• 한국멀티미디어학회논문지
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• 제3권2호
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• pp.174-183
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• 2000

시스템 수준의 프로토콜 명세를 위한 정형 기법들은 S/W 구현에 중심을 둔 반면, 성능의 향상을 위해서 프로토콜의 설계를 H/W로 구현하는 것에 대한 필요성이 증대되고 있다. 따라서, 특정한 프로토콜을 이용한 시스템의 S/W적 구현에서 H/W적 구현으로 기반 환경이 변화함에 따라 IP(Integrated Processing)기술의 도입이 필요하게 되었다. 또한, 정형 명세로부터 시작하는 H/W의 구현 방법은 정형 명세의 특성에 의해, 구현된 H/W의 정확성, 신뢰성을 보장할 수 있다. 본 논문에서는 형식기술기법중의 하나인 ESTELLE로 정형화된 프로토콜을 H/W언어인 VHDL로 변환하는 방법을 제시한다. 우선 ESTELLE 명세를 VHDL 명세로 변환하는 변환방법을 기술한다. 이는 개념적인 변환방법으로 프로토콜 명세화의 기본 단위인 computation unit과 communication unit의 동작과 H/W에서의 프로세스간 동작의 유사성 등을 비교 분석하였다. 그 후 변환 모델을 기술하고, Inres 프로토콜을 통하여 실제로 ESTELLE을 VHDL로 변환하는 예를 제시한다.

• 천문학회지
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• 제27권1호
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• pp.81-102
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• 1994

We have decomposed the 11-cm radio continuum emission of the W51 complex into thermal and non-thermal components. The distribution of the thermal emission has been determined by analyzing HI, CO, and IRAS $60-{\mu}m$ data. We have found a good correlation between the 11-cm thermal continuum and the 60- 11m emissions, which is used to obtain the thermal and non-thermal 11-cm continuum maps of the W51 complex. Most of the thermal continuum is emanating from the compact H II regions and their low-density ionized envelopes in W51A and W51B. All the H II regions, except G49.1-0.4 in W51B, have associated molecular clumps. The thermal radio continuum fluxes of the compact H II regions are proportional to the CO fluxes of molecular clumps. This is consistent with the previous results that the total mass of stars in an H II region is proportional to the mass of the associated molecular clump. According to our result, there are three non-thermal continuum sources in W51: G49.4-0.4 in W51A, a weak source close to G49.2-0.3 in W51B, and the shell source W51C. The non-thermal flux of G49.5-0.4 at 11-cm is $\~28 Jy$, which is $\~25\%$ of its total 11-cm flux. The radio continuum spectrum between 0.15 and 300 GHz also suggests an excess emission over thermal free-free emission. We show that the excess emission can be described as a non-thermal emission with a spectral index ${\alpha}{\simeq}-1.0 (S_v{\propto}V^a)$ attenuated by thermal free-free absorptions at low-frequencies. The non-thermal source close to G49.2-0.3 is weak $(\~9 Jy)$. The nature of the source is not known and the reality of the non-thermal emission needs to be confirmed. The non~thermal shell source W51C has a 11-cm flux of $\~130Jy$ and a spectral index ${\alpha}{\simeq}-0.26$.

• 한국산학기술학회논문지
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• 제19권3호
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• pp.669-678
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• 2018

본 연구는 차량센싱데이터, 공공데이터 등 다종의 빅데이터를 활용하여 주행환경 분석 플랫폼 구축을 위한 정보기술 인프라를 개발하였다. 정보기술 인프라는 H/W 기술과 S/W 기술로 구분할 수 있다. 먼저, H/W 기술은 빅데이터 분산 처리를 위한 병렬처리 구조의 소형 플랫폼 서버를 개발하였다. 해당 서버는 1대의 마스터 노드와 9대의 슬래이브 노드로 구성하였으며, H/W 결함에 따른 데이터 유실을 막기 위하여 클러스터 기반 H/W 구성으로 설계하였다. 다음으로 S/W 기술은 빅데이터 수집 및 저장, 가공 및 분석, 정보시각화를 위한 각각의 프로그램을 개발하였다. 수집 S/W의 경우, 실시간 데이터는 카프카와 플럼으로 비실시간 데이터는 스쿱을 이용하여 수집 인터페이스를 개발하였다. 저장 S/W는 데이터의 활용 용도에 따라 하둡 분산파일시스템과 카산드라 DB로 구분하여 저장하는 인터페이스를 개발하였다. 가공 S/W는 그리드 인덱스 기법을 적용하여 수집데이터의 공간 단위 매칭과 시간간격 보간 및 집계를 위한 프로그램을 개발하였다. 분석 S/W는 개발 알고리즘의 탐재 및 평가, 장래 주행환경 예측모형 개발을 위하여 제플린 노트북 기반의 분석 도구를 개발하였다. 마지막으로 정보시각화 S/W는 다양한 주행환경 정보제공 및 시각화를 위하여 지오서버 기반의 웹 GIS 엔진 프로그램을 개발하였다. 성능평가는 개발서버의 메모리 용량과 코어개수에 따른 연산 테스트를 수행하였으며, 타 기관의 클라우드 컴퓨팅과도 연산성능을 비교하였다. 그 결과, 개발 서버에 대한 최적의 익스큐터 개수, 메모리 용량과 코어 개수를 도출하였으며, 개발 서버는 타 시스템 보다 연산성능이 우수한 것으로 나타났다.

• 대한수학회논문집
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• 제22권1호
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• pp.65-74
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• 2007

Suppose that $\mu$ is a finite positive Borel measure on bounded symmetric domain $\Omega{\subset}\mathbb{C}^n\;and\;\nu$ is the Euclidean volume measure such that $\nu(\Omega)=1$. Suppose 1 < p < $\infty$ and r > 0. In this paper, we will show that the norms $sup\{\int_\Omega{\mid}k_z(w)\mid^2d\mu(w)\;:\;z\in\Omega\}$, $sup\{\int_\Omega{\mid}h(w)\mid^pd\mu(w)/\int_\Omega{\mid}h(w)^pd\nu(w)\;:\;h{\in}L_a^p(\Omega,d\nu),\;h\neq0\}$ and $$sup\{\frac{\mu(E(z,r))}{\nu(E(z,r))}\;:\;z\in\Omega\}$$ are are all equivalent. We will also show that the inclusion mapping $ip\;:\;L_a^p(\Omega,d\nu){\rightarrow}L^p(\Omega,d\mu)$ is compact if and only if lim $w\rightarrow\partial\Omega\frac{\mu(E(w,r))}{\nu(E(w,r))}=0$.

• 충청수학회지
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• 제27권4호
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• pp.697-705
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• 2014

For a complex measure ${\mu}$ on B and $f{\in}L^2_a(B)$, the Toeplitz operator $T_{\mu}$ on $L^2_a(B,dv)$ with symbol ${\mu}$ is formally defined by $T_{\mu}(f)(w)=\int_{B}f(w)\bar{K(z,w)}d{\mu}(w)$. We will investigate properties of the Toeplitz operator $T_{\mu}$ with symbol ${\mu}$. We define the Toeplitz type operator $T^r_{\psi}$ with symbol ${\psi}$, $$T^r_{\psi}f(z)=c_r\int_{B}\frac{(1-{\parallel}w{\parallel}^2)^r}{(1-{\langle}z,w{\rangle})^{n+r+1}}{\psi}(w)f(w)d{\nu}(w)$$. We will also investigate properties of the Toeplitz type operator with symbol ${\psi}$.

• 한국태양에너지학회 논문집
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• 제25권1호
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• pp.27-34
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• 2005

This study aims to evaluate application of a heat recovery ventilator(HRV) using photovoltaic(PV) system. To this end, we analyzed performance of a PV system, which it was evaluated by monthly power wattage and conversion efficiency according to design capacity of a HRV. The results of this study can be summarized as follows. (1) A conversion efficiency of the PCS was evaluated about 86% in rated power. (2) A maximum, minimum and average output power were respectively analyzed 49.2W, 47.3W, and 48.8W. (3) Total power wattage of 200W PV system was 211kW and it was 316kW in case of 300W PV system. (4) Insufficient electrical power of a duct and window type ventilation system was respectively calculated 133.5kW and 147.7kW.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2005년도 제36회 하계학술대회 논문집 B
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• pp.1681-1683
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• 2005

The molten carbonate fuel tell(MCFC) is endowed with the high potential especially in future electric power generation industry by its own outstanding characteristics. KEPCO(KEPRI) started a 100 kW MCFC system development program in 1993 and has been executed 100kW system develpilot plant successfully completed first phaseopment by 2005 on the basis of successful results of 25kW system development. In this program, the components and mechanical structure for 100 kW stack and system construction were completed on last year and now system pre-commissioning was being executed. A 100 kW MCFC power plant was constructed at the site of Boryeong Thermal Power Plant. A 100 kW MCFC system has characterized as a high pressure operation mode, $CO_2$ recycle, and externally reforming power generation system. The 100 kW MCFC system consisted with stacks which was made by two 50 kW sub-stacks, 90 cells with 6,000 cm2 active area and BOP including a reformer, a recycle blower, a catalytic burner, an inverter, and etc. The system will be operated under 3 atm pressure condition and expected to last over 5,000 hours by the end of this year.

• 한국수학교육학회지시리즈B:순수및응용수학
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• 제11권3호
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• pp.207-215
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• 2004

Let W(z) be a power series with operator coefficients such that multiplication by W(z) is contractive in extC(z). The overlapping space $\varepsilon$(W) of D(W) in C(z) is a Herglotz space with Herglotz function $\varphi$(z) which satisfies $\varphi$(z) + ${\varphi}^*(z^{-1})$ = 2[1-W$^*(z^{-1})W(z)]$.

• Journal of applied mathematics & informatics
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• 제40권3_4호
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• pp.507-513
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• 2022

In this paper, we investigate some results on complex delay-differential equations of the classical Malmquist theorem. A classic illustrations of their results states us that if a complex delay equation w(t + 1) + w(t - 1) = R(t, w) with R(t, w) rational in both arguments admits (concede) a transcendental meromorphic solution of finite order, then deg_wR(t, w) ≤ 2. Development and upgrade of such results are presented in this paper. In addition, Borel exceptional zeros and poles seem to appear in special situations.

• 수산해양기술연구
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• 제34권3호
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• pp.302-308
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• 1998

The author examined the response of Yoroi-mebaru, Sebastes hubbsi [MATSUBARA] to the underwater attracting lamps (0.5 W, 0.8 W, 1 W) line in the experimental water tank (550 L x 58 W x 73 H cm). The attracting rate investigated in accordance with the intervals of lighting and putting out hour (1, 5 minutes) when each of the underwater attracting lamps was gradually switched off after they were switched on all at once. The results are a follows: 1. Distribution rates of fish in the illuminated area was 35.7 % in case of 1 minute interval, and 50.3 % in case of 5 minutes interval. 2. Mean distribution rate of fish at the illuminated section: \circled1 Distribution rates at interval of 1 minute were 9.8 % in 1 W, 6.5 % in 0.8 W and 5.1 % in 0.5 W, respectively. \circled2 Distribution rates at interval of 5 minutes were 15.6 % in 1 W, 8.5 % in 0.5 W and 6.1 % in 0.8 W, respectively. 3. Attracting rates of the last section showed a little increasing as illuminating time elapsed. A difference of attracting rates according to lighting source in 5 minutes interval were bigger than that in 1 minute interval. 4. Attracting rates of fish in only last section switched on: \circled1 Attracting rates at interval in case of 1 minute were 30.0 % in 0.8 W, 16.0 % in 1 W and 8.0 % in 0.5 W, respectively. \circled2 Attracting rates at interval in case of 5 minutes were 56.0 % in 1 W, 30.7 % in 0.5 W and 10.7 % in 0.8 W. respectively.