• 제목/요약/키워드: Square planar

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도체스트립을 이용한 평판사각 스파이럴 안테나 (Planar Square-spiral Antenna using a strip conductor)

  • 양두영;이민수
    • 한국산학기술학회논문지
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    • 제13권5호
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    • pp.2325-2331
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    • 2012
  • UHF 대역인 860MHz~960MHz에서 동작하는 RFID 시스템용으로 도체스트립을 이용한 평판사각 스파이얼 안테나를 제안하고 분석하였다. 도체스트립의 공통선 길이, 분리간격, 선폭, 선간격, 스파이럴 회전수를 변화시켜서 안테나 입력임피던스와 RFID 테그칩 간을 정합스터브 없이 소형으로 설계하고, 최적화된 안테나를 제작하였다. 최적화된 결과로부터, VSWR<2인 범위의 주파수대역은 RFID 초고주파 대역인 100MHz를 포함한다. 안테나 이득은 910MHz 중심주파수에서 3.5DBi이고, 빔패턴은 수직과 수평방향으로 지향성 패턴을 갖는다. 따라서 제안된 안테나는 규정된 입력임피던스를 갖는 다양한 형태의 테그칩을 요구하는 실질적인 RFID 응용에 적합하다.

평면 배열 안테나 기반의 적응 빔형성 시스템 성능 분석 (Performance Analysis of Adaptive Beamforming System Based on Planar Array Antenna)

  • 문지윤;황석승
    • 한국전자통신학회논문지
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    • 제13권6호
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    • pp.1207-1212
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    • 2018
  • 신호정보 수집(: Signal Intelligence, SIGINT) 기술은 군수산업을 비롯한 여러 분야에서 다양한 데이터 수집을 목적으로 활발하게 사용되고 있다. 효율적으로 신호정보 및 데이터를 수집하고 수집된 데이터를 송/수신하기 위해서는 신호의 정확한 도래각 정보가 필요하고, 간섭 또는 재밍 신호로부터의 통신 방해가 최소화되어야 한다. 본 논문에서는 효율적으로 신호정보 및 데이터를 수집하고 송/수신하기 위한, 평면 배열 안테나 기반의 적응 빔형성 위성 시스템 구조를 소개한다. 제시된 적응 빔형성 시스템은 폄면 배열 형태의 안테나, MUSIC(: Multiple Signal Classification) 알고리즘 기반의 도래각 추정기, MVDR(: Minimum Variance Distortionless Response) 간섭 제거기, 신호처리 및 D/B 유닛, MMSE(: Minimum Mean Square Error) 기반의 송신 빔형성기 등으로 구성되어 있다. 또한, 컴퓨터 시뮬레이션을 통해, 제시된 시스템의 성능을 평가하고 분석한다.

고밀도 SMPS 용 변압기의 제조와 특성 (Fabrication and Characteristics of Transformers for High Power Density SMPS)

  • 김현식;김종령;허정섭;오영우;송재성
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2002년도 춘계학술대회 논문집 초전도 자성체
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    • pp.7-10
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    • 2002
  • We designed the flyback planar transformer, which had 8W capacity, with 70V input voltage and 8.2V output voltage for the establishment of design method and the confirmation of application possibility. The numerical value of inductance measured under the switching frequency of 120 kHz was 1650 ${\mu}H$, which was the inductance efficiency of 85~87% against theoretical value. The A.C. resistance of primary and secondary coil was 4.2 ${\Omega}$ and 0.25 ${\Omega}$ respectively. On the other hand, the quality factor for each wound numbers showed quite a high value of 158 and 75 respectively. And the Coupling Factor was 0.96~0.97 under 120 kHz switching frequency. And the shape of the output wave of the planar transformer at 70V input voltage was a stable square wave.

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광대역 슬리브 모노폴 안테나의 단순화 설계 (Design of Simplified Wideband Sleeve Monopole Antenna)

  • 황희용;최경
    • 전기전자학회논문지
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    • 제23권3호
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    • pp.1100-1103
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    • 2019
  • 본 논문에서는 기존의 3차원 구조의 슬리브모노폴 안테나(Sleeve monopole Antenna)를 모노폴과 접지면상의 작은 기생모노폴의 형태로 단순화하여도 비슷한 특성을 보이는 것을 확인하고 PCB상에 보다 광대역인 평면 슬리브모노폴 안테나의 설계 방법에 대해 다룬다. 설계 및 제작된 슬리브안테나는 평면형으로 메인 모노폴과 이에 근접하는 작은 사각형 슬리브로 구성되고 기존의 3차원 슬리브안테나와 비슷한 전방향(omni-directional)특성과 기존보다 46% 더 넓은 대역폭을 나타내었다.

Planar-Jet형 연소기 내 난류유동의 LES (Large-Eddy Simulation of Turbulent Flows in a Planar Combustor)

  • 김도형;양경수;신동신
    • 대한기계학회논문집B
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    • 제24권10호
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    • pp.1409-1416
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    • 2000
  • In this study, turbulent flows in a planar combustor which has a square rib-type flame holder are numerically investigated by Large Eddy Simulation(LES). Firstly, the flow fields with or without jet injection downstream of the flame-holder are examined using uniform inlet velocity. Comparison of the present LES results with experimental one shows a good agreement. Secondly, to investigate mixing of oxidizer(air) and fuel injected behind the flame holder, the scalar-transport equation is introduced and solved. From the instantaneous flow and scalar fields, complex and intense mixing phenomena between fuel and jet are observed. It is shown that the ratio of jet to blocked air velocity is an important factor to determine the flow structure. Especially, when the ratio is large enough, the fuel jet penetrates the main vortices shed from the flame holder, resulting in significant changes in the flow and scalar fields.

Performance of a Planar Leaky-Wave Slit Antenna for Different Values of Substrate Thickness

  • Hussain, Niamat;Kedze, Kam Eucharist;Park, Ikmo
    • Journal of electromagnetic engineering and science
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    • 제17권4호
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    • pp.202-207
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    • 2017
  • This paper presents the performance of a planar, low-profile, and wide-gain-bandwidth leaky-wave slit antenna in different thickness values of high-permittivity gallium arsenide substrates at terahertz frequencies. The proposed antenna designs consisted of a periodic array of $5{\times}5$ metallic square patches and a planar feeding structure. The patch array was printed on the top side of the substrate, and the feeding structure, which is an open-ended leaky-wave slot line, was etched on the bottom side of the substrate. The antenna performed as a Fabry-Perot cavity antenna at high thickness levels ($H=160{\mu}m$ and $H=80{\mu}m$), thus exhibiting high gain but a narrow gain bandwidth. At low thickness levels ($H=40{\mu}m$ and $H=20{\mu}m$), it performed as a metasurface antenna and showed wide-gain-bandwidth characteristics with a low gain value. Aside from the advantage of achieving useful characteristics for different antennas by just changing the substrate thickness, the proposed antenna design exhibited a low profile, easy integration into circuit boards, and excellent low-cost mass production suitability.

ON THE DOMINATION NUMBER OF A GRAPH AND ITS SQUARE GRAPH

  • Murugan, E.;Joseph, J. Paulraj
    • Korean Journal of Mathematics
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    • 제30권2호
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    • pp.391-402
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    • 2022
  • For a given graph G = (V, E), a dominating set is a subset V' of the vertex set V so that each vertex in V \ V' is adjacent to a vertex in V'. The minimum cardinality of a dominating set of G is called the domination number of G and is denoted by γ(G). For an integer k ≥ 1, the k-th power Gk of a graph G with V (Gk) = V (G) for which uv ∈ E(Gk) if and only if 1 ≤ dG(u, v) ≤ k. Note that G2 is the square graph of a graph G. In this paper, we obtain some tight bounds for the sum of the domination numbers of a graph and its square graph in terms of the order, order and size, and maximum degree of the graph G. Also, we characterize such extremal graphs.

Template Synthesis and Characterization of Four- and Five-Coordinate Copper(II) Complexes with Hexaaza Macrotricyclic Ligands 1,3,6,9,11,14-Hexaazatricyclo $[12.2.1.1^{6,9}]octadecane(L_1)$ and 1,3,6,10,12,15-Hexaazatricyclo $[13.3.1.1^{6,10}]eicosane(L_1)$

  • Myunghyun Paik Suh;Shin-Geol Kang;Teak-Mo Chung
    • Bulletin of the Korean Chemical Society
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    • 제11권3호
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    • pp.206-208
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    • 1990
  • Cu(II) hexaazamacrotricyclic complexes $[Cu(L)](ClO_4)_2$ and $[(Cu(L)Cl]ClO_4$, where L = 1,3,6,9,11,14-hexaazatricyclo$[12.2.1.1^{6,9}]octadecane(L_1)$ or 1,3,6,10,12,15-hexaazatricyclo$[13.3.1.1^{6,10}]eicosane(L_2)$, have been prepared by the simple template condensation reactions of triamines, diethylenetriamine for $L_1$, and N-(2-aminoethyl)-1,3-propanediamine for $L_2$, with formaldehyde in the presence of $Cu(OAc)_2\;or\;CuCl_2$. The Cu(II) complexes of $L_1$ contain two 1,3-diazacyclopentane ring moieties and those of $L_2$ contain two 1,3-diazacyclohexane ring moieties that are fused to the 14-membered macrocyclic framework. Spectra indicate that complexes $[Cu(L)](ClO_4)_2\;and\;[Cu(L)Cl]ClO_4$ have square-planar and square-pyramidal chromophores, respectively. square-planar $[Cu(L)](ClO_4)_2$ are remarkably stable against ligand dissociation in acidic aqueous solutions. Square-pyramidal $[Cu(L)Cl]ClO_4$ complexes dissociate their axial Cl-ligands easily in aqueous solutions to form $[Cu(L)H_2O]^{2+}$ species. Infrared and UV/vis absorption spectra of the Cu(II) complexes reveal that Cu-N interactions and the ligand field strengths are significantly weaker in the complexes of $L_2$ than in the complexes of $L_1$.

Platinum(Ⅱ) Complexes of 6,6$^\prime$-Dimethyl-2,2$^\prime$-diaminobiphenyl

  • 전무진
    • Bulletin of the Korean Chemical Society
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    • 제6권4호
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    • pp.238-240
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    • 1985
  • Carbonato and diammine platinum(Ⅱ) complexes of resolved 6,6'-dimehtyl-2,2'-diaminobiphenyl have been prepared. The absolute configuration of the square planar platinum(Ⅱ) complexes is determined on the basis of stereospecificity of the 6,6'-dimethyl-2,2'-diaminobiphenyl ligand, circular dichroism spectra of the complexes, and nonempirical circular dichroism method.

팔면체 $[M(II)Cl_2O_2N_2]$, 사각형 및 사면체 $[Pd(Ⅱ) X_2Y_2]$형태 착물의 쌍극자모멘트의 계산 [M(Ⅱ) = Ni(Ⅱ) 또는 Co(Ⅱ), X = N 그리고 Y = O 또는 S] (Calculation of the Dipole Moments for Octahedral $[M(II)Cl_2O_2N_2]$ Square Planar and Tetrahedral $[Pd(Ⅱ)X_2Y_2]$ Type Complexes [M(Ⅱ) = Ni(Ⅱ) or Co(Ⅱ), X = N and Y = O or S])

  • 안상운
    • 대한화학회지
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    • 제23권2호
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    • pp.59-64
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    • 1979
  • 팔면체 $[M(II)Cl_2N_2O_2]$, 사각형 및 사면체 $[Pd(II)X_2Y_2]$형태 착물의 쌍극자모멘트를 근사분자궤도함수를 사용하여 계산하였다. 이들 착물에 대하여 계산한 쌍극자모멘트의 값은 실험치와 비교적 잘 일치하였다. 계산한 쌍극자 모멘트를 기초로 하여 이들 착물에 대한 가능한 구조를 고찰하였다.

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