• 한국전자파학회논문지
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• 제16권3호
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• pp.300-310
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• 2005

본 논문에서는 사각 패치와 사각 링 스트립선로가 전자기적으로 결합된 3층 구조의 소형화된 EBG구조를 제안하였다. 제안한 EBG 구조는 상층의 사각 패치와 하층의 사각 링 스트립선로가 비아에 의해 접지면에 연결되었다. 반사위상 EM시뮬레이션을 통해 EBG구조 표면에서의 반사위상을 계산하여 EBG구조의 밴드갭 특성을 연구하였고, 반사위상에서 나타나는 밴드갭과 투과계수(S$_{21}$)에서 나타나는 밴드갭이 일치하는 것을 EM 시뮬레이션을 통해 확인하였으며, 측정은 제작이 용이한 프로브 안테나를 사용하여 EBG 구조의 표면을 진행하는 표면파의 투과계수를 측정하였다. 제안한 EBG구조는 동일한 크기의 기존 3층 구조에 비하여 밴드갭이 나타나는 주파수가 약 34 $\%$ 감소되었다. 측정한 결과 제안한 구조는 0.930 GHz에서 0.945 GHz까지의 밴드갭을 갖는다.

• 대기
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• 제26권3호
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• pp.387-400
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• 2016

In this study, the atmospheric $CO_2$ concentrations estimated by CT2013B, a recent version of CarbonTracker, are compared with $CO_2$ measurements from the Comprehensive Observation Network for Trace gases by Airliner (CONTRAIL) project during 2010-2011. CarbonTracker is an inversion system that estimates surface $CO_2$ fluxes using atmospheric $CO_2$ concentrations. Overall, the model results represented the atmospheric $CO_2$ concentrations well with a slight overestimation compared to observations. In the case of horizontal distribution, variations in the model and observation difference were large in northern Eurasia because most of the model and data mismatch were located in the stratosphere where the model could not represent $CO_2$ variations well enough due to low model resolution at high altitude and existing phase shift from the troposphere. In addition, the model and observation difference became larger in boreal summer. Despite relatively large differences at high latitudes and in boreal summer, overall, the modeled $CO_2$ concentrations fitted well to observations. Vertical profiles of modeled and observed $CO_2$ concentrations showed that the model overestimates the observations at all altitudes, showing nearly constant differences, which implies that the surface $CO_2$ concentration is transported well vertically in the transport model. At Narita, overall differences were small, although the correlation between modeled and observed $CO_2$ concentrations decreased at higher altitude, showing relatively large differences above 225 hPa. The vertical profiles at Moscow and Delhi located on land and at Hawaii on the ocean showed that the model is less accurate on land than on the ocean due to various effects (e.g., biospheric effect) on land compared to the homogeneous ocean surface.

• 폴리머
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• 제24권3호
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• pp.314-325
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• 2000

경질 사슬(HS) 함량이 각각 35.5 (TPU-35)와 53.4 wt% (TPU-53)인 열가소성 폴리우레탄(TPU)으로 개질된 폴리카보네이트(PC)의 열분해 특성을 DSC, GPC 및 FT-IR로 연구하였다. 경질 사슬 함량이 큰 TPU의 T$_{g}$가 높게 나타났으며, PC/TPU 블렌드에서 HS 함량에 관계없이 열처리 온도와 TPU 함량이 증가함에 따라 PC의 T$_{g}$가 감소하였다. 이는 열처리에 따른 열가소성 TPU물질의 열분해 현상에 기인한 것인데, PC/TPU-35 블렌드는 24$0^{\circ}C$에서, PC/TPU-53은 25$0^{\circ}C$에서 관찰되었다. DSC로 측정된 열분해 온도는 GPC에 의한 블렌드 조성별 분자량과 분자량 분포도 및 점도 측정으로도 재확인되었다. PC/TPU-35와 PC/TPU-53의 두 가지 블렌드를 열분해 온도의 전ㆍ후에서 가열한 시료를 FT-IR로 분석한 결과, PC의 카르보닐 스트레칭은 1774$cm^{-1}$ /, TPU는 1732와 1704$cm^{-1}$ /에서 나타났으며, 블렌드에서는 두 가지 구성물질의 특성피크(카르보닐기와 N-H 그룹)에 변화가 없는 것으로 보아, 두 가지 블렌드 사이의 분자간 상호작용이나 에스테르 교환반응의 가능성이 없는 증거로 생각된다. 아울러 분해온도 이전에서 가공된 시료의 두께 의존성 충격강도 및 굴곡강도를 측정하고, 상 형태학과도 비교하였다.다.

• Bulletin of the Korean Chemical Society
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• 제7권2호
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• pp.137-142
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• 1986

The luminescence spectra of $Ru(bpy)_3^{2+}$ in poly(methacrylic acid) (PMA) solutions varied sensitively with pH. At pH < 5.5, the emission intensity increased with pH up to 4 times, while it decreased with pH beyond the pH. The enhanced emission intensity was accompanied by blue-shift of the emission maxima as much as 15 nm. The enhancement of emission intensity was attributed to the restricted rotational mobility of ligand of the cation bound to densely coiled PMA molecules at pH < 5.5. The sharp decrease in emission intensity with increasing pH near pH 5.6 was accounted for conformational transition of the polymer to more extended structure, which was also revealed in viscosity measurement. The enhancement of emission intensity became higher as NaCl concentration of the solution increased. The binding constant of $Ru(bpy)_3^{2+}$ with two carboxylate groups of PMA was calculated as $2{\times}10^5\;M^{-1}$ in 0.1 M NaCl at pH 5.2. The pH dependence of luminescence quenching rate of $Ru(bpy)_3^{2+}$ by $Cu^{++}$ also showed maximum near pH 5, and the rate was more than $10^3$ times higher than that in water, whereas the maximum enhancement of quenching rate (about 20 times) in poly(acrylic acid) (PAA) solution occurred at pH 4.5. On the other hand, the pH dependence for neutral water soluble nitrobenzene (NB) exhibited opposite trend to that of $Cu^{++}$. The quenching constant vs pH curve for $MV^{++}$ was composite of those for $Cu^{++}$ and NB. The anomalous high quenching rate for $Cu^{++}$ in PMA solution at pH < 5.5 was attributed to the binding of $Ru(bpy)_3^{2+}$ and $Cu^{++}$ to the same region of PMA, when it conforms densely coiled structure in the pH range. The observation of mininium quenching rate for NB near pH 5.5 indicated that the $Ru(bpy)_3^{2+}$ bound to the densely coiled PMA is not accessible by NB, which is in bulk water phase. The composite nature of the pH dependence of quenching rate for $MV^{++}$ in PMA solution was attributed to the smaller binding affinity of the cation to PMA, compared to that of $Cu^{++}$. The sharp, cooperative conformational transition with pH observed in PMA was not revealed in PAA. But, the pH dependence of quenching rates in this polymer reflected increased charge density and, thus, binding of cations to the polymer, and expansion of the polymer chain with pH.