• 한국강구조학회 논문집
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• 제28권6호
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• pp.449-458
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• 2016

강박스거더교의 온도하중을 위한 유효온도를 산정하기 위하여, 강박스거더교의 시험체와 실교량에서 온도 데이터가 2년간 측정되었다. 이 실험체와 실교량의 온도 측정결과를 바탕으로 대기온도에 대한 최고 및 최저 유효온도를 2014년, 2015년, 그리고 연속 2년간 산정하였다. 산정된 최고, 최저 유효온도는 EURO code, 그리고 현행 도로교 설계기준과 서로 비교 평가되었다. 2년간(2 year) 측정한 데이터 기준으로 최대 유효온도와 Euro code의 결정계수는 교량 시험체에서 R=0.894, 실교량에서 R=0.927이 산정되며, 최저 유효온도는 교량 시험체에서 R=0.992, 실교량에서 R=0.813이 산정되었다. 또한 연구 결과는 도로교설계기준(한계상태설계법)의 최고온도와 유사하든가 약간 초과하는 것으로 평가되었다.

• 대한지리학회지
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• 제39권1호
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• pp.13-26
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• 2004

본 연구는 상대적 날씨 스트레스 지수로 NET의 적용 가능성을 파악하고자 하였다. 기상청에서 예보하고 있는 기온, 습도, 바람 자료를 이용하여 NET 값의 시공간적 분포 특성을 분석하였다. 여름철 스트레스 지수인 일 최고 NET의 지역별 스트레스 기준값은 바람과 습도보다는 기온의 영향을 받으므로 일 최고 기온의 분포와 유사하다. 겨울철 스트레스 지수인 일 최저 NET의 스트레스 기준값은 산지 지역과 서울 이북 지역에서는 낮은 기온의 영향을. 해안 지역에서는 강한 바람의 영향으로 기준값이 여름철에 비하여 다양하게 나타난다. 스트레스가 강한 날의 발생 빈도는 여름철은 뚜렷한 연변화가 나타나지 않지만, 겨울철에는 1990년대 중반 이후 뚜렷한 증가 경향을 보인다.

• 한국태양에너지학회 논문집
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• 제30권5호
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• pp.100-106
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• 2010

The purpose of this study is to predict the effective sky temperature on Osan City during the summer. The north latitude, east longitude of Osan City is $37^{\circ}06'$ and $127^{\circ}02'$. The altitude from the sea level is 48m. Empirical relations of the effective sky temperature suggested by Duffie and Beckman are compared on clear days. For the effective sky temperature prediction, data measured by the Korea Meteorological Administration is used as an input to the Bliss model. Both Hottel and Krondratyev model are used to calculate the water vapor emissivity. The results using Hottel's model match well with the empirical relation proposed by Bliss. The results show maximum, minimum, and average values depending on water vapor emissivity model. The maximum deviation is about 10K and is due to total emissivity model.

• 한국산학기술학회논문지
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• 제17권8호
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• pp.133-139
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• 2016

합리적인 설계 온도하중을 산정하기 위하여, 강상자형교의 시험체가 실물 규모로 제작되었다. 박스단면의 크기는 폭 2.0m, 높이 2.0m, 길이 3.0m이며, 슬래브의 두께는 17 cm이다. 온도 게이지를 사용하여 1년간 온도를 측정하였다. 또한 인근에 시험체와 유사한 방향으로 설치된 같은 형식의 실교량에서도 같은 기간에 온도를 측정하였다. 교량시험체는 21지점, 실교량에서는 19지점에서 온도를 측정하고 각 측점에서 측정온도를 통계 처리하여 추세선과 표준 오차를 산정하고, Euro code에서 제시한 대기온도 $24^{\circ}C{\sim}38^{\circ}C$에서 각 지점의 유효온도를 산정하였다. 교량시험체 모형에서는 $35^{\circ}C$이상에서 Euro code와 실교량과 비교하여 유효온도가 $2^{\circ}C{\sim}3^{\circ}C$ 정도 높게 산정되었다. 제시된 시험체와 실교량에서 Euro code에 대한 유효온도의 상관계수는 87.4%, 93.2%로 계산되었다. 국내 도로교설계기준에 따르면 합성교에서 최고기온은 $40^{\circ}C$로 규정하고 있는데 이는 본 연구에서 산정된 실교량과 Euro code의 유효온도와 거의 근접하는 것으로 평가된다. 각 지역별 최고 온도에 대한 Contour map에서 산정한 대기온도별 최고온도와 본 연구에서 제시한 유효온도를 접목하면 국내 교량 설계 시 각 지역의 특성을 고려한 설계기준이 확립될 수 있을 것이다.

• 한국산학기술학회논문지
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• 제21권11호
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• pp.740-745
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• 2020

콘크리트 박스거더교의 합리적인 설계 온도하중을 산정하기 위하여, 1개의 교량시험체를 제작하였다. 교량시험체에 설치된 23개의 온도 게이지에서 1년간의 여름과 겨울기간에 30분 간격으로 하루에 48세트의 온도를 측정하였다. 상부 콘크리트와 측벽, 하부슬래브에 두께에 따른 온도변화를 검토하기 위하여 두께에 따라 여러 온도게이지를 부착하였다. 각 측점에서 측정된 온도를 통계 처리하여 추세선과 표준오차를 산정하고, 대표측점의 온도분포와 추세선을 제시하였다. 이를 바탕으로 Euro code에서 제시한 대기온도에서 여름철의 최고 유효온도와 겨울철의 최저 유효온도를 각각 산정하였다. 최고 유효온도는 35℃ 이상에서 Euro code와 비교하여 1.5~2℃ 높게 산정되었고, 최저 유효온도는 -13℃~-19℃에서 0.5~1.1℃로 더 낮게 분석되었다. 양산지방의 50년빈도 최고 및 최저 기온에 따른 본 연구의 유효온도와 비교해 보면, 최고 유효온도는 4.7℃ 높게, 최저 유효온도는 4.5℃ 더 낮게 산정되었다. 점점 높아지는 기후변동을 고려하고, 본 분석의 결과를 반영하면, 현 온도설계기준은 그 범위를 더 크게 하는 것이 필요한 것으로 판단된다.

• Journal of Acupuncture Research
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• 제26권1호
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• pp.111-119
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• 2009

Objectives : The purpose of this study is to investigate the mechanism and effect of moxa bucket moxibustion, to be used as the quantitative data through the measurement of temperature, and to grasp the thermodynamic characteristics of moxa bucket moxibustion. Methods : We have selected the moxa bucket moxibustion. We have made a comparative study of the thermodynamic characteristics of moxa bucket moxibustion. We have examined combustion times, temperatures, temperature gradients in each period during a combustion of moxa bucket moxibustion made by oak wood. Results : 1. We could design the moxa bucket moxibustion so that it has $57.6^{\circ}C$ maximum temperature with 7g weight and 10mm height, if we use more weight of moxa or lower height of moxa, we can observe relatively elevated maximum temperature. We observed the maximum temperature following the measuring position of moxa bucket and we could see higher temperature at the center of the moxa bucket and lower temperature at the side of the moxa bucket. 2. We could design the moxa bucket moxibustion with 5g moxa and 10mm height so that it has 0.12 $1^{\circ}C/sec$ of maximum temperature gradient, and it has relatively high temperature gradient at lower weight and height condition. 3. We could design the moxa bucket moxibustion with 7g moxa and 15mm height so that it has 4,135sec of the longest effective temperature combustion time. If we use more weight of moxa or higher height of moxa, we can observe relatively extended effective temperature combustion time. Conclusions : We observed the longest effective combustion time following the measuring position of moxa bucket. We can see a higher temperature at the center of the moxa bucket and a lower temperature at the side of the moxa bucket.

• Journal of Acupuncture Research
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• 제24권1호
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• pp.49-77
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• 2007

Objectives: The purpose of this study is to investigate the mechanism and effect of moxa bucket moxibustion. Objectively, to be used as the quantitative data through the measurement of temperature, and to grasp the thermodynamic characteristics of moxa bucket moxibustion. Methods: We have selected of the moxa bucket moxibustion. We make a comparative study of the thermodynamic characteristics of moxa bucket moxibustion. We examined combustion times, temperatures, temperature gradients in each period during a combustion of moxa bucket moxibustion made by oak wood. Results: 1. We can design the moxa bucket moxibustion that it has 57.6$^{\circ}C$ maximum temperature with 7g weight and 10mm height, if we use more weight of moxa or lower the height of moxa, we can observe relatively elavated maximum temperature. We observe the maximum temperature following the measuring position of moxa bucket and we can see higher temperature at the center of the moxa bucket and lower temperature at the side of the moxa bucket. 2. We can design the moxa bucket moxibustion with 5g moxa and 10mm height that it has 0.121 $^{\circ}C$/sec of maximum temperature gradient, and it has relatively high temperature gradient at lower weight and height condition. 3. We can design the moxa bucket moxibustion with 7g moxa and 15mm height that it has 4,135sec of the longest effective temperature combustion time, if we use more weight of moxa or higher height of moxa, we can observe relatively extended effective temperature combustion time. We observe the longest effective combustion time following the measuring position of moxa bucket. We can see higher temperature at the center of the moxa bucket and lower temperature at the side of the moxa bucket.

• 소성∙가공
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• 제10권1호
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• pp.35-41
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• 2001

The high temperature deformation behavior of SCM 440 can be characterized by the hot torsion test in the temperature ranges of $900^{\circ}C$~$1100^{\circ}C$ and strain rate ranges of 0.05/sec~5/sec. The aim of this paper is to establish the quantitative equation of the volume fraction of dynamic recrystallization (DRX) as a function of processing variables, such as strain rate ($\varepsilon$), temperature (T), and strain ('$\varepsilon$). During hot deformation, the evolution of microstructure could be analyzed from work hardening rate ($\theta$). For the exact prediction of dynamic softening mechanism the critical strain ($\varepsilon_c$), the strain for maximum softening rate ($\varepsilon^*$ and Avrami' exponent (m') were quantitatively expressed by dimensionless parameter, Z/A, respectively. The transformation-effective strain-temperature curve for DRX could be composed. It was found that the calculated results were agreed with the experimental data for the steel at any deformation conditions.

• Journal of Acupuncture Research
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• 제18권6호
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• pp.171-187
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• 2001

Objective : Moxibustion has been proved efficacious for many diseases, but isn't widespread in the clinics due to a danger of skin burning, the smoke produced while burning a moxa combustion and so on. Therefore, another type of moxa that can be resolved these troubles is required. To improve the effect of moxibustion and develop the new thermal stimulating treatment, the performance of commercial moxibustion widely used are studied systematically and found out quantitatively. Methods : We have selected two types (small-size moxa A(sMA), small-size moxa B (sMB)) among small-size moxaes used widely in the clinic. We examined combustion time, various temperatures, temperature gradient in each period during a combustion of moxa. Results : 1. The combustion time in the preheating period appeared somewhat longer in sMA than in sMB. 2, The combustion time in the heating period appeared longer in sMA by 26% than in sMB. 3. The average temperature in the heating period was $37.6{\sim}37.8^{\circ}C\;in\;sMA\;and\;36.2{\sim}36.8^{\circ}C$ in sMB and the maximum temperature measured at a center of contact surface in sMA was $48.6^{\circ}C$, higher by over $2.8^{\circ}C$ than that of sMB moxibustion. 4. The average ascending temperature gradient in the heating period was $0.08{\sim}0.1^{\circ}C/sec$ in both moxaes, and the average ascending temperature gradient of heating period in sMB appeared larger. The maximum ascending temperature gradient appeared higher in sMB, and the time reaching maximum ascending temperature gradient appeared much earlier in sMA than in sMB. 5. The combustion time in the retaining period was around 100 sec in sMA and around 275 sec in sMB. 6. The average temperature in the retaining period was $42.2{\sim}46.0^{\circ}C\;in\;sMA\;and\;39.3{\sim}41.4^{\circ}C/sec$ in sMB. The minimum temperature in the retaining period was over $38.80^{\circ}C$ in sMA but just $34.7^{\circ}C$ in sMB. 7. The average descending temperature gradient in sMA was $-0.050{\sim}0.067^{\circ}C/sec$ and in sMB was $-0.030{\sim}0.037^{\circ}C/sec$ 8. The combustion time in the cooling period appeared longer over two times in sMA than in sMB, and the time which the cooling period (minimum temperature) finished at appeared later in sMB by 55 sec. 9. We classified the combustion process that the measured temperature rose over body heat($37^{\circ}C$) into the effective combustion period. The effective combustion time was 233.3 sec in sMA and 300.4 sec in sMB respectively, and was longer by about 29% in sMB. The average temperature and maximum temperature in the effective combustion time appeared higher in sMA. The time taken until the maximum temperature was reached was 225.1 sec in sMA and 244.5 sec in sMB, faster by about 20 sec in sMA. The maximum ascending temperature gradient during the effective combustion period appeared larger about 1.4 times in sMB, but the time when the maximum ascending temperature gradient happened was faster in sMA. Conclusion : It appears that sMB, compared with sMA, is proper if necessary to apply the long time and weak stimulus, because of the gentle stimulus during the relatively longer time. In contrast, sMA that the symmetrical combustion happened is proper if necessary to apply the short time and strong stimulus.

• Journal of Acupuncture Research
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• 제19권3호
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• pp.64-76
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• 2002

Objective : The purpose of this study is to investigate the mechanism and effect of moxibustion objectively and to be used as the quantitative data for developing the new thermal stimulating treatment by observing the combustion characteristics of commercial moxaes. Methods : We have selected two types(large-size moxa A(LMA), large-size moxa B(LMB)) among large moxaes used widely in the clinic. We examined combustion times, temperatures, temperature gradients in each period during a combustion of moxa. Results : 1. The ascending temperature gradient measured in the central point of non-contacted surface was fastest, the average ascending temperature gradient of both moxaes was $0.0384^{\circ}C/sec$, $0.0123^{\circ}C/sec$ respectively, 3.1 times faster in LMA. The maximum ascending temperature gradient was also about 2.9 times faster in LMA. The time required for the maximum ascending temperature gradient from ignition was 254sec, 411sec respectively. 2. The minimum descending temperature gradient in the retaining period was $-0.0250^{\circ}C/sec$, $-0.0090^{\circ}C/sec$ respectively and the average descending temperature gradient was $-0.0160^{\circ}C/sec$, $-0.0037^{\circ}C/sec$ respectively on the non-contact surface. 3. On the basis of the non-contact surface($A_I$), the time at which the effective stimulus period began to occur was about 264sec, 796sec respectively after an ignition, the time at which the maximum temperature began to occur was about 373sec, 1323sec respectively after an ignition, and the maximum temperature was $0.9^{\circ}C$ higher in LMA. The maximum ascending temperature gradient was also about 4.2 times faster in LMA. Conclusion : It was thought that not only the figure of moxicombustion device, but also the form and size of moxa had influence on the combustion characteristics deciding the performance of stimulus seriously.