester fibre multicord, non-woven polyester 지오텍스타일 및 knitted polyester 지오그리드 등 3가지 종류 보강재의 인장응력-변형률 관계 실험결과를 회귀분석하여 쌍곡선 함수형태로 이와같은 섬유보 강재의 비선형거동을 모델링하였다. 또한 이를 토대로 한 븐 연구 해석법의 적합성 검토를 위해, Ho & Rowe가 제시한 유한요소해석결과 및 LCPC, FHWA등에서 시행한 시험결과와 깊이별 각 섬유보강재의 최대인장력,변형량 및 지점별 변형률 등에 대해서도 비교하였다. 아울러 섬유 보강재의 상대강성, 뒤채움흙의 깊이별 구속효과의 정도, 다짐정도 및 침투수압 등이 각 섬유보강재의 변형량 및 전체적인 변형형태 등에 미치는 영향을 종합적으로 분석하였다.

• 대한조선학회논문집
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• 제33권2호
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• pp.1-12
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• 1996

본 논문에서는 갑판침입수의 유동특성을 단순화된 2차원 모델을 이용하여 고찰하였다. 기본방정식으로 천수파 모델에 기초한 보존형의 비선형 쌍곡선방정식이 도출되었고, 이를 계산하기 위한 시간영역 수치해법으로 predictor-corrector법과 2종 상류차분법을 채용한 유한차분법을 개발 적용하였다. 보아를 수반하는 몇가지 단순한 경우들에 대한 계산결과를 해석해와 비교하였으며, 본 수치해법이 갑판침입수의 유동해석에 유용한 방법임을 보였다. 갑판침입수의 유동 시뮬레이션 에들에서, 갑판침입수는 확산파의 형태로 감판상에 유입되며 갑판상의 구조물에 부딪힌 후 보아형태로 발달해 감이 보여지고 있다. 또한, 침입수 유동에 영향을 줄 수 있는 중요요소로서 갑판의 기울기, 상방향 가속도등이 다루어 졌고, 이들이 갑판 침입수의 유동에 상당한 영향을 미침을 확인하였다.

• 한국공간구조학회논문집
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• 제2권3호
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• pp.81-92
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• 2002

The objective of this paper is to help to make decision of the appropriate structural types in long span structured building due to range of span. For the intention, based on 7 forces of structural element, it is analized the relationships among 6 configurations of structural element(d/1), 25 structural types, 4 materials, and span-length known with 186 sample from 1850 to 1996. 1) bending forces: $club(1/100{\sim}1/10),\;plate(1/100{\sim}1/10),\;rahmen(steel,\;10{\sim}24m)\;simple\;beam(PC,\;10{\sim}35m)$ 2) shearing forces: $shell(1/100{\sim}1/1000)\;hyperbolic\;paraboloids(RC,25{\sim}97m)$ 3) shearing+bending forces: plate, folded $plate(RC21{\sim}59m)$ 4) compression axial forces: club, $arch(RC,\;32{\sim}65m)$ 5) compression+tension forces: shell, braced dome $shell(RC,\;40{\sim}201m),\;vault\;shell(RC,\;16{\sim}103m)$ 6) compression+tension axial forces: $rod(1/1000{\sim}1/100)$, cable(below 1/1000)+rod, coble+rod+membrane(below 1/1000), planar $truss(steel,\;31{\sim}134m),\;arch\;truss(31{\sim}135m),\;horizontal\;spaceframe(29{\sim}10\;8m),\;portal\;frame(39{\sim}55m),\;domical\;space\;truss(44{\sim}222m),\;framed\;\;membrane(45{\sim}110m),\;hybrid\;\;membrane\;(42{\sim}256m)$ 7) tension forces: cable, membrane, $suspension(60{\sim}150m),\;cable\;\;beam(40{\sim}130m),\;tensile\;membrane(42{\sim}136m),\;cable\;-slayed(25{\sim}90m),\;suspension\;membrane(24{\sim}97m),\;single\;layer\;pneumatic\;structure(45{\sim}231m),\;double\;layer\;pneumatic\;structures(30{\sim}44m)$

• Geomechanics and Engineering
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• 제4권3호
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• pp.173-190
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• 2012

With recent growing interests in the Performance-Based Seismic Design and Assessment Methodology, more realistic modeling of a structural system is deemed essential in analyzing, designing, and evaluating both newly constructed and existing buildings under seismic events. Consequently, a shallow foundation element becomes an essential constituent in the implementation of this seismic design and assessment methodology. In this paper, a contact interface fiber section element is presented for use in modeling soil-shallow foundation systems. The assumption of a rigid footing on a Winkler-based soil rests simply on the Euler-Bernoulli's hypothesis on sectional kinematics. Fiber section discretization is employed to represent the contact interface sectional response. The hyperbolic function provides an adequate means of representing the stress-deformation behavior of each soil fiber. The element is simple but efficient in representing salient features of the soil-shallow foundation system (sliding, settling, and rocking). Two experimental results from centrifuge-scale and full-scale cyclic loading tests on shallow foundations are used to illustrate the model characteristics and verify the accuracy of the model. Based on this comprehensive model validation, it is observed that the model performs quite satisfactorily. It resembles reasonably well the experimental results in terms of moment, shear, settlement, and rotation demands. The hysteretic behavior of moment-rotation responses and the rotation-settlement feature are also captured well by the model.

• 한국지반공학회:학술대회논문집
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• 한국지반공학회 2008년도 추계 학술발표회
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• pp.1404-1414
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• 2008

In the mechanistic-empirical trackbed design of railways, the resilient modulus is the key input parameter. This study focused on the resilient modulus prediction model, which is the functions of mean effective principal stress and axial strain, for three types of railroad trackbed materials such as crushed stone, weathered soil, and crushed-rock soil mixture. The model is composed with the maximum Young's modulus and nonlinear values for higher strain in parallel with dynamic shear modulus. The maximum values is modeled by model parameters, $A_E$ and the power of mean effective principal stress, $n_E$. The nonlinear portion is represented by modified hyperbolic model, with the model parameters of reference strain, ${\varepsilon}_r$ and curvature coefficient, a. To assess the performance of the prediction models proposed herein, the elastic response of a test trackbed near PyeongTaek, Korea was evaluated using a 3-D nonlinear elastic computer program (GEOTRACK) and compared with measured elastic vertical displacement during the passages of freight and passenger trains. The material types of sub-ballasts are crushed stone and weathered granite soil, respectively. The calculated vertical displacements within the sub-ballasts are within the order of 0.6mm, and agree well with measured values with the reasonable margin. The prediction models are thus concluded to work properly in the preliminary investigation.

• 한국압력기기공학회 논문집
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• 제20권1호
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• pp.56-65
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• 2024

Cast austenitic stainless steels (CASS) and austenitic stainless steel weldments with a ferrite-austenite duplex structure are widely used in nuclear power plants, incorporating ferrite phase to enhance strength, stress relief, and corrosion resistance. Thermal aging at 290-325℃ can induce embrittlement, primarily due to spinodal decomposition and G-phase precipitation in the ferrite phase. This study evaluates the effects of thermal aging by collecting and analyzing various mechanical properties, such as Charpy impact energy, ferrite microhardness, and tensile strength, from various literature sources. Different model expressions, including hyperbolic tangent and phase transformation equations, are applied to calculate activation energy (Q) of room-temperature impact energies, and the results are compared. Additionally, predictive models for Q based on material composition are evaluated, and the potential of machine learning techniques for improving prediction accuracy is explored. The study also examines the use of ferrite microhardness and tensile strength in calculating Q and assessing thermal embrittlement. The findings provide insights for developing advanced prediction models for the thermal embrittlement behavior of CASS and the weldments of austenitic steels, contributing to the safety and reliability of nuclear power plant components.

• Wind and Structures
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• 제27권1호
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• pp.11-27
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• 2018

The straight-cone steel cooling tower is a novel type of structure, which has a distinct aerodynamic distribution on the internal surface of the tower cylinder compared with conventional hyperbolic concrete cooling towers. Especially in the extreme weather conditions of strong wind and heavy rain, heavy rain also has a direct impact on aerodynamic force on the internal surface and changes the turbulence effect of pulsating wind, but existing studies mainly focus on the impact effect brought by wind-driven rain to structure surface. In addition, for the indirect air cooled cooling tower, different additional ventilation rate of shutters produces a considerable interference to air movement inside the tower and also to the action mechanism of loads. To solve the problem, a straight-cone steel cooling towerstanding 189 m high and currently being constructed is taken as the research object in this study. The algorithm for two-way coupling between wind and rain is adopted. Simulation of wind field and raindrops is performed with continuous phase and discrete phase models, respectively, under the general principles of computational fluid dynamics (CFD). Firstly, the rule of influence of 9 combinations of wind sped and rainfall intensity on flow field mechanism, the volume of wind-driven rain, additional action force of raindrops and equivalent internal pressure coefficient of the tower cylinder is analyzed. On this basis, the internal pressures of the cooling tower under the most unfavorable working condition are compared between four ventilation rates of shutters (0%, 15%, 30% and 100%). The results show that the 3D effect of equivalent internal pressure coefficient is the most significant when considering two-way coupling between wind and rain. Additional load imposed by raindrops on the internal surface of the tower accounts for an extremely small proportion of total wind load, the maximum being only 0.245%. This occurs under the combination of 20 m/s wind velocity and 200 mm/h rainfall intensity. Ventilation rate of shutters not only changes the air movement inside the tower, but also affects the accumulated amount and distribution of raindrops on the internal surface.

• 한국지반공학회논문집
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• 제21권2호
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• pp.113-120
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• 2005

수평하중을 받는 현장타설말뚝을 합리적이고 경제적으로 설계하기 위해서 가장 중요한 것은 지구조 사이의 상호작용을 이해하는 것이다. 그러나 지난 수십년 동안 수평하중을 받는 깊은 기초의 거동에 대한 많은 연구가 있었음에도 불구하고, 문제의 성격상 삼차원적이며 비대칭성으로 인하여 더해지는 지반고유의 비선형성, 불균일성, 복잡성 때문에 극한수평지지력을 공식화하기란 매우 어렵다 본 연구에서는 특정한 현장조건, 기초의 기하학적 특성(D/B비),하중조건 등에 따른 많은 설계 방법들 중에서 가장 널리 알려진 네 가지의 방법(즉, Reese, Broms, Hansen, 그리고 Davidson)에 대해서 재검토하였다. 그리고 본 연구의 밀환으로 행한 모형실험으로 얻어진 하중-변위곡선을 쌍곡선으로 변환하여 해석된 방곡선수평지지력(H$_h$)과 위의 네 가지 방법들에 의하여 예측되는 극한수평지지력(H$_u$)을 비교하였다. Reese와 Hansen의 방법에 의해 구한 H$_u$ / H$_h$비는 각각 0.966와 1.015로서 실험결과와 매우 근사한 극한수평지지력을 제시하고 있다. 반면에 Davidson의 방법에 의해 구한 H$_u$는 에 비하여 $30\%$ 가량 큰 것으로 예측하고 있으나 네 가지 방법중에서 예측 수평지지력값에 대한 C.O.V.가 가장 작다. 네 가지 방법 중 가장 단순한 Broms의 방법은 H$_u$/ H$_h$: 0.896으로서 네 방법 중에서 극한 수평지지력을 가장 작게 평가하는 것으로 나타나지만 극한수평지지력값을 예측함에 있어서 가장 작은 S.D.를 보인다. 결론적으로, 네 가지의 방법 중 그 어 것도 극한수평지지력을 정확하게 예측한다는 면에서 다른 방법보다 더 우수하다고 할 수는 없다. 또한, 계산과정이 얼마나 정교하거나 복잡한 것과는 상관없이 극한수평지지력을 예측하는데 있어서 신뢰도는 또 다론 문제인 것 같다.

• 한국광학회지
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• 제30권5호
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• pp.193-196
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• 2019

고출력 레이저 다이오드 광원의 안정적 구동을 위한 방열 관리는 필수적이며, 발열부인 활성층 근처의 열흐름에 있어 병목이 심하므로 그 부분의 열저항을 분석하고 설계에 적용하여 개선하는 것이 매우 중요하다. 띠형 발열구조를 갖는 레이저 다이오드 광원은 열전달층 두께에 따라 열저항이 지수함수적으로 급격하게 증가하다가 점점 선형적으로 포화되므로 열저항을 분석함에 있어서 오차가 큰 어려움이 있으며, 보다 정확한 열저항 모델링이 필요하여 수정된 두께의존성 모델함수를 제안하고 그 정확성을 검증하였다. 또한, 전산모사로 얻어낸 열저항의 변화경향성을 미분하여 열전달-단면적의 변화를 구하여 열병목 부위가 직관적으로 파악되게 하였고, 제안하는 모델함수의 열전달-단면적 결과와도 비교하여 분석모델의 예측 정확성을 부연 확인하였다. 고열전도 보조층을 활용하여 열저항이 개선된 구조에 대하여도 그 열전달-단면적 변화경향과 열저항 개선효과를 높은 정확도로 분석한 결과를 소개한다.

• 한국농공학회지
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• 제7권1호
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• pp.861-876
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• 1965

During my stay in the Netherlands, I have studied the following, primarily in relation to the Mokpo Yong-san project which had been studied by the NEDECO for a feasibility report. 1. Unit hydrograph at Naju There are many ways to make unit hydrograph, but I want explain here to make unit hydrograph from the- actual run of curve at Naju. A discharge curve made from one rain storm depends on rainfall intensity per houre After finriing hydrograph every two hours, we will get two-hour unit hydrograph to devide each ordinate of the two-hour hydrograph by the rainfall intensity. I have used one storm from June 24 to June 26, 1963, recording a rainfall intensity of average 9. 4 mm per hour for 12 hours. If several rain gage stations had already been established in the catchment area. above Naju prior to this storm, I could have gathered accurate data on rainfall intensity throughout the catchment area. As it was, I used I the automatic rain gage record of the Mokpo I moteorological station to determine the rainfall lntensity. In order. to develop the unit ~Ydrograph at Naju, I subtracted the basic flow from the total runoff flow. I also tried to keed the difference between the calculated discharge amount and the measured discharge less than 1O~ The discharge period. of an unit graph depends on the length of the catchment area. 2. Determination of sluice dimension Acoording to principles of design presently used in our country, a one-day storm with a frequency of 20 years must be discharged in 8 hours. These design criteria are not adequate, and several dams have washed out in the past years. The design of the spillway and sluice dimensions must be based on the maximun peak discharge flowing into the reservoir to avoid crop and structure damages. The total flow into the reservoir is the summation of flow described by the Mokpo hydrograph, the basic flow from all the catchment areas and the rainfall on the reservoir area. To calculate the amount of water discharged through the sluiceCper half hour), the average head during that interval must be known. This can be calculated from the known water level outside the sluiceCdetermined by the tide) and from an estimated water level inside the reservoir at the end of each time interval. The total amount of water discharged through the sluice can be calculated from this average head, the time interval and the cross-sectional area of' the sluice. From the inflow into the .reservoir and the outflow through the sluice gates I calculated the change in the volume of water stored in the reservoir at half-hour intervals. From the stored volume of water and the known storage capacity of the reservoir, I was able to calculate the water level in the reservoir. The Calculated water level in the reservoir must be the same as the estimated water level. Mean stand tide will be adequate to use for determining the sluice dimension because spring tide is worse case and neap tide is best condition for the I result of the calculatio 3. Tidal computation for determination of the closure curve. During the construction of a dam, whether by building up of a succession of horizontael layers or by building in from both sides, the velocity of the water flowinii through the closing gapwill increase, because of the gradual decrease in the cross sectional area of the gap. 1 calculated the . velocities in the closing gap during flood and ebb for the first mentioned method of construction until the cross-sectional area has been reduced to about 25% of the original area, the change in tidal movement within the reservoir being negligible. Up to that point, the increase of the velocity is more or less hyperbolic. During the closing of the last 25 % of the gap, less water can flow out of the reservoir. This causes a rise of the mean water level of the reservoir. The difference in hydraulic head is then no longer negligible and must be taken into account. When, during the course of construction. the submerged weir become a free weir the critical flow occurs. The critical flow is that point, during either ebb or flood, at which the velocity reaches a maximum. When the dam is raised further. the velocity decreases because of the decrease\ulcorner in the height of the water above the weir. The calculation of the currents and velocities for a stage in the closure of the final gap is done in the following manner; Using an average tide with a neglible daily quantity, I estimated the water level on the pustream side of. the dam (inner water level). I determined the current through the gap for each hour by multiplying the storage area by the increment of the rise in water level. The velocity at a given moment can be determined from the calcalated current in m3/sec, and the cross-sectional area at that moment. At the same time from the difference between inner water level and tidal level (outer water level) the velocity can be calculated with the formula $h= \frac{V^2}{2g}$ and must be equal to the velocity detertnined from the current. If there is a difference in velocity, a new estimate of the inner water level must be made and entire procedure should be repeated. When the higher water level is equal to or more than 2/3 times the difference between the lower water level and the crest of the dam, we speak of a "free weir." The flow over the weir is then dependent upon the higher water level and not on the difference between high and low water levels. When the weir is "submerged", that is, the higher water level is less than 2/3 times the difference between the lower water and the crest of the dam, the difference between the high and low levels being decisive. The free weir normally occurs first during ebb, and is due to. the fact that mean level in the estuary is higher than the mean level of . the tide in building dams with barges the maximum velocity in the closing gap may not be more than 3m/sec. As the maximum velocities are higher than this limit we must use other construction methods in closing the gap. This can be done by dump-cars from each side or by using a cable way.e or by using a cable way.