• 대한기계학회논문집
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• 제16권6호
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• pp.1179-1194
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• 1992

본 연구에서는 이 기존의 방법들을 개선하여 비균일격자계에서도 사용할 수 있는 비선형 함수관계를 제시하며, 이 방법과 기존의 해법들을 비교할 때 실제 유동장 에서의 해의 정확도 차이, 전산비용의 경제성등은 어느정도 인지를 밝히고, 또 개선된 해법이 앞서 제시한 좀 더 복잡한 유동장에서도 성공적으로 적용 가능한지의 여부를 판단하는 것을 그 목적으로 한다.

• 한국농공학회지
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• 제16권4호
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• pp.3545-3554
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• 1974

The objective of this study was to investigate the characteristics of the evaporation rate, the plastic shrinkage and the compressive strength of concrete exposed to a rapid evaporation environment immediately after casting. Drying of concrete were conducted under a controlled chamber in which the temperature was mainfoimed at 30 ${\pm}$1$^{\circ}C$, the relative humidity 22 ${\pm}$1 percent, and the wind velocity 7 ${\pm}$1 m/sec. The compressive strength of concrete was tested after 28 days of standard curing. The results obtained are as follows: 1. The evaporation rate was the highest at the very beginning, was decreased as the drying progresses, and was kept almost constant after 6 hours. 2. The shrinkage of concrete was changed in three different rates for the concrete mixture having its slump vallue between 3.0cm and 7.5cm. 3. The plastic shrinkage was ended within 5 or 6 hours after casting, regardless of the water cement ratio. 4. The shrinkage was increased within the limit of slump values between 3.0cm and 7.5cm as the water-cement ratio was increased. 5. The evaporation was kept on even after the plastic shrinkage was ended. 6. Within the limit of good workability (slump value between 4.5cm and 7.5cm), the compressive strength of concrete was increased when the shrinkage rate was slow but it was decreased when the rate was rapid 7. From the result of this study it is recommended that (1) the water-cement ratio should be less as long as the workability of concrete is allowable; (2) the evaporation should be prevented at least for 4 hours after casting concrete.

• Restorative Dentistry and Endodontics
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• 제10권1호
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• pp.85-92
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• 1984

The aim of this study was to examine the influence of the speed of grinding and coolants on mercury vaporization during amalgam removal. Forty amalgam filled stone dies were stored at $37^{\circ}C$ and 100% relative humidity for 7 days prior to the beginning of the mercury vapor experiment and were divided into 4 different groups; In Group I; Used by high speed without coolant & evacuator during amalgam removal. In Group II; Used by high speed with coolant & evacuator during amalgam removal. In Group III; Used by low speed without coolant & evacuator during amalgam removal. In Group IV; Used by low speed with coolant & evacuator during amalgam removal. The amalgam specimens were removed in a 30-second time period and mercury vapor was collected with membrane filter at 27mm from the site of removal and 45 degree above there. Samples in Group II, IV were removed with coolant spray at a flow rate of 30 ml/min with high-velocity evacuator. Mercury vapor collected membrane filter was analysed by Atomic Absorption Spectrophotometer using cold vapor method. The results were as follows; 1. The mercury vapor levels were obtained all of the Groups. 2. The mercury vapor levels of the Group II, IV (with coolant & evacuator) were less than that of the Group I, III (without coolant & evacuator). 3. The highest mercury vapor level recorded during amalgam removal procedure was Group I (used by high speed without coolant & evacuator) and its record was $0.78{\pm}0.09\;mg/m^3$, which exceed the T.L.V. by 15 times. 4. The mercury vapor level of the Group IV (used by low speed with coolant & evacuator) was more than that of the Group II (used by high speed with coolant & evacuator), but its difference was not significant, statistically. (p > 0.05)

• 한국식품과학회지
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• 제21권2호
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• pp.212-217
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• 1989

무우 및 고구마를 열풍건조하고 건조가 진행됨에 따라 표면적 변화를 측정하여 실험치와 잘 일치하는 건조수축식과 총괄적 건조 속도식을 구하였으며, 시료의 두께, 상대습도 및 풍속을 포함한 초기 건조속도의 함수관계 식을 구하였다. 건조속도 상수와 차수는 시료의 두께와 공기의 온도에 영향을 받았으며 일정한 건조 (d=4mm, $Ta=50^{\circ}C$, RH=10%, U=0.8m/s) 하에서 얻어진 총괄적 건조속도 식과 수축식은 무우는 $dx/dt=0.112{\times}10^{-2}{\cdot}A{\cdot}:(1-x)^{0.43}$, A=Ao(-0.480x+1)이었고, 고구마는 $dx/dt=0.115{\times}10^{-2}\;A(1-x)^{0.49}$, A=Ao(-0.368x+1)이었다. 또한 초기 건조속도의 변화는 시료의 두께, 상대습도, 및 풍속에 대해 무우는 $dx/dt=0.0648\;(RH)^{-0.31}\;(d)^{-0.75}\;(U)^{0.39}$이었고, 고구마는 $dx/dt=0.0547(RH)^{-0.28}\;(d)^{-0.63}\;(U)^{0.37}$이었다.

• 한국지반환경공학회 논문집
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• 제13권4호
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• pp.93-104
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• 2012

20세기 이후 지반의 불확실성을 이해하고 합리적인 해석방법을 개발하기 위한 노력이 경주되어 안전율 개념이 사용되어 왔으나 이러한 개념은 실제 적용되고 있는 인자들이 불확실성을 지님에도 그 대표값을 사용하기 때문에 지반구조물의 상대적인 신뢰성을 측정하는데 한계가 있다. 그러나 현재까지도 불확실성을 완전히 제거할 수 있는 방법은 없으며, 그나마 국내에서 수행되고 있는 지반조사 결과는 이러한 통계적 기법을 적용하는 것조차도 불가능할 정도로 충분치 못한 경우가 대부분이다. 또한 침하량이나 압밀속도 등 압밀 특성이 압밀이력에 따라 크게 차이가 남에도 불구하고 압밀상태에 대한 정확한 규명없이 설계하는 것은 많은 문제점을 나타내게 된다. 따라서 본 논문에서는 압밀인자 중 과압밀비를 중심으로 설계의 불확실성을 줄이기 위한 노력의 일환으로 남해안 중 광양과 부산지역에서 수행된 양질의 실내시험 결과를 바탕으로 압밀상태를 평가하고, 설계정수의 불확실성을 줄이기 위한 정규성 검증이나 이상치 제거 등의 통계처리를 통해 지역별로 깊이에 따른 과압밀비 등의 특성을 제안하였다.

• 한국세라믹학회지
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• 제36권1호
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• pp.7-14
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• 1999

SHS 마이크로파를 이용하여 티타늄, 지르코니움과 보론분말을 혼합하여 TiZrB2 고용체를 합성된 분말의 분말특성과 소결체의 소결특성을 연구하였다. 합성 중 온도 profile 결과 연소온도와 연소속도는 Zr의 몰비가 증가함에 따라 증가 하였으며, Ti0.2Zr0.8B2조서에서 연소온도와 연소속도는 285$0^{\circ}C$, 14.6m/sec로 최고값을 얻었다. 190$0^{\circ}C$에서 30 MPa의 압력으로 60분간 고온가압소결한 TiZrB2고용체는 TiB2와 ZrB2로 상분리가 최고값을 얻었다. 190$0^{\circ}C$에서 30MPa의 압력으로 60분간 고압가압소결한 TiZrB2 고용체는 TiB2와 ZrB2로 상분리가 일어나 복합체가 형성되었으며, Ti0.8Zr0.2B2에서 가장 좋은 물성값을 나타내었는데 상대밀도, 꺽임강도, 파괴인성 및 경도는 각각 99%, 680MPa, 7.3MPam1/2, 2750Kg/$ extrm{mm}^2$이었다.

• Bulletin of the Korean Chemical Society
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• 제31권10호
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• pp.2841-2848
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• 2010

Quasiclassical trajectory (QCT) method has been used to investigate stereodynamics information of the reaction $O(^1D)+H_2{\rightarrow}\;OH$+H on the DK (Dobbyn and Knowles) potential energy surface (PES) at a collision energy of 23.06 kcal/mol, with the initial quantum state of reactant $H_2$ being set for v = 0 (vibration quantum number) and j = 0-5 (rotation quantum number). The PDDCSs (polarization dependent differential cross sections) and the distributions of P($\theta_r$), P($\phi_r$), P($\theta_r$, $\phi_r$) have been presented in this work. The results demonstrate that the products are both forward and backward scattered. As j increases, the backward scattering becomes weaker while the forward scattering becomes slightly stronger. The distribution of P($\theta_r$) indicates that the product rotational angular momentum j' tends to align along the direction perpendicular to the reagent relative velocity vector k, but this kind of product alignment is found to be rather insensitive to j. Furthermore, the distribution of P($\phi_r$) indicates that the rotational angular momentum vector of the OH product is preferentially oriented along the positive direction of y-axis, and such product orientation becomes stronger with increasing j.

• 한국정보통신학회:학술대회논문집
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• 한국정보통신학회 2015년도 추계학술대회
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• pp.999-1001
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• 2015

CW 도플러 레이더는 도플러 효과를 이용하여 특정한 물체의 상대 속도를 획득할 수 있다. 하지만 두 개 이상의 물체를 탐지하기 위해서는 CW 도플러 레이더에 FFT를 사용하여 주파수 영역에서 분석해야하며, 이러한 경우 주파수 영역에서는 물체의 개수와 속도를 구할 수 있지만 물체의 접근 또는 이탈 정보를 판단하기에는 어렵다는 단점이 존재한다. 본 논문에서는 두 개 이상의 물체를 탐지하기 위해 FFT를 사용할 경우 주파수 영역에서 물체의 접근 또는 이탈 정보를 효율적으로 판단하기 위한 알고리즘을 제안한다. 제안하는 알고리즘은 주파수 영역에서 실수부와 허수부로 나눈 후 각 주파수들의 진폭을 합한 값이 주파수의 좌측에 있으면 이탈, 우측에 있으면 접근으로 판단한다.

• Wind and Structures
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• 제13권6호
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• pp.557-580
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• 2010

A new inflow turbulence generation method and a combined dynamic SGS model recently developed by the authors were applied to evaluate the wind effects on 508 m high Taipei 101 Tower. Unlike the majority of the past studies on large eddy simulation (LES) of wind effects on tall buildings, the present numerical simulations were conducted for the full-scale tall building with Reynolds number greater than $10^8$. The inflow turbulent flow field was generated based on the new method called discretizing and synthesizing of random flow generation technique (DSRFG) with a prominent feature that the generated wind velocity fluctuations satisfy any target spectrum and target profiles of turbulence intensity and turbulence integral length scale. The new dynamic SGS model takes both advantages of one-equation SGS model and a dynamic production term without test-filtering operation, which is particular suitable to relative coarse grid situations and high Reynolds number flows. The results of comparative investigations with and without generation of inflow turbulence show that: (1) proper simulation of an inflow turbulent field is essential in accurate evaluation of dynamic wind loads on a tall building and the prescribed inflow turbulence characteristics can be adequately imposed on the inflow boundary by the DSRFG method; (2) the DSRFG can generate a large number of random vortex-like patterns in oncoming flow, leading to good agreements of both mean and dynamic forces with wind tunnel test results; (3) The dynamic mechanism of the adopted SGS model behaves adequately in the present LES and its integration with the DSRFG technique can provide satisfactory predictions of the wind effects on the super-tall building.

• 대한기계학회논문집B
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• 제24권5호
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• pp.632-639
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• 2000

Conjugate heat transfer from a heat generating module ($31{\times}31{\times}7mm^3$) bonded through the module support on the floor of a parallel-plate channel(20mm high, 400mm wide, and 800mm long) to mixed convective air flow(0.2${\sim}$0.9m/s) is studied experimentally. The input power to the module is changed in a range 1.0${\sim}$4.5W, the floor thickness 0.2${\sim}$5mm, and the thermal resistance of module support, Rc:=0.06, 1.03 and 82.0K/W. Thermal conductance(Uc) of the board and convective thermal conductance($U_A$) from the module were derived, and the effect of V; Rc and t on Uc was investigated. It is found that the conjugate conductance (Uc) and the conductive heat transfer ratio ($Q_B$/Q) depend on the thermal resistance of the module support, the air velocity and the board thickness. The change of the module support resistance and the board thickness helps to elucidate the relative significance of heat transfer paths through the module support, the board, and from the board surface to the air. Additional information is investigated about the dependence of the heat transfer rate on the mixed convection parameter.