• 한국산림과학회지
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• 제85권2호
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• pp.288-299
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• 1996

본 연구는 heat pulse법을 이용하여 신갈나무 장령림 임분(林分)의 증산량(蒸散量)을 알기 위한 기초연구로서, 신갈나무 입목에 있어서 일사량(日射量), 온도(溫度), 습도(濕度)(대기포차(大氣飽差)) 등의 변화(變化)에 따른 heat pulse 속도(速度)의 일변화와 계절변화, 방위별 heat pulse 속도(速度)의 차이, 변재부에 있어 깊이별 heat pulse 속도(速度)의 차이, 우세목(優勢木), 준우세목(準優勢木), 열세목(劣勢木)의 heat pulse 속도(速度)의 차이, 엽(葉)의 수분포텐셜과 heat pulse 속도(速度)와의 관계, 줄기에 있어 수분상승의 방향, 그리고, heat pulse법으로 측정한 단목(單木)과 임분(林分)의 일일(一日), 월별(月別), 년간(年間) 증산량(蒸散量) 등을 측정고찰하였다. 얻어진 결과를 요약하면 다음과 같다. 1. 신갈나무의 heat pulse 속도(速度)(V)와 수액유속(樹液流速)(SFR)과의 관계는 SFR=1.37V였다. 2. 우세목(優勢木), 준우세목(準優勢木), 열세목(劣勢木)의 heat pulse 속도(速度)를 비교하면, 수액유속(樹液流速)은 우세목(優勢木)이 가장 높고, 준우세목(準優勢木), 열세목(劣勢木) 순위였다. Heat pulse 속도(速度)는 일사량(日射量), 온도(溫度), 대기포차(大氣飽差) 등의 크기에 따라 일변화하였다. 3. Heat pulse 속도(速度)와 엽(葉)의 수분포텐셜은 거의 비슷한 일변화를 나타냈다. 4. Heat pulse 속도(速度)의 계절변화는 7월에 평균 2.9cm/hr로 가장 낮았고, 5월이 평균 4.0cm/hr로 가장 높게 나타났다. 5. 줄기에 있어서 heat pulse 속도(速度)의 차이는 북측이 가장 높았고, 서측이 그 다음 순이었으며, 남측과 동측은 큰 차이없이 가장 낮은 값을 나타냈다. 6. 변재부에 있어서 깊이별 heat pulse 속도(速度)의 차이는 수피로부터 0.5cm 깊이에서 가장 높고, 다음 1.0cm, 1.5cm 순으로 나타났다. 7. 줄기에 있어 수분이동방향(水分移動方向)은 4본 모두 부분적(部分的) 수직상승(垂直上昇)(sectorial straight ascent)을 나타내고 있었다. 8. 수액유량(樹液流量)(SF)은 SF=1.37AV식으로 나타났고, 이 식으로 구한 수액유량(樹液流量)은 우세목(優勢木)이 준우세목(準優勢木)과 열세목(劣勢木)보다 현저히 높았다. 9. 1ha의 임분(林分)에 대한 1일의 증산량(蒸散量)의 구성비율(構成比率)은 낮이 72%, 밤이 28%였고, 증산량(蒸散量)은 약 5.6ton/ha/day이었다. 10. 1ha의 월별(月別) 증산량(蒸散量)은 5월이 168ton/ha/month으로 가장 많았고, 7월이 125ton/ha/month로 가장 낮았다. 또 1 ha의 년간(年間) 증산량(蒸散量)은 839ton/ha/yr이었다.

• 한국산림과학회지
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• 제82권2호
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• pp.152-165
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• 1993

본(本) 연구(硏究)는 heat pulse법(法)을 이용하여 낙엽송 임분(林分)의 증산량(蒸散量)을 알기 위한 기초 연구로써, 일사량(日射量), 온도(溫度), 습도(濕度) 등의 변화에 따른 heat pulse 속도(速度)의 일변화와 계절변화, 방위별 heat pulse 속도(速度)의 차이, 변재부(邊材部)에 있어서 깊이별 heat pulse 속도(速度)의 차이, 우세목(優勢木), 준우세목(準優勢木), 열세목(劣勢木)의 heat pulse 속도(速度)의 차이, 엽(葉)의 수분(水分)포텐셜과 heat pulse 속도(速度)와의 관계, 줄기에 있어 수분상승의 방향, heat pulse법(法)으로 추산한 임분(林分)의 증산량(蒸散量)등에 대하여 측정 고찰하였다. 얻어진 결과를 요약하연 다음과 같다. 1 낙엽송의 heat pulse 속도(速度)(V)와 수액유속(樹液流速)(SFR)과의 관계는 SFR=1.37V($r=0.96^{**}$)의 식으로 나타냈다. 2. 우세목(優勢木), 준우세목(準優勢木), 열세목(劣勢木)의 heat pulse 속도(速度)를 비교하면, 수액유속(樹液流速)은 우세목(優勢木)이 가장 높고, 준우세목(準優勢木), 열세목(劣勢木) 순위였다. Heat pulse 속도(速度)는 일사량(日射量), 온도(溫度), 대기포차(大氣飽差) 등의 크기에 따라 심한 변화(變化)를 나타냈다. 3. 입목(立木) 개체간(個體間)의 heat pulse 속도(速度)의 차이는 이른 아침과 밤에는 거의 없으나, 일사량(日射量)이 높은 12시부터 16시 사이에는 약간의 차이를 나타냈다. 4. Heat pulse 속도(速度)와 수분(水分)포텐셜은 거의 비슷한 일변화 경향을 나타냈다. 5. Heat pulse 속도(速度)의 계절변화는 8월에 가장 높았고, 10월이 가장 낮았다. 그리고 6, 7, 9월의 heat pulse 속도(速度)는 거의 비슷한 값을 나타냈다. 6. 줄기에 있어 방위별 heat pulse 속도(速度)는 동측이 가장 높았고, 서측과 북측은 비슷한 속도를 나타냈으며, 남측의 속도가 가장 낮았다. 7. 변재부(邊材部)에 있어서 깊이별 heat pulse 속도(速度)의 차이는 수피(樹皮)로부터 2cm 깊이에서 가장 높고, 다음이 1cm 깊이, 그리고 3cm 깊이에서 가장 낮았다. 8. 줄기에 있어 수분이동방향(水分移動方向)은 5본 모두 오른쪽 나선상승(螺旋上昇)(spiral ascent turning right)을 나타내고 있었다. 특히 지상의 3m까지는 매우 느린 회선(回旋)을 나타내다가 그 이상의 수고(樹高)에서는 매우 빠른 회선(回旋)으로 상승됨을 알 수 있었다. 9. 수액유량(樹液流量)(SF)은 SF=1.37AV 식(式)으로 나타났고, 이 식으로 구한 수액유량(樹液流量)은 우세목(優勢木)이 준우세목(準優勢木)과 열세목(劣勢木)보다 현저히 높았다. 10. 1ha의 임분(林分)에 대한 1일의 증산량(蒸散量)의 구성비율(構成比率)은 낮이 83%, 밤이 17%였고, 증산량(蒸散量)은 약 30.8ton/ha/day이었다. 11. 1ha의 월별(月別) 증산량(蒸散量)은 8월이 1,194ton/ha/month로 가장 많았고, 5월이 386ton/ha/month로 가장 낮았다. 또 1ha의 연간(年間) 증산량(蒸散量)은 3,983ton/ha/yr이었다.

• 설비공학논문집
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• 제12권3호
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• pp.284-291
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• 2000

A basic pulse tube refrigerator has been constructed with extensive instrumentation to study the characteristics of the heat exchanger experimentally under the oscillating pressure and the oscillating flow. This paper describes the sequential experiments with the basic pulse tube refrigerator. The experiments were performed for various cycle frequencies under the square pressure wave forms. First, the heat flux was measured through the cycle at the both cold and warm end heat exchangers without the regenerator. In order to enhance the thermal communication capability of the heat exchanger with the gas at low operating frequencies, a unique design of the triangular shape radial fin concept was applied to the heat exchangers. For the fin heat exchanger, the measured heat flux and the calculated heat flux from the two well-known oscillating heat transfer correlations were compared and discussed. Second, the regenerator was added to the pulse tube to make a basic pulse tube refrigerator configuration. The experiment showed the great impact of the regenerator on the temperature and the heat flux profiles. At the warm-end, the cyclic averaged heat flux had its maximum value at the specific operating frequency. The paper presents the explanation of the surface heat pumping effect as well as the experimental data.

• Journal of Welding and Joining
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• 제33권6호
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• pp.60-66
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• 2015

Molten zone shape of pulse laser welding is affected by welding conditions such as beam power, beam speed, irradiation time, pulse frequency, etc. and is divided into conduction type and keyhole type. It is necessary to design heat source model for irradiation of laser beam in the pulse laser welding. Shape variables and the maximum energy density value of the heat source model are different depending on the molten zone shape. In this paper, pulse laser welding simulation for joining of cylindrical part and circular cover was carried out. The heat source model for pulse laser beam with circular path was applied to the heat input boundary condition, radiative and conductive heat transfer were considered for the thermal boundary condition. For each phase, thermal and mechanical properties according to temperature were also applied to analysis. Analytical results were in good agreement with the molten zone size of specimen under the same welding conditions. So, the reliability of the welding simulation was verified. Finally, the improvements for reducing residual deformation after cover welding could be reviewed analytically.

• 한국초전도ㆍ저온공학회논문지
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• 제2권1호
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• pp.45-50
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• 2000

The present study has been conducted to observe the heat transfer under pulsating pressure and oscillating flow. The experimental apparatus was fabricated to measure the gas temperature, the wall temperature. the pressure and the instantaneous heat flux inside the pulse tube. The measured gas temperature and heat flux must be calibarated to compensate their finite time constant in the oscillating flow conditious. The experiment was performed from 1 Hz to 5 Hz. The phase difference between the instantaneous heat flux and the gas-wall temperature difference was clearly observed. The experimental heat fluxes were compared to the theroretical correlations such as Complex Nusselt Number Model(CNNM) and Variable Coefficient Model(CVM). The heat flux predisted by CNNM was always greater than that of VCM. The experiment confirmed the valisity of the VCM for the instantaneous heat flux under the pulsating pressure and oscillating flow in the warm end of the pulse tube.

• 한국수자원학회:학술대회논문집
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• 한국수자원학회 2001년도 학술발표회 논문집(I)
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• pp.52-59
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• 2001

Methods to measure and estimate transpiration of a forest composed of evergreen broad-leaved trees (Pasania edulis Makino) are studied. Heat pulse velocity has been measured along with soil moisture and micrometeorological factors at the Fukuoka Experimental Forest, the Research Institute of Kyushu University Forests in Fukuoka, Japan (33$^{\circ}$38'N, 130$^{\circ}$31'E, alt. 75m). Tree cutting measurement was conducted to convert the heat pulse velocity into sap flow and transpiration. A big leaf model to calculate transpiration and Interception loss is examined and the estimated values are compared with the measured values obtained from the heat pulse measurement. The results show that 1) Pasania edulis Makino posessing radial pore structure had relatively high water content and high heat pulse velocity even within the central part of the stem near the pith, 2) the heat pulse velocity was well correspond to the water uptake in the tree cutting measurement, 3) the estimation of sap flow based on the heat pulse velocity is accurate, and 4) the big leaf model using the parameters obtained from measurement of a portable photosynthesis system in one day in summer gives reasonable estimation of transpiration independent of seasons and weather.

• 대한한의진단학회지
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• 제19권2호
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• pp.91-100
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• 2015

Objectives The aim of this study is to develop a structured clinical protocol related with acquisition of radial pulse wave in the randomized, $2{\times}2$ cross-over design, and cold-heat intervention trial for a pilot and preliminary study. Methods The protocol was contrived based on wide ranging literature searches for cold-heat intervention experiments and radial pulse diagnoses. Results Sample size of 60 subjects was calculated based on an effect size derived from the previous study designed to detect the pre-post cold-heat differences in the radial pulse. Each subjects will be randomly assigned to the cold (first) to heat (last) group (n=30) or heat (first) to cold (last) group (n=30). All subjects will fill out a case report form and questionnaires related with pattern identification, dietary patterns, sleep quality, and physical activity will be surveyed and used as a secondary outcomes. Safety assessment will be reported at the final stage. Conclusions This protocol will provide an additional reference to future studies related with observation of radial pulse during any interventions and also expect to be used as a guideline for acquisition of reliable radial pulse wave data.

• Journal of Mechanical Science and Technology
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• 제19권6호
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• pp.1378-1389
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• 2005

This work provides the fundamental knowledge of energy transport characteristics during very short-pulse laser heating of semiconductors from a microscopic viewpoint. Based on the self-consistent hydrodynamic equations, in-situ interactions between carriers, optical phonons, and acoustic phonons are simulated to figure out energy transport mechanism during ultrafast pulse laser heating of a silicon substrate through the detailed information on the time and spatial evolutions of each temperature for carriers, longitudinal optical (LO) phonons, acoustic phonons. It is found that nonequilibrium between LO phonons and acoustic phonons should be considered for ultrafast pulse laser heating problem, two-peak structures become apparently present for the subpicosecond pulses because of the Auger heating. A substantial increase in carrier temperature is observed for lasers with a few picosecond pulse duration, whereas the temperature rise of acoustic and phonon temperatures is relatively small with decreasing laser pulse widths. A slight lagging behavior is observed due to the differences in relaxation times and heat capacities between two different phonons. Moreover, the laser fluence has a significant effect on the decaying rate of the Auger recombination.

• 한국정밀공학회지
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• 제14권5호
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• pp.53-59
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• 1997

This study has been performed to inmvestigate MRR(metal removal rate), REW(relative electrode wear), surface roughness, heat transumutation layer and microhardness distribution in cross-section of the machined surface with various pulse-on duration and peak pulse current, using the copper and graphite electrode on the heat treated STD11 which is extensively used for metallic molding steel with the EDM. The results obtained are as follows; a) There exists critical pulse-on duration(If Ip equals 5A, .tau. on is 50 .mu. s) which shows the the maximum MRR in accordance with peak oulse current and the MRR decreases when the pulse-on duration exceeds the critical pulse-on during because of the abnormal electric discharge. b) Safe discharge is needed to make maximum of MRR and the metalic organization must be complicated for discharge induction. c) Graphite has much more benefits than copper electrode when rapid machining is done without electrode wear. d) The most external surface has the highest microhardness because of car- burizing from heat analysis of the dielectric fluid and the lower layar of the white covered layer has lower microhar dness than base matal because of softening.

• Journal of Welding and Joining
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• 제21권4호
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• pp.56-62
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• 2003

MIG brazing is used for many parts without melting base metal because of high productivity. Pulsed MIG brazing can be used to further reduce heat input and to improve the process stability. However, a significant amount of zinc in galvanized sheet steel is burned off in the area of brazes. Therefore, the brazing method to reduce the heat input is needed. In the brazing for galvanized sheet steel, variable polarity AC pulse MIG arc brazing can be applied to more decrease the heat input by setting EN-ratio adequately. In this research, we studied for the variable polarity AC pulse MIG arc brazing to decrease the heat input by using ERCuSi-A wire. As the result of increasing EN-ratio, melting ratio of base metal and burning off of zinc were reduced in galvanized sheet steel.