• 한국해양학회지:바다
• /
• 제26권2호
• /
• pp.96-109
• /
• 2021

담수를 통해 유입되는 육상 기원 물질은 연안 일차 생산을 제어하는 주요 요소이므로 육상-해양 coupling을 파악하는 것은 연안 생태 변화를 이해하는데 중요하다. 본 논문에서는 육상-해양 coupling 양상을 시간에 따라 세 단계(Base flow, Plume event, Residual flow)로 구분하여 개념화하였고, 낙동강 하구에서 각 양상의 출현을 확인하기위해 다양한 플랫폼에서 측정된 자료를 사용하여 분석하였다. 사용된 자료는 원격 탐사 측정 자료(Geostationary Ocean Color Image; GOCI), 현장 실측 자료(Marine Environment Information System; MEIS), 연속 측정 자료(유량 자료, 기상 자료)로 구분될 수 있다. 주성분분석을 통해 MEIS 자료를 육상-해양 coupling의 세 단계로 구분하였고, 이 구분을 2013-2018년 동안의 여타 자료에 적용하여 단기간 육상-해양 coupling 양상을 살펴보았다. 낙동강 하구에서는 예상과는 달리 Plume event때 Chlorophyll-a (Chl-a) 최대값이 나타났다. 이는 담수 증가에도 탁도 증가는 크지 않았고, 플러싱 효과도 약해 식물플랑크톤이 증가 할 수 있는 여건이 조성되었기 때문으로 분석되었다. 육상-해양 coupling을 기반으로 여러 하구들과 비교해보았을 때 육상-해양 coupling은 담수 유입에 영향을 받는 하구에서 흔한 현상이나 하구에서 형성되는 플룸 크기에 따라 육상-해양 coupling이 다르게 나타났다. 낙동강 하구처럼 작은 플룸(~10 km 규모) 이 형성되는 하구에서는 식물플랑크톤의 즉각적인 반응으로 인해 Plume event 단계에 Chl-a 최댓값이 나타나는 반면, ~100 km 이상의 큰 플룸이 형성되는 하구(담수 배출이 크고, 플러싱이 강한 곳)에서는 본 연구에서 개념화한 육상-해양 coupling 양상(Residual flow 때 Chl-a 최대)을 따르는 것으로 나타났다.

• 한국전자파학회논문지
• /
• 제14권1호
• /
• pp.20-26
• /
• 2003

본 논문에서는 접지면에 어퍼쳐를 갖는 hairpin-comb 대역 통과 여파기를 제안하였다. Hairpin-comb 공진기는 두 공진기 사이의 간격이 매우 좁더라도 약한 커플링을 유지하는 특성이 있으므로 협대역 대역통과 여파기 제작시 여파기의 전체적인 크기를 작게 할 수 있는 장점이 있다. 그러나 일반적인 마이크로 스트립에서는 공진기 사이가 최소한의 거리가 되더라도 커플링이 너무 미약하여 사용할 수 없다. 그러므로 본 논문에서는 접지면에 어퍼쳐를 사용하여 약한 커플링을 보상함으로써 일반 마이크로 스트립에서도 협대역 대역통과 여파기를 제작할 수 있었다. 또한 공진기 사이의 거리 변환 없이 어퍼쳐의 크기에 의해서 커플링을 조절함으로써 전체 여파기의 크기를 고정시킨 상태에서 대역폭을 조절할 수 있는 장점이 있다. 본 논문에서는 중심 주파수가 1.78 GHz이고 대역폭이 62 MHz(3.5%)인 여파기를 제작하였다.

• Interaction and multiscale mechanics
• /
• 제1권4호
• /
• pp.449-465
• /
• 2008

In this paper a general approach for studying the motion of a cantilever beam interacting with a 2D fluid flow is presented. The fluid is solved by a general purpose commercial computational fluid dynamics (CFD) package (FLUENT 6.2), while the structure is managed by means of a dedicated finite element method solver, coded in FLUENT as a user-defined function (UDF). A weak fluid structure interaction coupling scheme is adopted exchanging information at the end of each time step. An arbitrary cantilever beam can be introduced in the CFD mesh with its wetted boundaries specified; the cantilever can also interact with specified rigid and flexible walls through use of a non-linear contact algorithm. After a brief review of relevant scientific contributions, some test cases and application examples are presented.

• Bulletin of the Korean Chemical Society
• /
• 제21권10호
• /
• pp.969-972
• /
• 2000

[Fe II Fe III $BPLNP(OAc)_2](BPh_4)_2$ (1), a new model for the reduced form of the purple acid phosphatases, has been synthesized by using a dinucleating ligand, 2,6-bis[((2-pyridylmethyl)(6-methyl-2-pyridylmethyl)ami-no)methyl]-4-nitrophenol (HBPLNP) . Complex 1 has been studied by electronic spectral, NMR, EPR, SQUID, and electrochemical methods. Complex 1 exhibits two strong bands at 498 nm $(\varepsilon=$ 2.6 ${\times}10^3M-^1cm-^1)$ and 1363 nm $(\varepsilon=$ 5.7 ${\times}10^2M-^1cm-^1)$ in $CH_3CN.$ These are assigned to phenolate-to-FeIII and intervalence charge-transfer transitions, respectively. NMR spectrum of complex 1 exhibits sharp isotropically shifted resonances, which number is half of those expected for a valence-trapped species, indicating that electron transfer between FeⅡ and FeⅢ centers is faster than NMR time scale at room temperature. Complex 1 undergoes quasireversible one-electron redox processes. The $FeIII_2/FeIIFeIII$ and $FeIIFeIII/FeII_2$ redox couples are at 0.807 and 0.167 V ver-sus SCE, respectively. It has Kcomp = 5.9 ${\times}$10 1s(acetato) ligand combination sta-bilizes a mixed-valence FeIIFeIII complex in the air. Interestingly, complex 1 exhibits intense EPR signals at g = 8.56, 5.45, 4.30 corresponding to mononuclear high-spin FeⅢ species, which suggest a very weak magnetic coupling between the iron centers. Magnetic susceptibility study shows that there is a very weak antiferromag-netic coupling (J = $-0.78cm-^1$, H = $-2JS_1${\times}$S_2)$ between FeII and FeIII centers. Thus, we can suggest that complex 1 has a very weak antiferromagnetic coupling between the iron centers due to the electronic effect of the nitro group in the bridging phenolate ligand.

• Progress in Superconductivity
• /
• 제1권1호
• /
• pp.1-8
• /
• 1999

The magnetization and/or resistivity of high $T_c$ superconductors ($YBa_2Cu_3O_{7-\delta}$(YBCO) single crystal, $Bi_2Sr_2CaCu_2O_8$ (Bi-2212) single crystal, $Tl_2Ba_2CaCu_2O_8$ (Tl-2212) film, $HgBa_2Ca_2Cu_3O_8$ (Hg-1223) film) have been measured as a function of magnetic field H and temperature T. The extracted fluctuation part of the magnetization and conductivity exhibits a critical behavior consistent with the three-dimensional XY model. The dynamic critical exponent z does not sensitively vary with a type of the superconductors. The value of z ranges from 1.5 to $1.8{\pm}0.1$. However, the static critical exponent ${\nu}$ is the most largely increased in Tl-2212 that has a weaker interlayer coupling strength than YBCO; the value of ${\nu}$ is 0.669, 0.909, 1.19, and 1.338 for YBCO, Bi-2212, Hg-1223, and Tl-2212 respectively. The results indicate that the weak interlayer coupling along the c-axis of high $T_c$ superconductors near $T_c$ does not influence the dynamic critical exponent z (the same value of superfluid $^4He$), but significantly increases the static critical exponent ${\nu}$.

• 대한전자공학회논문지TC
• /
• 제47권10호
• /
• pp.67-73
• /
• 2010

유한한 기판 크기가 H-평면상에 배열된 두 개의 패치안테나간의 상호결합 특성에 미치는 영향에 대하여 연구하였다. 표면파의 여러 가지 이동경로에 따른 위상차에 의한 간섭 효과를 이용하여 표면파를 서로 상쇄시켜 상호결합을 작게 할 수 있다. 유전상수가 10 이고 기판 두께가 3.2 mm 인 경우 패치안테나 중심 간의 거리가 0.5 $_0$에서 1.0 $\lambda_0$로 두 배 증가할 때, 상호 결합이 큰 기판 크기에서는 상호결합이 4.85 dB 감소하나 최적화된 기판 크기에서는 상호결합이 34.28 dB 감소한다. 최적화된 기판 크기에서 패치안테나 중심 간의 거리 증가에 따른 상호결합 감소율이 매우 큼을 볼 수 있었다. 이미지 방법으로 계산한 최적화된 기판 크기와 전산모의 결과로 얻어진 최적화된 기판 크기가 잘 일치하였다.

• Bulletin of the Korean Chemical Society
• /
• 제26권12호
• /
• pp.1965-1968
• /
• 2005

Extended H$\ddot{u}$ckel molecular calculations have been used to analyze how the magnitude of exchange coupling is influenced by the structural distortions in a series of dinuclear six-coordinate copper(II) complexes bridged by the planar bis-bidentate oxalate anion. Copper(II) ions have distorted octahedral surroundings, one being axially elongated and the other compressed. The magnetic interaction is strong in the former complexes and very weak in the latter. This is interpreted as resulting from a switching of magnetic spin orbitals due to the structural distortions (bond elongation or compression) of the copper sites.

• 대한전자공학회논문지
• /
• 제24권1호
• /
• pp.133-139
• /
• 1987

A phase-locked Channel-Substrate-Planar(CSP) laser arrays is described. Arrays of emitters with weak coupling are operated in a set of discrete modes determined by the number and spacing of the emitters. The interactions between emitters lead to a splitting of the wave-length and gain which are calculated from the coupling strength. Phase-locked arrays has exhibited to CW output-power as high as 80 m W and the highest order mode will have preferred oscillation. A strong hole burning is occurred at p=30m W. The most stable lasing mode is occurred at element spacing S=3.5\ulcornerm and there is no coupling at S>7 \ulcornerm.

• Bulletin of the Korean Chemical Society
• /
• 제17권5호
• /
• pp.452-457
• /
• 1996

The effects caused by the ionization on the electronic structure and geometry on C60 are studied by the modified Su-Schriffer-Heeger (SSH) model Hamiltonian. After the ionization of C60, the bond structure of the singly charged C60 cation is deformed from Ih symmetry of the neutral C60 to D5d, C1, and C2, which is dependent upon the change of the electron-phonon coupling strength. The electronic structure of the C60+ cation ground state undergoes Jahn-Teller distortion in the weak electron-phonon coupling region, while self-localized states occur in the intermediate electron-phonon region, but delocalized electronic states appear again in the strong electron-phonon region. In the realistic strength of the electron-phonon coupling in C60, the bond structure of C60+ shows the layer structure of the bond distortion and a polaron-like state is formed.

• International Journal of Control, Automation, and Systems
• /
• 제4권6호
• /
• pp.689-696
• /
• 2006

This paper presents a new algorithm for the closed-loop $H_{\infty}$ composite control of weakly coupled bilinear systems with time-varying parameter uncertainties and exogenous disturbance using the successive Galerkin approximation(SGA). By using weak coupling theory, the robust $H_{\infty}$ control can be obtained from two reduced-order robust $H_{\infty}$ control problems in parallel. The $H_{\infty}$ control theory guarantees robust closed-loop performance but the resulting problem is difficult to solve for uncertain bilinear systems. In order to overcome the difficulties inherent in the $H_{\infty}$ control problem, two $H_{\infty}$ control laws are constructed in terms of the approximated solution to two independent Hamilton-Jacobi-Isaac equations using the SGA method. One of the purposes of this paper is to design a closed-loop parallel robust $H_{\infty}$ control law for the weakly coupled bilinear systems with parameter uncertainties using the SGA method. The other is to reduce the computational complexity when the SGA method is applied to the high order systems.