• 한국수산과학회지
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• 제34권6호
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• pp.624-631
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• 2001

오징어 채낚기 어선의 집어등을 점등한 상태에서의 오징어 군을 어군 탐지기에 의해 관찰하고, 어선 양현의 조획기에 설치된 낚시의 도달 심도를 달리하여 광원 출력 조건별로 조획 시험을 실시하여 어군의 분포 심도를 추정하는 한편 수심별 수중 조도를 측정함으로써 어군이 밀집하여 분포하고 있는 조획 심도에서의 광 환경에 대해서 검토하였다 집어등 점등시 어군 탐지기에 나타난 어군은 낚시 어구 주위를 중심으로 수심 50m까지의 얕은 곳에서 높은 밀도의 반응을 보였으나, 시간이 경과함에 따라 어군 층은 침하하여 수심 $60\~80m$사이에서 안정되었다. 어선의 각 현별 낚시 최선단의 도달 심도를 변화시킨 경우의 조획량은 심도를 90m로 설정한 현측이 60m로 설정한 현보다 많았으나, 조획이 적어진 해뜰 무렵에 광원 출력을 할로겐등 24kW로 절환하여 조업한 후에는 60m 충에서 조획 증가 경향이 현저하게 나타났다. 어군 탐지기와 조획 시험에서 추정된 오징어의 중요한 조획층으로 사료되는 수심 $60\~80m$에서의 수중 조도는 각 광원 출력별 평균 $3.0\times10^{-2}\sim\;3.4\times10^{-2}lx$의 범위에서 분포하였다.

• 천문학회지
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• 제48권4호
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• pp.213-228
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• 2015

The Horizon Run 4 is a cosmological N-body simulation designed for the study of coupled evolution between galaxies and large-scale structures of the Universe, and for the test of galaxy formation models. Using 6300³ gravitating particles in a cubic box of L_box = 3150 h⁻¹Mpc, we build a dense forest of halo merger trees to trace the halo merger history with a halo mass resolution scale down to M_s = 2.7 × 10¹¹h⁻¹M_⊙. We build a set of particle and halo data, which can serve as testbeds for comparison of cosmological models and gravitational theories with observations. We find that the FoF halo mass function shows a substantial deviation from the universal form with tangible redshift evolution of amplitude and shape. At higher redshifts, the amplitude of the mass function is lower, and the functional form is shifted toward larger values of ln(1/σ). We also find that the baryonic acoustic oscillation feature in the two-point correlation function of mock galaxies becomes broader with a peak position moving to smaller scales and the peak amplitude decreasing for increasing directional cosine μ compared to the linear predictions. From the halo merger trees built from halo data at 75 redshifts, we measure the half-mass epoch of halos and find that less massive halos tend to reach half of their current mass at higher redshifts. Simulation outputs including snapshot data, past lightcone space data, and halo merger data are available at http://sdss.kias.re.kr/astro/Horizon-Run4.

• 대한원격탐사학회지
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• 제36권5_2호
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• pp.949-959
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• 2020

본 논문에서는 CAS500-1/2를 이용한 산출물 생성에 관련한 선행연구로 KOMPSAT-3A 스트립영상을 사용한 비접근 지역의 도엽별 DSM을 생성하는 방법을 제안한다. 제안 기법은 1:5000 도엽정보의 입력을 통한 영역 설정을 통해 도엽별로 산출물이 나올 수 있도록 설계됐으며, 강인한 스테레오 영상정합 기법인 MDR을 적용하여 스테레오 페어에서도 최적의 DSM이 나오도록 설정했다. 스트립 영상이 분할된 여러 장의 단위 영상으로 들어오는 것을 고려하여 하나의 도엽에 여러 쌍의 영상 페어를 처리하여 통합하는 방식으로 DSM의 생성을 시도했으며, 처리결과 도엽 간의 접합부분에서 이격 발생을 최소화한 DSM의 생성이 가능함을 확인할 수 있었다. 최종적으로 GCP와의 비교를 통한 정확도 검증결과 5 m 이내의 정확도가 나타나는 것을 확인할 수 있었다.

• Earthquakes and Structures
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• 제24권4호
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• pp.289-301
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• 2023

Developing a competent soil-bridge interaction model for the seismic analysis of piled foundation bridges is of utmost importance for investigating the seismic response and assessing fragility of these lifeline structures. To this end, ground motion histories are deemed necessary at various depths along the piles supporting the bridge. This may be effectively accomplished through time history analysis of a free-field standalone soil column extending from bedrock level to ground surface subjected to an input bedrock motion at its base. A one-dimensional site/ground response analysis (vide one-directional shear wave propagation through the soil column) is hence conducted in the present research accounting for the nonlinear hysteretic behavior of the soil stratum encompassing the bridge piled foundation. Two homogeneous soil profiles atop of bedrock have been considered for comparison purposes, namely, loose and dense sand. Analysis of the standalone soil column has been performed under a set of ten selected actual bedrock ground motions adopting a nonlinear time domain approach in an incremental dynamic analysis framework. Amplified retrieved PGA and maximum soil shear strains have been generally observed at various depths of the soil column when moving away from bedrock towards ground surface especially at large hazards associated with high (input) PGA values assigned at bedrock. This has been accompanied, however, by some attenuation of the amplified PGA values at shallower depths and at ground surface especially for the loose sand soil and particularly for cases with higher seismic hazards associated with large scaling factors of bedrock records.

• Nuclear Engineering and Technology
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• 제39권5호
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• pp.603-616
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• 2007

Roy Huddle, having invented the coated particle in Harwell 1957, stated in the early 1970s that we know now everything about particles and coatings and should be going over to deal with other problems. This was on the occasion of the Dragon fuel performance information meeting London 1973: How wrong a genius be! It took until 1978 that really good particles were made in Germany, then during the Japanese HTTR production in the 1990s and finally the Chinese 2000-2001 campaign for HTR-10. Here, we present a review of history and present status. Today, good fuel is measured by different standards from the seventies: where $9*10^{-4}$ initial free heavy metal fraction was typical for early AVR carbide fuel and $3*10^{-4}$ initial free heavy metal fraction was acceptable for oxide fuel in THTR, we insist on values more than an order of magnitude below this value today. Half a percent of particle failure at the end-of-irradiation, another ancient standard, is not even acceptable today, even for the most severe accidents. While legislation and licensing has not changed, one of the reasons we insist on these improvements is the preference for passive systems rather than active controls of earlier times. After renewed HTGR interest, we are reporting about the start of new or reactivated coated particle work in several parts of the world, considering the aspects of designs/ traditional and new materials, manufacturing technologies/ quality control quality assurance, irradiation and accident performance, modeling and performance predictions, and fuel cycle aspects and spent fuel treatment. In very general terms, the coated particle should be strong, reliable, retentive, and affordable. These properties have to be quantified and will be eventually optimized for a specific application system. Results obtained so far indicate that the same particle can be used for steam cycle applications with $700-750^{\circ}C$ helium coolant gas exit, for gas turbine applications at $850-900^{\circ}C$ and for process heat/hydrogen generation applications with $950^{\circ}C$ outlet temperatures. There is a clear set of standards for modem high quality fuel in terms of low levels of heavy metal contamination, manufacture-induced particle defects during fuel body and fuel element making, irradiation/accident induced particle failures and limits on fission product release from intact particles. While gas-cooled reactor design is still open-ended with blocks for the prismatic and spherical fuel elements for the pebble-bed design, there is near worldwide agreement on high quality fuel: a $500{\mu}m$ diameter $UO_2$ kernel of 10% enrichment is surrounded by a $100{\mu}m$ thick sacrificial buffer layer to be followed by a dense inner pyrocarbon layer, a high quality silicon carbide layer of $35{\mu}m$ thickness and theoretical density and another outer pyrocarbon layer. Good performance has been demonstrated both under operational and under accident conditions, i.e. to 10% FIMA and maximum $1600^{\circ}C$ afterwards. And it is the wide-ranging demonstration experience that makes this particle superior. Recommendations are made for further work: 1. Generation of data for presently manufactured materials, e.g. SiC strength and strength distribution, PyC creep and shrinkage and many more material data sets. 2. Renewed start of irradiation and accident testing of modem coated particle fuel. 3. Analysis of existing and newly created data with a view to demonstrate satisfactory performance at burnups beyond 10% FIMA and complete fission product retention even in accidents that go beyond $1600^{\circ}C$ for a short period of time. This work should proceed at both national and international level.