• 에너지공학
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• 제29권2호
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• pp.61-67
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• 2020

ESS 기반 건축물은 에너지 절감을 ZEB, BEMS, FEMS 등 에너지 절감을 위한 주효한 수단으로 활발히 연구되고 있다. 하지만 규모가 큰 건축물에서는 에너지 사용설비가 매우 많아, 실시간 계측 시스템 구축을 위해서는 중요 에너지 사용 설비 파악이 필요하다. 또한 에너지 사용량이라는 종속변수에 영향을 끼치는 인자들 역시 무수히 많아, 효과적인 에너지 관리가 어렵다는 한계점이 있다. 따라서 본 연구에서는 실증 ESS 유통 물류시설을 대상으로 실사를 통해 에너지 공급현황에 따른 측정 경계 방법론을 적용, 계측 시스템 구축을 위한 우선순위를 제시하였다. 이후 실제 유통물류 시설의 에너지 사용량에 영향을 미치는 독립변수 파악을 위해 필요한 영향 변수들을 고유변수와 기상변수로 분류하여 종속변수인 실제 유통물류 시설의 에너지 사용량에 영향을 끼칠 가능성이 있는 모든 인자들을 영향변수화 하여, 이를 가이드라인으로 제시하였다. 본 연구 결과를 적용함으로써 복잡한 구조의 유통 물류 시설에서 저비용, 고효율로 모니터링 시스템 구축할 수 있고, 그렇게 계측된 에너지 사용량에 주요한 독립변수를 파악하여 에너지 사용량의 추이 파악과 절감포인트 도출을 통한 효과적인 ESS-기반 시설물의 운용이 가능할 것으로 기대된다.

• 천문학회보
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• 제38권2호
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• pp.57.1-57.1
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• 2013

We investigate the method to measure both the present value of the matter energy density contrast and the Hubble parameter directly from the measurement of the linear growth rate which is obtained from the large scale structure of the Universe. From this method, one can obtain the value of the nuisance cosmological parameter $\Omo$ (the present value of the matter energy density contrast) within 3% error if the growth rate measurement can be reached $z >3.5$. One can also investigate the evolution of the Hubble parameter without any prior on the value of $H_0$ (the current value of the Hubble parameter). Especially, estimating the Hubble parameter are insensitive to the errors on the measurement of the normalized growth rate $f \sigma_8$. However, this method requires the high $z$ ($z >3.5$) measurement of the growth rate in order to get the less than 5% errors on the measurements of $H(z)$ at $z \leq 1.2$ with the redshift bin $\Delta z = 0.2$. Thus, this will be suitable for the next generation large scale structure galaxy surveys like WFMOS and LSST.

• 한국원자력학회:학술대회논문집
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• 한국원자력학회 2004년도 추계학술발표회 발표논문집
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• pp.1353-1354
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• 2004

It was estimated by an analysis method thai the inner shell of HANARO reactor will be deformed due to pressure, loads, creep and growth during reactor operation. To confirm the analysis validity and safe operation of reactor, we developed tools to remotely measure the straightness of the inner shell located 12m below the pool top. The performance and the accuracy of the measurement tools have been verified through tests using a dummy inner shell and steel straight edge. The accuracy of the measurement shows very good results with a maximum error of 0.06mm by steel straight edge. The technical experiences described in this paper will be a good reference not only for the operation and maintenance of HANARO but also for the next performance of the measurement in the future.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2003년도 추계학술대회
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• pp.1109-1114
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• 2003

The initial crack often occurs on the bonded interface and it is the general cause of the interface fracture. It is very significant to establish the measurement method of interfacial crack by applying the ultrasonic technology into the interface of bonded dissimilar materials. In this paper, the interfacial crack length was measured by ultrasonic attenuation coefficient in the Al/Epoxy bonded dissimilar materials of double-cantilever beam(DCB). The energy release rate, G, was obtained by the experimental and Ripling's equation measurement of compliance. The experimental results represent that the relation between interfacial crack length for the ultrasonic attenuation coefficient and energy release rate is increased proportionally. From the experimental results, a measurement method of the interfacial crack length by the ultrasonic attenuation coefficient was proposed and discussed.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2006년도 하계학술대회 논문집 Vol.7
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• pp.5-7
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• 2006

In this paper, we analyzed the elements of measurement uncertainty on electrical performance test which are the most important things in photovoltaic module performance test. Repeating the performance test by 6 men, the measurement uncertainty could be calculated. In this experiment, Solar Simulator (A-Class pulse type) used for domestic certificate test of PV module is Pasan IIIb (Balval, Switzerland). The possible elements of the measurement uncertain that could effect electrical performance test of PV module are reference cell, spectrum correction, error from measurement repetition, test condition, stability and uniformity of artificial solar simulator. To find the measurement uncertainty, 6 men repeated the test by 10 times. And the results were that numerical average value was 124.44W and measurement uncertainty was $124.44W{\pm}0.75W$ with 95% confidence level for 125W PV module.

• 방사선산업학회지
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• 제6권3호
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• pp.231-237
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• 2012

This paper introduces a gamma-ray measurement system for a transportable tomography which is applicable for an industrial process diagnosis. The gamma-ray measurement system consists of pulse mode operating 72 channel CsI detectors, main AMP-pulse shaper, single channel analyzer, counter and control PC. The CsI crystal is coupled with a PIN diode which is connected to an amplifier and pulse shaper. For a compact design, the amplifier and pulse shaping circuit are included in a single package. 36 sets of CsI detectors are connected to a multi-channel counter through single channel analyzers. A computer controls and collects data from two multi-channel counters. This configuration results in 72 channel counting system in total. The CT rotator and radiation measurement system are controlled by a PC with LabVIEW program. Tomographic data were measured for a phantom by the measurement system and transportable gamma-ray CT. From the experimental data image reconstructions were performed by ML-EM algorithm. The result showed that the CsI detector system can be a suitable component for transportable gamma-ray CT system.

• 한국방사성폐기물학회:학술대회논문집
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• 한국방사성폐기물학회 2017년도 춘계학술논문요약집
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• pp.149-150
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• 2017

• Journal of Radiation Protection and Research
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• 제43권1호
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• pp.29-38
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• 2018

Background: Radon contributing about 42% of annual average dose, mainly comes from soil. In this paper, standard measurement procedures for soil radon exhalation rate are suggested and their measurement uncertainties are analyzed. Materials and Methods: We used accumulation method for estimating surface exhalation rate. The closed-loop measurement system was made up with a RAD7 detector and a surface chamber. Radon activity concentrations in the system were observed as a function of time, with data collection of 5 and 15-minute and the measurement time of 4 hours. Linear and exponential fittings were used to obtain radon exhalation rates from observed data. Standard deviations of measurement uncertainties for two approaches were estimated using usual propagation rules. Results and Discussion: The exhalation rates (E) from linear approach, with 30 minutes measurement time were $44.8-48.6mBq{\cdot}m^{-2} {\cdot}s^{-1}$ or $2.14-2.32atom{\cdot}cm^{-2}{\cdot}s^{-1}$ with relative measurement uncertainty of about 10%. The contributions of fitting parameter A, volume (V) and surface (S) to the estimated measurement uncertainty of E were 59.8%, 30.1% and 10.1%, in average respectively. In exponential fitting, at 3-hour measurement we had E ranged of $51.6-69.2mBq{\cdot}m^{-2} {\cdot}s^{-1}$ or $2.46-3.30atom{\cdot}cm^{-2}{\cdot}s^{-1}$ with about 15% relative uncertainty. Fitting with 4-hour measurement resulted E about $51.3-68.2mBq{\cdot}m^{-2} {\cdot}s^{-1}$ or $2.45-3.25atom{\cdot}cm^{-2}{\cdot}s^{-1}$ with 10% relative uncertainty. The uncertainty contributions in exponential approach were 75.1%, 13.4%, 8.7%, and 2.9% for total decay constant k, fitting parameter B, V, and S, respectively. Conclusion: In obtaining exhalation rates, the linear approach is easy to apply, but by saturation feature of radon concentrations, the slope tends to decrease away from the expected slope for extended measurement time. For linear approach, measurement time of 1-hour or less was suggested. For exponential approach, the obtained exhalation rates showed similar values for any measurement time, but measurement time of 3-hour or more was suggested for about 10% relative uncertainty.

• 한국방사선학회논문지
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• 제7권3호
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• pp.245-249
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• 2013

천연 탄탈의 중성자포획에 의한 공명에너지를 측정하기 위하여 교토대학의 원자로연구소의 46-MeV 전자선형가속기의 광핵반응에서 발생하는 중성자를 이용하였다. 중성자포획에서 발생되는 즉발감마선을 BGO($Bi_4Ge_3O_{12}$)섬광검출장치로 측정하였다. 검출장치는 탄탈 시료에서 발생되는 즉발감마선을 기하학적으로 모두 측정하도록 만들어져 있으며 측정되어진 전기적 신호를 탄탈의 중성자 공명에너지 동정하는 스펙트럼구성에 사용하였다. 연구에서 사용되어진 중성자의 에너지는 1 ~ 200 eV 영역에 대하여 각각의 공명에너지를 분석하였다. 중성자에너지 측정은 중성자 비행시간법(TOF: Time-of-Flight)을 통하여 측정하였다. 광핵반응을 통한 중성자발생에서는 고에너지영역에서 강한 제동복사선이 발생하므로 수 keV영역 이하 영역의 중성자에너지에 대해서만 중성자공명을 측정하였다. 얻어진 Ta에 대한 중성자 포획 공명에너지 측정결과는 이전의 실험에 의한 측정 결과들 및 ENDF/B-VI와 Mughabghab의 평가된 값들과 비교 및 검토를 하였다. 측정되어진 공명들은 4.28 eV에서 거대 공명들을 측정하였고 그 이상의 에너지 영역의 다른 공명들도 이론에 의해서 계산되어진 값들과 비교하였다. 144.3 eV를 제외한 공명들은 평가값들과 거의 일치하는 경향을 보였다.

• 신재생에너지
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• 제3권4호
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• pp.114-122
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• 2007

This paper addresses the measurement of structural loads on the Unison U50 wind turbine. The load measurement are carried out to determine the actual loads acting on a wind turbine. This is needed not only the certification process but also improving the technical development for prototype wind turbine. The measurement system is consists of measuring load, operating quantities and meteorological signal. All data that occur during the operating of a WT are stored the data acquisition system automatically. With using the measured data, load spectrum and equivalent load are evaluated according to IEC61400-13 "Measurement of mechanical loads".