101 research outputs found

    A STUDY ON SERIES SLOT ARRAY ANTENNA DESIGN METHODOLOGY AND ITS APPLICATION TO DUAL LINEAR POLARIZATION

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    ํ•™์œ„๋…ผ๋ฌธ (๋ฐ•์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ์ „๊ธฐยท์ปดํ“จํ„ฐ๊ณตํ•™๋ถ€, 2014. 2. ๋‚จ์ƒ์šฑ.๋ณธ ๋…ผ๋ฌธ์—์„œ๋Š” ์ž„์˜์˜ ์„ ํ˜•ํŽธํŒŒ ๋ฐœ์ƒ์„ ์œ„ํ•œ ์ง๋ ฌ ์Šฌ๋กฏ ๋ฐฐ์—ด์•ˆํ…Œ๋‚˜ ์„ค๊ณ„ ๋ฐฉ๋ฒ•์„ ์ œ์‹œํ•˜์˜€๋‹ค. 45๋„ ๊ธฐ์šธ์–ด์ง„ ์„ ํ˜•ํŽธํŒŒ ๋ฐœ์ƒ์ด ๊ฐ€๋Šฅํ•˜๊ณ  ๋™์‹œ์— ์ž„ํ”ผ๋˜์Šค ์ •ํ•ฉ, ๊ท ์ผ์ „์žฅ ๋ถ„ํฌ๋ฅผ ํ˜•์„ฑํ•  ์ˆ˜ ์žˆ๋„๋ก '๊ต์ฐจ ๋ฆฌ์•กํ„ด์Šค ์Šฌ๋กฏ ์Œ'์„ ๊ธฐ๋ณธ ๋ฐฉ์‚ฌ์ฒด๋กœ ์ œ์•ˆํ•˜์˜€๋‹ค. ์ด ๊ธฐ๋ณธ ๋ฐฉ์‚ฌ์ฒด๋ฅผ ์ด์šฉํ•˜๋ฉด ๊ฐœ๋ณ„ ๋ฐฉ์‚ฌ ์Šฌ๋กฏ ๊ฐ„์˜ ๊ฐ„๊ฒฉ์ด ๊ด€๋‚ด ํŒŒ์žฅ์˜ ๋ฐ˜ ํŒŒ์žฅ ๊ฐ„๊ฒฉ์œผ๋กœ ์œ„์น˜์‹œํ‚ฌ ์ˆ˜ ์žˆ๊ธฐ ๋•Œ๋ฌธ์— grating lobe๋ฅผ ์–ต์ œํ•  ์ˆ˜ ์žˆ๋‹ค. ๋˜ํ•œ, ์ œ์•ˆํ•œ ์•ˆํ…Œ๋‚˜ ์„ค๊ณ„ ๊ธฐ๋ฒ•์€ ๊ธฐํŒ ์ง‘์  ๋„ํŒŒ๊ด€ ๊ธฐ์ˆ  (substrate integrated waveguide, SIW)์„ ํ†ตํ•ด ๊ตฌํ˜„ํ•˜์˜€๊ณ  ์ „์žฅ ์‹œ๋ฎฌ๋ ˆ์ดํ„ฐ ๋ฐ ์ œ์ž‘, ์ธก์ •์„ ํ†ตํ•ด ์„ค๊ณ„ ๊ธฐ๋ฒ•์˜ ์ ํ•ฉ์„ฑ์„ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ๋จผ์ €, Ka-๋ฐด๋“œ ์šฉ ์„ ํ˜• ๋ฐ ํ‰๋ฉด ๋ฐฐ์—ด์•ˆํ…Œ๋‚˜๋ฅผ ์„ค๊ณ„ํ•˜์˜€๋‹ค. 45๋„ ์„ ํ˜•ํŽธํŒŒ๋ฅผ ๋ฐœ์ƒ์‹œํ‚ค๊ธฐ ์œ„ํ•ด ์ ์ธต์˜ SIW ๊ตฌ์กฐ๋กœ ๋ฐฐ์—ด์•ˆํ…Œ๋‚˜๋ฅผ ๊ตฌํ˜„ํ•˜์˜€์œผ๋ฉฐ ๊ท ์ผ ์ „์žฅ์ด ๋ฐœ์ƒ๋˜๋Š” ์›๋ฆฌ๋ฅผ ๋“ฑ๊ฐ€ํšŒ๋กœ ๋ฐ ์ž„ํ”ผ๋˜์Šค, ์ „๋ฅ˜ ์ˆœํ™˜ ๋ฐฉ์ •์‹์„ ์ด์šฉํ•˜์—ฌ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ๋‚˜์•„๊ฐ€, ์ „์ž์žฅ ์‹œ๋ฎฌ๋ ˆ์ดํ„ฐ๋ฅผ ํ†ตํ•œ ๊ฒฐ๊ณผ์™€ ๋น„๊ตโ€ข๋ถ„์„ํ•˜์˜€๋‹ค. ๋‘ ๋ฒˆ์งธ๋กœ, ๋‚ฎ์€ ๋ถ€์—ฝ๋ ˆ๋ฒจ์„ ๊ฐ€์ง€๋„๋ก ๊ฐœ๋ณ„ ๋ฐฉ์‚ฌ์ฒด์˜ ์ „์žฅ ๊ณ„์ˆ˜ ์กฐ์ ˆ ๋ฐฉ๋ฒ•์„ ์ œ์•ˆํ•˜์˜€๋‹ค. ๊ฐ ์ง๋ ฌ ๋ฐฉ์‚ฌ ์Šฌ๋กฏ์„ ํ๋ฅด๋Š” ๋ชจ๋“œ ์ „๋ฅ˜์˜ ํฌ๊ธฐ๋ฅผ ์กฐ์ ˆํ•˜๊ธฐ ์œ„ํ•ด ๊ฐœ๋ณ„ ๋ฐฉ์‚ฌ์ฒด์˜ ์œ„์น˜๋ฅผ ์ค‘์‹ฌ์„ ์„ ๋”ฐ๋ผ ์ด๋™์‹œํ‚ฌ ์ˆ˜ ์žˆ๋‹ค. ์ด๋Ÿฌํ•œ ์˜ต์…‹ ์กฐ์ ˆ ๋ฐฉ๋ฒ•์„ ์ด์šฉํ•˜์—ฌ โ€’20 dB ๋ฐ โ€’26 dB Dolph-Chebyshev ๊ณ„์ˆ˜๋ฅผ ๊ฐ€์ง€๋Š” ์„ ํ˜• ๋ฐฐ์—ด์•ˆํ…Œ๋‚˜๋ฅผ ์„ค๊ณ„ํ•˜์˜€๊ณ  ์ œ์•ˆํ•œ ๋ฐฉ๋ฒ•์˜ ํšจ์šฉ์„ฑ์„ ์ œ์ž‘ ๋ฐ ์ธก์ •์„ ํ†ตํ•ด ๊ฒ€์ฆํ•˜์˜€๋‹ค. ๋งˆ์ง€๋ง‰์œผ๋กœ, ยฑ45๋„ ์ด์ค‘ ์„ ํ˜•ํŽธํŒŒ ๋ฐœ์ƒ์„ ์œ„ํ•œ ์„ค๊ณ„ ๊ธฐ๋ฒ•์„ ์ œ์•ˆํ•˜์˜€๋‹ค. ๋™์ผํ•œ ๊ฐœ๊ตฌ๋ฉด์„ ๊ณต์œ ํ•˜๋Š” ๋‘ ์„ ํ˜•ํŽธํŒŒ ๊ฐ„์˜ ๊ฒฉ๋ฆฌ๋„๋ฅผ ์ตœ๋Œ€ํ™”ํ•˜๊ธฐ ์œ„ํ•ด ๊ต์ฐจ ์Šฌ๋กฏ ๊ฐ„์— ์ˆ˜์ง ์กฐ๊ฑด์„ ๋งŒ์กฑํ•  ์ˆ˜ ์žˆ๋„๋ก ๊ธฐํŒ์˜ ์œ ์ „์œจ ๋ฐ ๋ฐฉ์‚ฌ SIW์˜ ํญ์„ ๊ฒฐ์ •ํ•˜์˜€๋‹ค. ๋‚˜์•„๊ฐ€ ์ œ์•ˆํ•œ ์„ค๊ณ„ ๊ธฐ๋ฒ•์„ 8 ร— 8 ์ด์ค‘ ํ‰๋ฉด ๋ชจ๋…ธํŽ„์Šค ์•ˆํ…Œ๋‚˜ ์„ค๊ณ„์— ์‘์šฉํ•˜์˜€๋‹ค. ๋ชจ๋…ธํŽ„์Šค ๋™์ž‘์„ ์œ„ํ•ด ๊ธฐ์กด์˜ ๊ธˆ์† ๋„ํŒŒ๊ด€ ์ „์†ก์„ ๋กœ๋ฅผ ์ด์šฉํ•ด ์ œ์ž‘๋œ ๋น„๊ต๊ธฐ๋ฅผ ๊ฒฐํ•ฉํ•˜์˜€์œผ๋ฉฐ ๋ฐ˜์‚ฌ์†์‹ค, ๋ฐฉ์‚ฌํŒจํ„ด, ์ด๋“ ๋“ฑ์˜ ์ „๊ธฐ์ ์ธ ๊ฒฐ๊ณผ๋ฅผ ํ™•์ธํ•˜์˜€๋‹ค.1. Introduction 1 1.1 Conventional Slot Array Antennas for Linear Polarization 3 1.2 Substrated Integrated Waveguide (SIW) Technology 5 2. Linear Slot Array Antenna for 45ยบ-Inclined Linear Polarization 9 2.1 Introduction 9 2.2 Proposed Antenna Configuration 10 2.2.1 Single Slot Module and Impedance Extraction 11 2.2.2 Alternating Reactance Slot Pair 14 2.2.3 Equivalent Circuit Analysis using Recursive Formulas 17 2.2.4 Centered-Inclined Series-to-Series Coupling Slot 20 2.3 Simulation and Measurement 22 2.4 Summary 25 3. Planar Slot Array Antenna for 45ยบ-Inclined Linear Polarization 30 3.1 Introduction 30 3.2 Proposed Antenna Configuration 33 3.3 Feeding Network Design and Analysis 35 3.4 Coupling and Radiating Slot Arrangement for In-Phase Excitation 41 3.5 Wideband Coax-to-SIW Transition Design and Analysis 42 3.6 Simulation and Measurement 48 3.6.1 Uniform Electric Field Distribution 48 3.6.2 Back-to-Back Coax-to-SIW Transition 52 3.6.3 Reflection Coefficient, Gain, and Radiation Patterns 54 3.7 Summary 57 4. Excitation Control Method for Low Sidelobe Level 63 4.1 Introduction 63 4.2 Axial Displacements for Excitation Control 66 4.3 Design Procedure for Excitation Control 73 4.4 Simulation and Measurement 77 4.5 Summary 82 5. Dual Linear Polarized SIW Monopulse Antenna for Tracking Radar 85 5.1 Introduction 85 5.2 Design Considerations for Dual LP Radiating SIWs 88 5.3 The Proposed Dual LP 8 by 8 SIW Monopulse Protptype Antenna 92 5.3.1 Folded Short-Circuited Stubs 95 5.3.2 Shunt-to-Series Coupling Slots 96 5.3.3 Series-to-Series Coupling Slots 97 5.4 RWG Comparator for Monopulse Operation 98 5.5 Experimental Results 103 5.5.1 Dual LP SIW Sub-Array Antenna 103 5.5.2 Dual LP SIW Monopulse Antenna 107 5.6 Summary 109 6. Conclusion 116Docto

    ๋ฌธ์ œ ํ•ด๊ฒฐ์‹ ๊ต์ˆ˜ ๋ฐฉ๋ฒ•์ด ํ•™์ƒ์˜ ์„ฑ์ทจ๋„, ๊ณผํ•™์  ๊ณผ์ • ๊ธฐ์ˆ , ๊ณผํ•™ ํ™œ๋™ ์ธ์‹์— ๋ฏธ์น˜๋Š” ํšจ๊ณผ

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    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ)--์„œ์šธๅคงๅญธๆ ก ๅคงๅญธ้™ข :็ง‘ๅญธๆ•Ž่‚ฒ็ง‘ ๅŒ–ๅญธๅฐˆๆ”ป,1996.Maste

    Study on Research Trend related to Children with Special needs Reported in the Korean Journal Art Therapy

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    ใ€Œ้Ÿ“.็พŽ็›ธไบ’้˜ฒ่ก›ๆข็ด„ใ€์— ๊ด€ํ•œ ็ก็ฉถ : ๅœ‹ๅฎถๅˆฉ็›Š์˜ ่ง€้ปž์—์„œ

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    ํ•™์œ„๋…ผ๋ฌธ(์„์‚ฌ)--์„œ์šธๅคงๅญธๆ ก ๅคงๅญธ้™ข :ๆ”ฟๆฒปๅญธ็ง‘ ๆ”ฟๆฒปๅญธๅฐˆๆ”ป,1996.Maste

    Feature-guided Image Stippling

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    The Effects of Hexamethylenetetramine Concentration on the Structural and Electrochemical Performances of Ni(OH)2 Powder for Pseudocapacitor Applications

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    Ni hydroxides (Ni(OH)2) are synthesized on Ni foam by varying the hexamethylenetetramine (HMT) concentration using an electrodeposition process for pseudocapacitor (PC) applications. In addition, the effects of HMT concentration on the Ni(OH)2 structure and the electrochemical properties of the PCs are investigated. HMT is the source of amine-based OHโˆ’ in the solution; thus, the growth rate and morphological structure of Ni(OH)2 are influenced by HMT concentration. When Ni(OH)2 is electrodeposited at a constant voltage mode of -0.85 V vs. Ag/AgCl, the cathodic current and the number of nucleations are significantly reduced with increasing concentration of HMT from 0 to 10 mM. Therefore, Ni(OH)2 is sparsely formed on the Ni foam with increasing HMT concentration, showing a layered double-hydroxide structure. However, loosely packed Ni(OH)2 grains that are spread on Ni foam maintain a much greater surface area for reaction and result in the effective utilization of the electrode material due to the steric hindrance effect. It is suggested that the Ni(OH)2 electrodes with HMT concentration of 7.5 mM have the maximum specific capacitance (1023 F/g), which is attributed to the facile electrolyte penetration and fast proton exchange via optimized surface areas.2
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