• 한국초전도학회:학술대회논문집
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• 한국초전도학회 2008년도 High Temperature Superconductivity Vol.XVIII
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• pp.70-70
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• 2008

• 한국재료학회지
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• 제15권6호
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• pp.408-412
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• 2005

[ $Ba_{1.5}Sr_{0.5}SiO_4:Eu$ ] phosphor particles with high photoluminescence intensity under long wavelength ultraviolet were prepared by spray pyrolysis. We investigated the effect of $NH_4F$ flux added into starting solution on the morphology and photoluminescence intensity of $Ba_{1.5}Sr_{0.5}SiO_4:Eu$ phosphor prepared by spray pyrolysis. $Ba_{1.5}Sr_{0.5}SiO_4:Eu$ phosphor particles prepared from starting solution containing $NH_4F$ flux had the maximum photoluminescence intensity at the post-treatment temperature of $1200^{\circ}C$ and the maximum photoluminescence intensity of $Ba_{1.5}Sr_{0.5}SiO_4:Eu$ phosphor particles prepared from the starting solution containing $NH_4F$ flux was $137\%$ of that of the phosphor particles prepared from the starting solution without flux material. $Ba_{1.5}Sr_{0.5}SiO_4:Eu$ phosphor particles prepared from starting solution containing $NH_4F$ flux had larger size and more aggregated morphology than those prepared from starting solution without flux material. The photoluminescence intensity of $Ba_{1.5}Sr_{0.5}SiO_4:Eu$ phosphor particles prepared from starting solution containing $NH_4F$ flux above $3wt.\%$ had high photoluminescence intensities. The addition amount of $NH_4F$ flux showing the maximum photoluminescence intensity was $12wt.\%$. The optimum amount of $NH_4F$ flux was $5wt.\%$ when we considered the morphological and photoluminescence characteristics of $Ba_{1.5}Sr_{0.5}SiO_4:Eu$ ohosphor particles prepared by spray pyrolysis.

• Ocean Science Journal
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• 제40권3호
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• pp.167-176
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• 2005

A time-series sediment trap was deployed at 1,034 m water depth in the eastern Bransfield Strait for a complete year from December 25, 1998 to December 24, 1999. About 99% of total mass flux was trapped during an austral summer, showing distinct seasonal variation. Biogenic particles (biogenic opal, particulate organic carbon, and calcium carbonate) account for about two thirds of annual total mass flux $(49.2\;g\;m^{-2})$, among which biogenic opal flux is the most dominant (42% of the total flux). A positive relationship (except January) between biogenic opal and total organic carbon fluxes suggests that these two variables were coupled, due to the surface-water production (mainly diatoms). The relatively low $\delta^{13}C$ values of settling particles result from effects on C-fixation processes at low temperature and the high $CO_2$ availability to phytoplankton. The correspondingly low $\delta^{l5}N$ values are due to intense and steady input of nitrates into surface waters, reflecting an unlikely nitrate isotope fractionation by degree of surface-water production. The $\delta^{l5}N$ and $\delta^{l3}C$ values of sinking particles increased from the beginning to the end of a presumed phytoplankton bloom, except for anomalous $\delta^{l5}N$ values. Krill and the zooplankton fecal pellets, the most important carriers of sinking particles, may have contributed gradually to the increasing $\delta^{l3}C$ values towards the unproductive period through the biomodification of the $\delta^{l3}C$ values in the food web, respiring preferentially and selectively $^{12}C$ atoms. Correspondingly, the increasing $\delta^{l5}N$ values in the intermediate-water trap are likely associated with a switch in source from diatom aggregates to some remains of zooplankton, because organic matter dominated by diatom may be more liable and prone to remineralization, leading to greater isotopic alteration. In particular, the tendency for abnormally high $\delta^{l5}N$ values in February seems to be enigmatic. A specific species dominancy during the production may be suggested as a possible and speculative reason.

• 대한환경공학회지
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• 제28권10호
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• pp.1046-1054
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• 2006

낙동강 매리원수의 경우 HPO가 42.9%, HPI가 39.3% 및 TPI가 17.8%를 차지하고 있는 것으로 나타났다. HPO를 세분화한 결과에서 HPO-FA와 HPO-HA의 구성비는 62%와 38%로 나타났고, HPO-car과 HPO-phe로 분류하였을 경우는 HPO 중에서는 각각 64%와 36%를 차지하고 있는 것으로 나타났다. 또한, HPI를 세분화하여 조사한 결과, HPI에 대한 함량은 HPI-N이 44%, HPI-C가 56%를 차지하고 있는 것으로 나타났다. 분리된 NOM을 이용한 막 오염 평가에서 공극 크기가 100 kDa 이상인 막에서는 HPI-N이 가장 막 오염을 많이 유발하는 NOM으로 나타났고, 다음으로 HPO-car, HPO-HA, HPO-FA, HPI-C, HPO-phe 순으로 나타났다. 또한, 10 kDa 막에서는 HPI-N, HPI-C, HPO-HA, HPO-car, HPO-FA, HPO-phe 순으로 막 오염을 많이 유발하는 것으로 나타났다. 100 kDa 막의 경우 친수성 NOM에 비하여 소수성 NOM에서 상대적으로 $K_s$, $K_i$, $K_c$ 값이 크게 나타났으며 소수성 NOM의 경우 막 공극 내부와 막 공극 표면에서 막 오염을 유발하는 것으로 나타났다. 특히 HPI-N과 HPO-car가 막의 공극 내부에서 막 오염을 일으키는 주요 NOM으로 작용하고 있었다. 10 kDa 막의 경우 소수성 NOM에 비해 친수성 NOM 중 HPI-N이 상대적으로 주된 막 오염 물질로 나타났다. 100 kDa 이상의 공극이 큰 막에서는 소수성 계열의 NOM이 막의 공극내부에서 막 오염을 유발하는 것이 주된 막 오염 메카니즘이었으며, 10 kDa 정도의 공극이 작은 막의 경우 친수성 계열의 NOM이 막 표면에서 막 오염을 유발하는 것이 주된 막 오염 메카니즘이었다. 투과 flux 감소에 대한 NOM의 분자량 분포 영향을 살펴본 결과, 전반적으로 2,000 g/mol 이하의 분자량 범위에서 90% 이상의 분포범위를 나타내고 있어 투과 flux 감소에 대한 유기물 분자량 크기분포의 영향은 없는 것으로 나타났다.

• 한국산업보건학회지
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• 제31권2호
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• pp.173-183
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• 2021

Objectives: This study evaluated the skin permeability of lawsone in henna hair dyes to understand the exposure characteristics of henna hair dyes in the human body. It examined the protective effects of protectants by applying protectants A, B, and C to test skin. Methods: Skin absorption tests were conducted using Franz diffusion cells according to OECD test guideline 428. After applying one kind of natural henna hair dye and chemical henna hair dye, respectively, to a standardized pig skin model, samples of receptor fluid were collected at 1h, 3h, 6h, and 24h. The skin permeation of lawsone was determined using HPLC. After the skin absorption experiment, the skin to which hair dye was applied was analyzed to determine the residual amount of lawsone in the skin. Results: The cumulative permeation of both natural and chemical henna hair dyes increased over time, and the natural henna hair dye had a flux value (t=3.194, p<.05) high both in the K_p value (t=3.207, p<.05) and the residual amount (t=22.701, p<.001). For skin treated with a protectant, the cumulative permeation of natural henna hair dye 24h control and the cumulative permeation of protectant A, B, and C increased over time. Flux and K_p values were in the order control > protectant A > protectant C > protectant B. The residual amount (F=4.469, p<.05) was in the order of protectant C > protectant A > protectant B > control. At 3h, the dye application time of natural henna hair dye, the lawsone flux value (F=4.454, p<.05) and K_p value (F=4.455, p<.05) were higher in the control group than in the protectant groups. The 24h cumulative permeation of the chemical henna hair dye increased with time in both the control and the protectant groups, and the flux and K_p values were in the order of protectant A > protectant C > protectant B > control. The residual amount (F=7.901, p<.01) was in the order of protectant B > protectant A> protectant C > control. Conclusions: Within the normal dyeing time for henna hair dye (three hours for natural henna hair dyes and 30 minutes for chemical henna hair dyes) lawsone skin penetration was not observed even when no protective agent was applied. After that time, however, evidence of skin penetration and retention of lawsone and the protective effect of protective agents were observed.

• Korean Chemical Engineering Research
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• 제48권1호
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• pp.75-79
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• 2010

에틸렌디아민테트라아세트산, 구연산 및 $NH_4Cl$ 융제가 첨가된 분무용액으로부터 분무열분해법에 의해 얇은 막 구조의 전구체 분말들을 합성하였다. $1,200^{\circ}C$에서 소성 과정을 거친 유기 첨가제와 융제를 사용하지 않은 $BaMgAl_{10}O_{17}:Eu$ 형광체는 $1{\sim}5{\mu}m$ 크기의 구형이며, 두꺼운 막 형태의 속이 빈 구조를 가졌다. 반면에 에틸렌디아민아세트산과 구연산을 첨가하여 합성된 BAM:Eu 형광체는 판상 구조의 미세한 크기를 가졌다.$NH_4Cl$ 융제의 첨가량이 0, 6, 35 wt%일때 합성된 미세 형광체들의 결정자 크기는 각각 23, 35, 33 nm였다. 최대의 발광 세기를 나타내는 최적의 융제 첨가량은 형광체의 35 wt%였으며, 융제를 첨가하지 않은 분무용액으로부터 합성된 형광체의 발광 세기의 215%였다.

• 멤브레인
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• 제28권5호
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• pp.368-377
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• 2018

정삼투 공정에 유용한 유도용질로서 n-nitrilotris(methylene) phosphonic acid (NTPA) 염을 합성하였다. NTPA에 첨가하는 KOH의 함량을 변화시켜 NTPA-4K, NTPA-5K, NTPA-6K 세 종류의 유도용질을 합성하고 $^1H$-NMR, $^{13}C$-NMR을 통하여 확인하였다. 유도용질의 물성을 확인하기 위해 삼투압, 점도, 수투과도, 역염 투과도를 측정하였다. 정삼투 공정에서는 증류수를 유입용액으로 사용하고 0.5 M의 유도용액으로 실험한 결과 각각 수투과도는 35.8, 38.8, 42.2 LMH를 나타내고 5.4, 6.9, 7.4 gMH의 역염 투과도를 나타내었다. 이는 기존의 NaCl 유도용액보다 높은 수투과도와 훨씬 낮은 역염 투과도를 확인하였다. 정삼투 공정 후 묽어진 유도용질의 회수를 위해 나노여과 방식으로 상용막을 사용하여 제거율을 측정한 결과 90% 이상의 높은 성능을 확인하였다.

• Korean Chemical Engineering Research
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• 제43권3호
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• pp.407-411
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• 2005

분무용액에 다양한 융제들을 도입하여 분무열분해법에 의해 YAG:Tb($Y_3Al_5O_{12}:Tb$) 형광체들을 합성하였다. 융제의 종류, 유기 첨가물 및 후열처리 온도 등이 YAG:Tb 형광체의 형태, 결정성 및 발광 특성에 미치는 영향 등을 조사하였다. 유기첨가물로 사용된 구연산과 에틸렌 글리콜은 고온의 열처리 과정에서 YAG:Tb 형광체의 형태 파괴 없이 발광 특성을 증대시켰다. 반면에 다량의 융제를 포함한 분무용액으로부터 분무열분해 공정에 의해 합성된 전구체 분말은 $1300^{\circ}C$에서의 후열처리 후에 구형의 형태가 사라졌다. 리튬 탄산염을 융제로 함유한 분무용액으로부터 합성된 YAG:Tb 형광체는 후열처리 후에 미세하면서도 균일한 형태를 가졌다. 융제로서 사용된 리튬 탄산염은 YAG:Tb 형광체의 발광 휘도 개선에도 효과적이었다. 리튬 탄산염을 융제로 첨가한 경우에 합성된 YAG:Tb 형광체의 최적의 발광 세기는 융제를 첨가하지 않은 경우에 합성된 형광체의 발광세기의 189％였다.

• International Journal of Air-Conditioning and Refrigeration
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• 제9권2호
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• pp.85-93
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• 2001

The present study experimentally investigated the effect of refrigeration oil on the condensation heat transfer for R-22 and R-407C in a microfin tube with a U-bend. Mineral oil and POE oil were used for R-22 and R-407C respectively. Experimental parameters were an oil concentration from 0 to 5%, a mass flux from 100 to 400 $kg/m^2s$ and an inlet quality from 0.5 to 0.9. The enhancement factors for both R-22 and R-407C refrigerants at the first straight section decreased continuously as the oil concentration increased. The decreased rapidly as the mass flux decreased and the inlet quality increased. The heat transfer coefficients in the U-bend showed the maximum at the 90$^{\circ}$position. the heat transfer coefficients at the second straight section within the dimensionless length of 48 were larger by a maximum of 33% than the average heat transfer coefficient at the first straight section.

• 한국세라믹학회지
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• 제50권6호
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• pp.485-488
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• 2013

A SiC-$CeO_2$ composite membrane was successfully fabricated using an ally-hydridopolycarbosilane (AHPCS) binder and treated by dip-coating at 60 times with a $CeO_2$ sol solution. The dip-coated SiC membrane was calcined at 773 K and then sintered at 1173 K under an air atmosphere. The coated membrane was characterized by X-ray diffraction (XRD), field-emission scanning electron microscopy (FE-SEM) and a BET surface analysis. The difference in permeation performance between $H_2$ and CO gases was measured by varying the temperature. The permeation flux of $H_2$ on the SiC membrane with layered $CeO_2$ was obtained as $8.45{\times}10^{-6}\;mol/m^2sPa$ at room temperature. The CO permeation flux was $2.64{\times}10^{-6}\;mol/m^2sPa$ at room temperature. The reaction enthalpy (${\Delta}H^{\circ}$) for the hydrogen permeation process was calculated as -7.82 J/mol by Arrhenius plots.