• 화약ㆍ발파
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• 제28권1호
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• pp.27-39
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• 2010

측정된 지반진동의 최대입자속도 자료에 대한 통계분석을 통해 환산거리 개념에 기초한 제어발파 설계조건식은 구할 수 있다. 이들 설계조건식들은 안전발파를 위한 다양한 허용기준에 따라 사용할 수 있는 환산거리의 최소값을 정의하는 형태로 되어 있다. 국내에서 널리 사용되는 환산거리에는 자승근 환산거리(SRSD)와 삼승근 환산거리(CRSD)의 두 가지가 있다. 따라서 SRSD와 CRSD의 설계조건식들은 각각 $D/\sqrt{W}{\geq}30m/kg^{1/2}$와 $D/\sqrt[3]{W}{\geq}60m/kg^{1/3}$의 형태가 된다. 제어발파 설계 시에는 이들 조건식들과 이격거리를 알고 있으므로 지반진동에 대해 구조물의 안정을 보장할 수 있는 최대 지발당장약량를 계산할 수 있다. 그러나 SRSD와 CRSD의 최대 지발당장약량은 각각 $W=O(D^2)$와 $W=O(D^3)$의 차원으로 나타난다. 따라서 SRSD에 비해 CRSD의 장약량은 두 회귀식의 유사한 적합도에도 불구하고 두 함수의 교점을 지나면 기하급수적으로 증가하게 된다. 따라서 본 논문에서는 CRSD의 지나치게 많은 장약량으로 인해 발생할 지도 모를 구조물의 피해를 방지하기 위해 CRSD는 어떤 특정한 거리 이내에서만 사용하도록 제한한다. 그 정확한 한계는 SRSD와 CRSD의 장약량 차가 교점 이내에서의 양자 간의 최대차를 초과하기 시작하는 점까지이다.

• Bulletin of the Korean Chemical Society
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• 제28권1호
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• pp.108-114
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• 2007

The lyotropic behaviors to form the structure of distearoylphosphatidylcholine (DSPC)-based liquid crystal (LC) hydrated by only propylene glycol (PG) without water were examined by differential scanning calorimetry (DSC), X-ray diffractions (XRD), polarized microscope (PM) and transmission electron microscope (TEM). By increasing the amount of PG instead of water, it showed the phase transition to be gradually changed from anisotropic structures to other structures more close to isotropic ones and their appearance to be changed from solid-like states to liquid-like ones with more fluidity. Below 50% w/w PG, the mixtures of DSPC and PG resulted in no direct observation of LC structure through PM because they were very close to solid-states. From 55% w/w to 90% w/w of PG, the dense lamella crystalline structures were observed through PM, and their thickness and area decreased as the content of PG increased. Measured by DSC with heating process, the main phase transition from α -lamella phase to isotropic phase appeared from 52.89 °C to 47.41 °C to show linearly decreasing behaviors because PG affects the hydrophobic region of DSPC-based lamella phase. The repeating distance of the lamella phase and the interlayer distance between bilayers were calculated with XRDs and the average number of bilayers related to the thickness in LC structure was approximately estimated by combining with TEM results. The WAXS and DSC measurements showed that all of PG molecules contributed to swelling both the lipid layer in the edge region of lamella phase close to phosphate groups and the interlayer between bilayers below 90% w/w of PG. The phase and thermal behaviors were found to depend on the amount of PG used by means of dissolving DSPC as a phospholipid and rearranging its structure. Instead of water, the inducement of PG as a polar solvent in solid-lamella phase is discussed in terms of the swelling effect of PG for DSPC-based lamella membrane.

• Nuclear Engineering and Technology
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• 제55권12호
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• pp.4637-4641
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• 2023

For nuclear decommissioning applications, a study was conducted to investigate the feasibility of using a laser for long-distance cutting in complex structures. Cutting tests were performed on stainless steel plates with thicknesses ranging from 10 mm to 30 mm at distances of 300 mm-700 mm from the laser head, using a laser power of 6 kW. Remarkably, the 10 mm and 20 mm thick stainless-steel plates were successfully cut at a distance of 700 mm from the head. Based on the trends observed in the results, it is anticipated that these thicknesses could also be cut at distances of approximately 1 m. Similarly, the 30 mm thick stainless-steel plate was effectively cut at a distance of 500 mm from the head. To evaluate the amount of secondary waste generated, the kerf width was measured. Due to the long-distance cutting, the average kerf width ranged from 6 mm to 16 mm. Despite the wider kerf width, long-distance cutting holds promise for efficiently handling hard-to-reach targets in nuclear decommissioning scenarios.

• 한국수소및신에너지학회논문집
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• 제28권2호
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• pp.166-173
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• 2017

For commercialization of hydrogen refuelling station (HRS), we need to reduce the clearance distance for jet fire in the real entities in the HRS. Thus, we revisited the current regulations of clearance distance for jet fire in the law. The law in korea has been set up by replica of japan, not by our own scientific basis. Recently, sandia lab developed Hydrogen Risk Assessment Model (HyRAM) tools and we simulated a series of circumstances such as 10 to 850 bar with several leak hole sizes. In 850 bar with 10 mm diameter hole leak cases, it shows $4,981kW/m^2$ at 12 m separation from leak source and $1,774kW/m^2$ at 17 m separation from leak source. In 850 bar with 1 mm diameter leak hole, it shows $0.102kW/m^2$ at 12 m separation and $0.044kW/m^2$ at 17 m separation. Current law may be acceptable with 1 mm hole size with 850 bar.

• 화약ㆍ발파
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• 제8권1호
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• pp.3-16
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• 1990

The cautious blasting works had been used with emulsion explosion electric M/S delay caps. Drill depth was from 3m to 6m with Crawler Drill $\varphi{70mm}$ on the calcalious sand stone(sort-moderate-semi hard Rock). The total numbers of feet blast were 88. Scale distance were induces 15.52-60.32. It was applied to propagation Law in blasting vibration as follows. Propagtion Law in Blasting Vibration $V=K(\frac{D}{W^b})^n$ where V : Peak partical velocity(cm/sec) D : Distance between explosion and recording sites (m) W : Maximum Charge per delay-period of eighit milliseconds or more(Kg) K : Ground transmission constant, empirically determind on th Rocks, Explosive and drilling pattern ets. b : Charge exponents n : Reduced exponents Where the quantity $D/W^b$ is known as the Scale distance. Above equation is worked by the U.S Bureau of Mines to determine peak particle velocity. The propagation Law can be catagrorized in three graups. Cabic root Scaling charge per delay Square root Scaling of charge per delay Site-specific Scaling of charge per delay Charge and reduction exponents carried out by multiple regressional analysis. It's divided into under loom and over loom distance because the frequency is verified by the distance from blast site. Empirical equation of cautious blasting vibration is as follows. Over 30m----under l00m----- $V=41(D/3\sqrt{W})^{-1.41}$ -----A Over l00m-----$V= 121(D/3\sqrt{W})^{-1.66}$-----B K value on the above equation has to be more specified for furthur understang about the effect of explosives, Rock strength. And Drilling pattern on the vibration levels, it is necessary to carry out more tests.

• 화약ㆍ발파
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• 제9권4호
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• pp.3-12
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• 1991

The cautious blasting works had been used with emulsion explosion electric M /S delay caps. Drill depth was from 3m to 6m with Crawler Drill 70mm on the calcalious sand stone (soft-moderate-semi hard Rock) . The total numbers of feet blast were 88. Scale distance were induces 15.52-60.32. It was applied to Propagation Law in blasting vibration as follows .Propagtion Law in Blasting Vibration V=k(D/W/sup b/)/sup n/ where V : Peak partical velocity(cm/sec) D : Distance between explosion and recording sites(m) W ; Maximum Charge per delay -period of eight milliseconds or more(Kg) K : Ground transmission constant, empirically determind on the Rocks, Explosive and drilling pattern ets. b : Charge exponents n : Reduced exponents Where the quantity D/W/sup b/ is known as the Scale distance. Above equation is worked by the U.S Bureau of Mines to determine peak particle velocity. The propagation Law can be catagrorized in three groups. Cabic root Scaling charge per delay Square root Scaling of charge per delay Site-specific Scaling of charge delay Charge and reduction exponents carried out by multiple regressional analysis. It's divided into under loom and over loom distance because the frequency is varified by the distance from blast site. Empirical equation of cautious blasting vibration is as follows. Over 30m--under 100m----V=41(D/ W)/sup -1.41/-----A Over l00m---------V=121(D/ W)/sup -1.56/-----B K value on the above equation has to be more specified for furthur understand about the effect of explosives. Rock strength, And Drilling pattern on the vibration levels, it is necessary to carry out more tests.

• 대한수학회보
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• 제55권1호
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• pp.115-137
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• 2018

Let $R_{u{^2},v^2,w^2,p}$ be a finite non chain ring ${\mathbb{F}}_p[u,v,w]{\langle}u^2,\;v^2,\;w^2,\;uv-vu,\;vw-wv,\;uw-wu{\rangle}$, where p is a prime number. This ring is a part of family of Frobenius rings. In this paper, we explore the structures of cyclic codes over the ring $R_{u{^2},v^2,w^2,p}$ of arbitrary length. We obtain a unique set of generators for these codes and also characterize free cyclic codes. We show that Gray images of cyclic codes are 8-quasicyclic binary linear codes of length 8n over ${\mathbb{F}}_p$. We also determine the rank and the Hamming distance for these codes. At last, we have given some examples.

• 한국축산시설환경학회지
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• 제14권3호
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• pp.159-166
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• 2008

본 연구의 목적은 현재 일본 마루야마에서 재발된 방제기의 최대 살포 거리가 120 m 이기 때문에 140 m 이상 살포할 수 있는 방제기를 개발하는 것이다. 넓은 지역에 살포가 가능한 광역방제기 팬의 성능에 대하여 현장실험을 하여 얻은 데이터를 영상처리하여 분석한 후 현장에 보급하는 것이다. 살포된 색소의 분포도는 육안에 의한 분석을 할 수도 있지만 정확하고 신뢰도를 높이기 위해 영상처리를 이용하여 이치화 하였다. 연구에 사용된 방제기 팬은 최고 살포거리가 140 m이고 유효 살포거리가 100 m가 되도록 설계 및 제작되었다. 실험은 10 m 간격으로 지상에서 1 m 위치에 A4 용지를 부착한 후 용지에 흡착한 용액을 2치화 영상처리를 하여 살포량 및 살포거리를 측정하였다. 용지를 수거하여 영상처리를 이용하여 이치화 하였다. 그레이레벨은 0에서 255로 나타냈다. 흑색은 0, 백색은 255로 이치화 하였다. 10 m의 경우는 용지에 방제액의 살포량이 많아서 떨어졌고, 30 m 부분은 색소가 흘러내려 흑색이 적게 나타난 것으로 판단된다. $20{\sim}100m$까지 그레이레벨이 200 이하로 방제가 균등하게 이루어졌으며, 180 m까지 살포가 가능한 것으로 나타났다. 실험을 통하여 축산농가의 구제역 등 방제작업에 이용이 가능할 것으로 판단된다.

• 한국전기전자재료학회논문지
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• 제36권3호
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• pp.261-265
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• 2023

In this paper, we analyzed the transformation of the power following by the angle of incidence of the solar, the angle of photovoltaic module and artificial solar changed from 30° to 90° and synchronously changed the distance from 0.1 m to 0.5 m. Setting the distance between the artificial solar and the luminometer from 0.1 m to 0.5 m and set the angles to 90°, 60°, 45°, and 30°, the angle was 90° and when the distance was 0.1 m, the maximum Illuminance was 19,580 lux, the light could be obtained more. If the angle of incidence between the Artificial solar and the photovoltaic module was 90° and the variable resistance was 1,000 Ω at a distance of 0.4 m, the maximum power reached 0.82 W. Provided that the angle of incidence between the artificial solar and the photovoltaic module was 90° and the distance was 0.2 m since the variable resistance had the maximum power of 500 Ω, the maximum power was 0.78 W. At 1,000 Ω, the maximum power is 0.80 W so the maximum power at the variable resistance 1,000 Ω could obtain higher power than the variable resistance 500 Ω. The variable resistance was 1,000 Ω and the angle of incidence between the Artificial solar and the photovoltaic module was 90° at a distance of 0.4 m, and the maximum power reached 0.82 W. The angle was 60° at 0.3 m and 0.4 m the maximum power reached 0.10 W. The angle was 45° at 0.2 m maximum power reached 0.020 W, the angle was 30° at 0.4 m, and the maximum power reached 0.004 W. In four results about maximum power depending on the angle of incidence between the artificial solar and the photovoltaic module, the luminous efficiency and maximum power can be got the best at an angle of 90°.

• 한국콘텐츠학회논문지
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• 제12권2호
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• pp.105-115
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• 2012

본 논문에서는 휴대폰 카메라를 통해 간판영상의 한글문자를 인식한 후 오인식 된 결과를 교정하는 방법으로 인식 후보를 음소단위 분할하고 연산 가중치를 적용한 weighted Disassemble Levenshtein Distance(wDLD)를 제안한다. 제안된 방법은 인식된 문자열을 음소 단위로 분할한 후 입력 형태의 거리값을 산출하여, 가장 유사한 상호명을 데이터베이스에서 검출 한다. 제안된 방법의 효율성을 검증하기 위해, 전국의 상호명 중 중복되는 상호명을 제거한 130만개의 상호명을 이용하여 데이터베이스 사전을 구축하였다. 또한 대표적인 문자열 비교 알고리즘인 Levenshtein Distance와 음소를 분할하여 적용한 Disassemble Levenshtein Distance 방법, 그리고 본 논문에서 제안한 인식 후보의 음소 단위 분할 방법과 연산 가중치를 적용한 weighted Disassemble Levenshtein Distance의 교정율을 비교 분석 하였다. 그 결과 제안된 weighted Disassemble Levenshtein Distance(wDLD)은 Levenshtein Distance와 Disassemble Levenshtein Distance방법에 비해 각각 평균 29.85%와 6%의 인식률의 향상을 보였다.