• 감성과학
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• 제8권4호
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• pp.385-391
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• 2005

화장품을 바를 때 피부와 손가락 사이에서 일어나는 마찰계수는 화장품의 주관적 평가에 많은 영향을 주는 요소이다. in-vivo상태에서 피부와 접촉자 간의 마찰계수는 접촉자의 모양이나 거칠기의 정도 그리고 누르는 하중에 따라 변할 수 있다. 본 실험에서는 리니어 모터와 다축 로드셀을 이용하여 여러 가지 접촉자를 in-vivo상태에서 직접 피부에 접촉시키고 실시간으로 마찰계수를 측정할 수 있는 장치를 개발하였다. 이 장치를 이용하여 피부와 접촉자 간의 마찰계수를 측정하고 그 데이터를 화장품을 바를 때의 전후와 비교$\cdot$분석하였다. 또한 화장품을 바를 때 주관적인 평가에서 이용되는 형용사를 조사하며 마찰계수와의 그 상관관계를 분석하였다. 그 결과, 피부와 접촉자 간의 마찰계수는 화장품의 종류와 접촉자의 성질에 따라 0.17-1.2사이에서 나타나며, 주관적인 평가 또한 화장품을 바른 후 시간의 경과함에 따라 변하며, 그것은 마찰계수와 관련이 있음을 확인할 수 있었다.

• 한국대기환경학회지
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• 제19권3호
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• pp.285-296
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• 2003

The measurement of the radiation energy, trunk temperature, leaf area index (LAI), air temperature, vapor pres-sure, and precipitation has been conducted under a mixed forest at Kwangneung Arboretum during the period of 2001. Characteristics of the diurnal and seasonal variation of the radiative energy were investigated. The aerodynamic roughness length was determined as about 1.6 m and the mean albedo was about 0.1 The downward short-wave radiation was linearly correlated with the net radiation and its correlation coefficient was about 0.96. From this linear relation, the heating coefficient was calculated and its annual mean value was about 0.21 The albedo and heating coefficient was varied with season, surface characteristics, and meteorological conditions. The diurnal and seasonal variations of radiation energy were discussed in terms of the surface characteristics and meteorological conditions. In the daytime, during clear skies, net radiation was dominated by the shortwave radiation. In presence of clouds and fog, the radiation energy was diminished. At night, the net radiation was entirely dominated due to the net longwave radiation. There was no distinct diurnal variation in net radiation flux during the overcast or rainy days. The net radiation was strongest in spring and weakest in winter. The seasonal development in leaf area was also reflected in a strong seasonal pattern of the radiation energy balance. The timing, duration, and maximum leaf area and trunk temperature were found to be an important control on radiation energy budget. The trunk temperature was either equal or warmer than air temperature during most of the growing season because the canopy could absorb a substantial amount of sunlight. After autumn (after the middle of October), the trunk temperature was consistently cooler than air temperature.

• International Journal of Air-Conditioning and Refrigeration
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• 제13권1호
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• pp.51-60
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• 2005

This paper reviews the studies on the pressure drop and the heat transfer in microchannels. Although a lot of studies about the single-phase flow have been done until now, conflicting results are occasionally reported about flow transition from laminar flow to turbulent flow, friction factor, and Nusselt number. Some studies reported the early flow transition due to relatively greater wall effect like surface roughness, but the other studies showed that the flow transition occurred at the Reynolds number of about 2300 and the early flow transition might be due to less accurate measurement of the channel geometry. Also, there have been arguments whether the conventional relation based upon continuum theory can be applied to the fluid flow and the heat transfer in microchannels without modification or not. The studies about the two-phase flow in microchannels have been mostly about investigating the flow pattern and the pressure drop in rectangular channels using two-component, two-phase flow like air/water mixture. Some studies proposed correlations to predict two-phase flow pressure drop in microchannels. They were mostly based on Lockhart-Martinelli model with modification on C-coefficient, which was dependent on channel geometry, Reynolds number, surface tension, and so on. Others investigated the characteristics of flow boiling heat transfer in microchannels with respect to test parameters such as mass flux, heat flux, system pressure, and so on. The existing studies have not been fully satisfactory in providing consistent results about the pressure drop and the heat transfer in microchannels. Therefore, more in-depth studies should be done for understanding the fundamentals of the transport phenomena in the microchannels and giving the basic guidelines to design the micro devices.

• Ocean Science Journal
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• 제40권1호
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• pp.25-44
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• 2005

Long-term, continuous, and real-time ocean monitoring has been undertaken in order to evaluate various oceanographic phenomena and processes in the East/Japan Sea. Recent technical advances combined with our concerted efforts have allowed us to establish a real-time monitoring system and to accumulate considerable knowledge on what has been taking place in water properties, current systems, and circulation in the East Sea. We have obtained information on volume transport across the Korea Strait through cable voltage measurements and continuous temperature and salinity profile data from ARGO floats placed throughout entire East Sea since 1997. These ARGO float data have been utilized to estimate deep current, inertial kinetic energy, and changes in water mass, especially in the northern East Sea. We have also developed the East Sea Real-time Ocean Buoy (ESROB) in coastal regions and made continual improvements till it has evolved into the most up-to-date and effective monitoring system as a result of remarkable technical progress in data communication systems. Atmospheric and oceanic measurements by ESROB have contributed to the recognition of coastal wind variability, current fluctuations, and internal waves near and off the eastern coast of Korea. Long-tenn current meter moorings have been in operation since 1996 between Ulleungdo and Dokdo to monitor the interbasin deep water exchanges between the Japanese and Ulleung Basins. In addition, remotely sensed satellite data could facilitate the investigation of atmospheric and oceanic surface conditions such as sea surface temperature (SST), sea surface height, near-surface winds, oceanic color, surface roughness, and so on. These satellite data revealed surface frontal structures with a fairly good spatial resolution, seasonal cycle of SST, atmospheric wind forcing, geostrophic current anomalies, and biogeochemical processes associated with physical forcing and processes. Since the East Sea has been recognized as a natural laboratory for global oceanic changes and a clue to abrupt climate change, we aim at constructing a 4-D continuous real-time monitoring system, over a decade at least, using the most advanced techniques to understand a variety of oceanic processes in the East Sea.

• 대한치과보철학회지
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• 제44권5호
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• pp.594-605
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• 2006

Statement of problem: Modification of titanium implant surface has potential to ensure clinically favorable performance that several surface modification technologies have been introduced. Among the methods. anodizing method and sol-gel hydroxyapatite coating method have gained much interest due to its roughness and chemical composition of the coating layer, but more of its biocompatibility result is required. Purpose : The purpose of this study was to compare bone-implant interface shear strength of four different surface treated implants as time elapsed. Resonance frequency analysis(RFA) and removal torque measurement methods were employed to measure implant stability at one week and six week after implantation. Material and method: A total of 80 screw-shaped implant [20 machined, 20 resorbable media blasted(RBM), 20 anodized, and 20 anodized+hydroxyapatite sol-gel coated] were prepared, and one of each group was implanted in the tibia of a New Zealand white rabbit that total 20 of them were used. In order to test the implant stability and implant-tissue interface contact changing in the bone bed, each 10 rabbit were sacrificed 1 week and 6 week later while resonance frequency and removal torque were measured. One-way analysis of variance and the Tukey test were used for statistical analysis. Results : The results were as follows. 1. There was no statistically significant difference of implant stability quotients(ISQ) value in RFA between individual groups after 1 week of implantation and 6 weeks(p>0.05). But, there was statistically significant increase of ISQ value in 6 weeks group compared to 1 week group(p<0.05). 2. There was no statistically significant difference in removal torque analysis between individual groups after 1 week of implantation and 6 weeks(p>0.05). but there was statistically significant increase in all 4 groups after 6 weeks compared to 1 week later(p<0.05). 3. There was no statistically significant difference in removal torque analysis between anodized group and HA coating after anodic oxidation 6 weeks later(p>0.05), but significant difference was appeared in both groups compared to RBM group and smooth-machined group(p<0.05). Conclusions : It can be suggested that changes in surface characteristics affect bone reactions. Anodized and anodized+hydroxyapatite sol-gel coating showed significantly improved bone tissue response to implants, but further study on the effect of hydroxyapatite dissolution is needed.

• 한국표면공학회:학술대회논문집
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• 한국표면공학회 2003년도 추계학술발표회초록집
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• pp.134-135
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• 2003

The dental implant materials required good mechanical properties, such as fatigue strength, combined with a high resistance to corrosion. For increasing fatigue resistance and delaying onset of stress corrosion cracking, shot peening has been used for > 50 years to extend service life of metal components. However, there is no information on the electrochemical behavior of shot peened and hydroxyapatite(HA) coated Ti-6Al-4V alloys. To increase fatigue strength, good corrosion resistance, and biocompatibility, the electrochemical characteristics of Ti/TiN/HA coated and shot peened Ti-6Al-4V alloys by electron beam physical vapor deposition(EB-PVD) have been researched by various electrochemical method in 0.9%NaCl. Ti-6Al-4V alloys were prepared under the condition of hydrogen and vacuum arc furnace. The produced materials were quenched at 1000$^{\circ}C$ under high purity dried Ar atmosphere and were hold at 500$^{\circ}C$ for 2 hrs to achieve the fatigue strength(1140㎫) of materials. Ti-6Al-4V alloys were prepared under the condition of hydrogen and vacuum arc furnace. Shot peening(SP) and sand blasting treatment was carried out for 1, 5, and 10min. On the surface of Ti-6Al-4V alloys using the steel balls of 0.5mm and alumina sand of 40$\mu\textrm{m}$ size. Ti/TiN/HA multilayer coatings were carried out by using electron-beam deposition method(EB-PVD) as shown Fig. 1. Bulk Ti, powder TiN and hydroxyapatite were used as the source of the deposition materials. Electrons were accelerated by high voltage of 4.2kV with 80 - 120mA on the deposition materials at 350$^{\circ}C$ in 2.0 X 10-6 torr vacuum. Ti/TiN/HA multilayer coated surfaces and layers were investigated by SEM and XRD. A saturated calomel electrode as a reference electrode, and high density carbon electrode as a counter electrode, were set according to ASTM GS-87. The potentials were controlled at a scan rate of 100 mV/min. by a potentiostat (EG&G Co.273A) connected to a computer system. Electrochemical tests were used to investigate the electrochemical characteristics of Ti/TiN/HA coated and shot peened materials in 0.9% NaCl solution at 36.5$^{\circ}C$. After each electrochemical measurement, the corrosion surface of each sample was investigated by SEM.

• 한국재료학회지
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• 제5권6호
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• pp.690-698
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• 1995

Oxidized Si wafer 위에 반응가스로 Si $H_4$과 Ge $H_4$을 사용하여 RTCVD(rapid thermal chemical vapor deposition)법으로 증착온도 450~5$50^{\circ}C$에서 다결정 S $i_{1-x}$G $e_{x}$ 박막을 증착하였다. 증착된 S $i_{1-x}$, G $e_{x}$ 박막은 증착온도와 Ge $H_4$Si $H_4$입력비 변화에 따른 Ge몰분율 변화와 증착속도에 대해 고찰하였으며, XRD와 AFM(atomic force microscopy)등을 이용하여 결정상과 표면거칠기 등을 조사하였다. 실험결과, 다결정 S $i_{1-x}$G $e_{x}$ 박막은 32~37 Kcal/mole의 활성화에너지 값을 가졌으며 증착속도는 증착온도와 입력비 중가에 따라 증가하였다. 또한 조성분석으로부터 입력비 감소와 증착온도 증가에 따라 Ge몰분율이 감소함을 알 수 있었다. 증착된 S $i_{1-x}$G $e_{x}$ 박막은 450, 475$^{\circ}C$에서 임력비가 0.05일때 비정질 형태로 존재하였으며 그 이외의 실험영역에서는 다결정 형태로 존재하였다. 기존의 다결정 Si 중착온도($600^{\circ}C$이상)와 비교하여 Ge $H_4$을 첨가함으로써 비교적 낮은온도(5$50^{\circ}C$이하) 영역에서 다결정 S $i_{1-x}$G $e_{x}$ 박막을 얻을 수 있었다. 또한 증착층의 표면거칠기를 측정한 결과, 증착온도와 입력비가 증가함에 따라 표면 거칠기( $R_{i}$ )가 증가함을 알 수 있었다.을 알 수 있었다.

• 한국지구과학회지
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• 제43권5호
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• pp.604-617
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• 2022

해수면온도는 해양-대기의 현상을 이해하고 기후변화를 예측하기 위해 사용되는 중요한 변수이다. 마이크로파 영역의 인공위성 원격탐사는 구름과 강수와 같은 기상현상 위성 관측 측기의 경로에 존재하더라도 해수면온도 획득을 가능하게 한다. 따라서 마이크로파 해수면온도의 높은 활용도를 고려하면 위성 해수면온도를 정확도를 지속적으로 검증하고 오차 특성을 분석할 필요가 있다. 본 연구에서는 2014년 3월부터 2021년 12월까지 약 8년 동안 Global Precipitation Measurement (GPM)/GPM Microwave Imager (GMI) 마이크로파 해수면온도의 정확도를 표층 뜰개 부이 수온 자료를 사용하여 검증하였다. GMI 해수면온도는 실측 해수면온도에 비해 0.09 K의 편차와 0.97 K의 평균 제곱근 오차를 보였고, 이는 기존 연구 결과에 비해 다소 높게 나타났다. 이외에도 GMI 해수면 온도의 오차 특성은 위도, 연안과의 거리, 해상풍 및 수증기량과 같은 환경적 요인과 관련성이 있다. 오차는 육지에서 300 km 이내의 거리에서 해안 지역에 가까운 지역과 고위도 지역에서 증가하는 경향이 있다. 또한 낮에는 약한 풍속(<6 m s^-1), 밤에는 강한 풍속(>10 m s^-1) 범위에서 상대적으로 높은 오차가 나타났다. 대기 수증기는 30 mm 미만의 매우 낮은 범위 또는 60 mm보다 큰 매우 높은 범위에서 높은 해수면온도 차이에 기여했다. 이러한 오차들은 저수온에서 GMI 자료의 정확도가 떨어지는 기존 연구와 일치하며, 연안으로부터의 거리, 풍속, 수증기량에 의한 오차의 경우 육지와 해양의 방사율 차이 및 바람에 의한 해수면 거칠기 변화, 수증기의 마이크로파 대기 흡수에서 기인하는 것으로 추정된다. 이는 한반도 주변해에서 마이크로파 위성 계산 SST를 보다 광범위하게 활용하기 위해서는 GMI 해수면온도 오차의 특성에 대한 이해가 필요함을 시사한다.

• 한국지반환경공학회 논문집
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• 제4권4호
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• pp.45-51
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• 2003

암반 내에서 주입재는 토사지반에서와는 달리 절리면을 따라 맥상으로 주입되며 그 결과 암반 내의 불연속면의 특성을 변화시키게 된다. 그러므로 그라우팅 후 암반의 변형특성은 주입재가 주입되는 절리의 방향, 절리의 특성, 그리고 현지암반의 응력상태에 따라 달라지게 된다. 즉 그라우팅에 의한 보강효과를 정확히 평가하기 위해서는 암반 내의 불연속면의 특성과 주입재의 특성이 암반의 변형거동에 미치는 영향을 규명하여야 한다. 그러나 현재까지 현장에서 적용되고 있는 그라우팅공법은 시공자의 경험에 의존하고 있으며, 그 효과에 대한 검증도 현장에서의 탄성파속도 측정, 투수시험 등을 통하여 평가하고 있다. 따라서, 본 연구에서는 그라우팅에 의한 댐 기초 암반절리면의 전단변형특성을 파악하기 위해서 자연암석 절리면에 OPC(Ordinary Portland Cement)와 Micro Cement를 각각 주입하여, 주입재의 종류, 절리면 거칠기의 평균진폭(a)에 대한 주입두께(t)를 변화시켜가면서 암석절리면 직접전단시험을 실시한 실험결과들을 비교 분석하여 최대전단강도, 잔류전단강도 등의 전단특성에 미치는 영향에 대하여 검토하였다.

• 한국농공학회지
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• 제18권2호
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• pp.4116-4120
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• 1976

With the use of many rivers increased nearly to the capacity, the need for information concerning daily quantities of water and the total annual or seasonal runoff has became increased. A systematic record of the flow of a river is commonly made in terms of the mean daily discharge Since. a single observation of stage is converted into discharge by means of rating curve, it is essential that the stage discharge relations shall be accurately established. All rating curves have the looping effect due chiefly to channel storage and variation in surface slope. Loop rating curves are most characteristic on streams with somewhat flatter gradients and more constricted channels. The great majority of gauge readings are taken by unskilled observers once a day without any indication of whether the stage is rising or falling. Therefore, normal rating curves shall show one discharge for one gauge height, regardless of falling or rising stage. The above reasons call for the correction of the discharge measurements taken on either side of flood waves to the theoretical steady-state condition. The correction of the discharge measurement is to consider channel storage and variation in surface slope. (1) Channel storage As the surface elevation of a river rises, water is temporarily stored in the river channel. There fore, the actual discharge at the control section can be attained by substracting the rate of change of storage from the measured discharge. (2) Variation in surface slope From the Manning equation, the steady state discharge Q in a channel of given roughness and cross-section, is given as {{{{Q PROPTO SQRT { 1} }}}} When the slope is not equal, the actual discharge will be {{{{ { Q}_{r CDOT f } PROPTO SQRT { 1 +- TRIANGLE I} CDOT TRIANGLE I }}}} may be expressed in the form of {{{{ TRIANGLE I= { dh/dt} over {c } }}}} and the celerity is approximately equal to 1.3 times the mean watrr velocity. Therefore, The steady-state discharge can be estimated from the following equation. {{{{Q= { { Q}_{r CDOT f } } over { SQRT { (1 +- { A CDOT dh/dt} over {1.3 { Q}_{r CDOT f }I } )} } }}}} If a sufficient number of observations are available, an alternative procedure can be applied. A rating curve may be drawn as a median line through the uncorrected values. The values of {{{{ { 1} over {cI } }}}} can be yielded from the measured quantities of Qr$.$f and dh/dt by use of Eq. (7) and (8). From the 1/cI v. stage relationship, new vlues of 1/cI are obtained and inserted in Eq. (7) and (8) to yield the steady-state discharge Q. The new values of Q are then plotted against stage as the corrected steadystate curve.