• 한국전기화학회:학술대회논문집
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• 한국전기화학회 2001년도 연료전지심포지움 2001논문집
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• pp.179-184
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• 2001

The diffusion layer within MEA(membrane electrode assembly) has been evaluated important factor for improvement of cell performance in DMFC. The diffusion layer in MEA structure leads to the reduction of catalyst loss in active catalysts layer as well as prevention of water-flooding in cathode. Cell performance is directly affected by interior properties of diffusion layer materials. Acetylene Black and $RuO_2$ with large pore size and low porosity compared to Vulcan XC-72R gave better performance caused by vigorous methanol diffusion and water removal. And $RuO_2$ as diffusion layer materials showed different behavior in anode and cathode compartment, that is, diffusion layers in anode and cathode side make methanol diffusion and water removal facilitate, respectively.

• Investigative Magnetic Resonance Imaging
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• 제6권2호
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• pp.158-165
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• 2002

목적: 체내에 주입된 Gd-DTPA가 뇌의 확산강조 자기공명영상 신호강도 및 현성확산계수에 미치는 영향을 알아보았다. 대상 및 방법 : 성숙한 잡견 5마리에 대하여 동맥내 도관삽입에 의한 좌측 내경동맥 색전방법을 이용하여 초급성 뇌경색 동물모델을 만들었다. 색전 후 1시간째 확산강조영상을 시행하고, Gd-DTPA를 주입한 다음 다시 90분까지 11회의 추가 확산강조영상을 얻었다. 관심영역을 설정하여 측정한 초급성 뇌경색부위와 반대측 정상부위의 확산강조영상 신호강도 및 현성확산계수를 분석하였다. 결과: 뇌경색은 색전 후 1시간에 시행한 확산강조 자기공명영상에서 잡견 5마리 모두에서 발견되었다. 확산강조영상에서 초급성 뇌경색부위의 신호강도는 Gd-DTPA 주입 여부와 관계없이 시간이 경과함에 따라 증가하였으나, 관류가 유지된 정상부위의 신호강 도는 Gd-DTPA 주입 후 2분에 시행한 첫 검사에서 오히려 저하된 후, 시간경과에 따라 다시 증가하였다. 현성확산계수는 초급성 뇌경색부위에서 Gd-DTPA주입여부에 관계없이 시간 이 경과함에 따라 지속적으로 감소되었으나, 관류가 유지된 반대측 정상부위에서는 변화하지 않았다. 결론: 체내에 주입된 Gd-DTPA는 초급성 뇌경색부위 및 정상부위의 현성확산계수에 영향을 미치지 않으나, 정상부위에서는 조영제 주입 직후 초기의 자화율효과에 의해 확산강조영상의 신호 강도를 저하시켰다. 조영제 주입 후 시행한 확산강조영상 신호 강도의 정량적인 측정이 필요한 연구 혹은 임상 증례에 대하여는 현성확산계수를 측정함으로써 Gd-DTPA의 자화율효과에 의한 영향을 배제하여야 할 것이다.

• 한국지반환경공학회 논문집
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• 제3권1호
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• pp.13-26
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• 2002

본 연구에서는 아연 및 카드뮴의 확산계수에 미치는 온도영향에 대한 연구를 위해 $15^{\circ}C$와 $55^{\circ}C$에서 확산실험을 수행하였다. 온도변화에 따른 유효확산계수의 변화를 비교할 경우 두 금속 모두에서 $55^{\circ}C$에서의 유효확산계수가 $15^{\circ}C$에서의 확산계수에 비해 최대 10배까지 큰 것으로 나타났다. 그리고 온도증가에 따른 확산속도의 증가와 더불어 중금속들의 흡착량 또한 증가하는 것으로 나타났다. 그러므로 지연인자를 얻는 방법의 차이에 따라 비교적 흡착량을 과다하게 평가하는 흡착실험을 통해 얻은 지연인자를 이용하여 유효확산계수를 산정할 경우 확산계수를 과대평가 할 수 있다. 그리고 연속추출 실험 결과, 아연의 경우에는 탄산염 형태로의 분배경향이 가장 크게 나타났고, 카드뮴의 경우에는 이온교환형태로의 분배가 가장 크게 나타났다. 특히 실험을 수행한 온도가 증가함에 따라 아연 확산실험의 경우에는 탄산염 형태와 유기물 형태로의 분배가 증가하는 것으로 나타났다. 반면 카드뮴 확산실험의 경우에는 온도변화와 무관하게 60%이상이 이온교환 형태로 분배됨을 알 수 있었다.

• 대한기계학회논문집B
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• 제21권4호
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• pp.494-502
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• 1997

Experiments on corresponding jet flames with stagnant point diffusion flames have been carried out in initial injection periods. A compensated measurement of maximum flame temperature, which is based on the ion signal, has been employed to inspect flame responses to time-varying strain rates. The flame responses are obtained at two conditions for the slowly time-varying strain rate and the case of flame extinction, and analyzed to confirm similarity between a stagnant point diffusion flame and an evolving jet diffusion flame. Nonsteady effects are addressed via the comparison between several time scales. The time variation with low strain rates, in which illustrates the flame behavior of the upper branch far from extinction in the well-known S-curve, is confirmed to produce a quasi-steady flame response through the nonsteady experiments. The time variation with strain rates in the case of flame extinction indicates an unsteady effect of flame response. It is therefore found that the flame responses near jet tip depend on time histories of characterized strain rates in the developing process.

• Corrosion Science and Technology
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• 제16권4호
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• pp.201-208
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• 2017

A finite element analysis is proposed to study the effect of specimen dimensions on lateral diffusion of hydrogen during hydrogen permeation flux measurements. The error of measurement on thick specimens because of 1D diffusion approximation may be as much as 70%. A critical condition for accurate measurements is to designate the area of hydrogen monitoring/exit surface smaller than the area of hydrogen charging/entry surface. For thin to medium thickness specimens (ratio of thickness to specimen radius of 5:10 and below), the charging surface should be maximized and the monitoring surface should be minimized. In case of relatively thick specimens (ratio of thickness to specimen radius above of 5:10), use of a hydrogen-diffusion barrier on the specimen boundaries is recommended. It would completely eliminate lateral losses of hydrogen, but cannot eliminate the deviation towards 2D diffusion near the side edges. In such a case, the charging surface should be maximized and the monitoring surface should be as closer in dimension as the charging surface. A regression analysis was carried out and an analytical relationship between the maximum measurement error and the specimen dimensions is proposed.

• Bulletin of the Korean Chemical Society
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• 제5권6호
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• pp.249-253
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• 1984

Mutual diffusion coefficients of choline chloride were determined by using the diaphragm cell method in aqueous solutions of chondroitin sulfate A at $25^{\circ}C$. The diffusion coefficients of choline chloride in 0.1g/100ml, 0.5g/100ml and 1g/100ml respectively of chondroitin sulfate solutions were compared with those of binary systems of water-choline chloride. At low concentrations, the diffusion coefficients of the choline chloride in the presence of chondroitin sulfate were significantly smaller than the values obtained in the absence of chondroitin sulfate, indicating a strong interaction between these solutes. The effect of this interaction on the diffusion of choline ion is largest at higher chondroitin sulfate concentrations and at lower choline chloride concentrations. The influence of chondroitin sulfate is overcome at higher choline chloride concentrations. Self-diffusion coefficients of choline ion in the presence of chondroitin sulfate are also obtained. Excellent agreements were obtained between the experimental data and the calculated values obtained by using the Manning's equations. These observations suggest that the interaction between choline chloride and chondroitin sulfate involves primarily a long range electrostatic effect and there is no appreciable "condensation" or binding of choline ion to the chondroitin sulfate.

• 한국연소학회지
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• 제17권1호
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• pp.58-65
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• 2012

The influence of magnetic field on propane and acetylene diffusion flames have been experimentally investigated using an electromagnetic system. Periodically induced magnetic field having various frequencies and duty ratios was established in square wave form. The maximum intensity and gradient of magnetic field were 1.3 T and 0.27 T/mm, respectively. The width of a propane flame was reduced up to 4.5% and the brightness was enhanced up to 25% when the magnetic field was induced. The soot emission from an acetylene flame was ceased when magnetic field was induced. The alteration of flow field, which is due to the paramagnetic characteristics of oxygen molecule, is most likely to be responsible for the change in flame size and brightness. The effect of magnetic field on diffusion flames, which competes with the gravitational effect, was more apparent from a smaller size flame. The magnetic field effect, therefore, could be important under microgravity conditions. Since the time required to alter the flow field must be finite, the magnetic field effect is likely to be less significant for a periodically oscillating magnetic field at a high frequency or having a small duty ratio.

• 한국자기공명학회논문지
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• 제20권2호
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• pp.61-65
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• 2016

Undesirable convective flow in an NMR tube inhibits the accurate measurement of diffusion coefficients by NMR spectroscopy. To minimize the convection effects, various methods have been suggested, and it has been known that the use of sample rotation can be useful. However, it has not been clearly examined that the convection suppressing effect of the sample rotation under the different spinning speeds. In this study, the relation between convective flow and the sample rotation was investigated using PGSE NMR diffusion experiments to reveal the feasibility for controlling the convective flow in an NMR tube by sample rotation itself. The viscosity effect was also examined using solvents with four different viscosities, acetone-$d_6$ chloroform-d, pyridine-$d_5$, and $D_2O$. The sample rotation showed apparent convection suppressing effects at all temperature range for the low viscosity solvents, acetone-$d_6$ and chloroform-d, even at the faster than 5 Hz spinning rate. The similar patterns were also observed for pyridine-$d_5$ and $D_2O$, which have higher viscosity. This effect was observed even at high temperatures where convective flow arises conspicuously.

• 한국분말재료학회지
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• 제23권6호
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• pp.432-436
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• 2016

We investigate the microstructural and magnetic property changes of $DyH_2$, $Cu+DyH_2$, and $Al+DyH_2$ diffusion-treated NdFeB sintered magnets with the post annealing (PA) temperature. The coercivity of all the diffusion-treated magnets increases with increasing heat treatment temperature except at $910^{\circ}C$, where it decreases slightly. Moreover, at $880^{\circ}C$, the coercivity increases by 3.8 kOe in Cu and 4.7 kOe in Al-mixed $DyH_2$-coated magnets, whereas this increase is relatively low (3.0 kOe) in the magnet coated with only $DyH_2$. Both Cu and Al have an almost similar effect on the coercivity improvement, particularly over the heat treatment temperature range of $790-880^{\circ}C$. The diffusivity and diffusion depth of Dy increases in those magnets that are treated with Cu or Al-mixed $DyH_2$, mainly because of the comparatively easy diffusion path provided by Cu and Al owing to their solubility in the Nd-rich grain boundary phase. The formation of a highly anisotropic $(Nd,\;Dy)_2Fe_{14}B$ phase layer, which acts as the shell in the core-shell-type structure so as to prevent the reverse domain movement, is the cause of enhanced coercivity of diffusion-treated Nd-Fe-B magnets.

• Journal of Advanced Marine Engineering and Technology
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• 제30권1호
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• pp.140-149
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• 2006

Characteristics of a laminar diffusion flame placed near wall in microgravity have been numerically analyzed in a two-dimension. The fuel for the flame is $C_2H_4$. The flame is initiated by imposing a high temperature ignition source. The flow field, temperature field, and flame shape in microgravity diffusion flame are detailed. Especially, effects of surrounding air velocity and fuel injection velocity on the microgravity diffusion flame have been discussed accounting for standoff distance. And, the effect of curvature rate has been also studied. The results showed that velocities in a diffusion flame were overshoot because of volumetric expansion and distribution of temperature showed regularity by free-buoyancy This means that the diffusion flame in microgravity is very stable, while the flame in normal gravity is not regular and unstable due to buoyancy. Standoff distance decreases with increase in surrounding air velocity and with decrease in fuel injection velocity. With increasing curvature rate, the position of reaction rate moves away the wall.