• Korean Journal of Materials Research
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• v.5 no.7
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• pp.835-841
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• 1995

The deposition properties of Si$_3$N$_4$ deposited by low pressure chemical vapor deposition were studied to evaluate Si$_3$N$_4$as part of multi-layer coatings for anti-oxidation and anti-wear coating of graphite in the propellant-burning environment. Si$_3$N$_4$was deposited on the pack-SiC coated graphite and the tendencies of deposition rate and surface morphology changes with temperatures and reaction gas ratios were investigated. In low deposition temperatures the deposition rate increased tilth increasing temperature but in high temperatures the deposition rate decreased with increasing temperature. The grain size of Si$_3$N$_4$decreased with increasing temperature. In condition that the range of reaction gas ratios is 20$\leq$NH$_3$/SiH$_4$$\leq$40, the deposition rate and surface morphology did not change. The Si$_3$N$_4$deposited at 800~130$0^{\circ}C$ was amorphous, and by post-annealing at 130$0^{\circ}C$ in a $N_2$ambient, the Si$_3$N$_4$crystalized.

• Journal of the Korean Electrochemical Society
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• v.7 no.1
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• pp.32-37
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• 2004

The charge/discharge capacity of natural graphite anode in lithium secondary batteries was examined as a function of charge/discharge rate. When the natural graphite anode was galvanostatically cycled in the range of 0.0-2.0V $(vs.\;Li/Li^+)$, the charging capacity decreased with an increase in the charging rate, which is caused by an earlier approach to the charging cut-off (0.0 V) before the complete charging that is in turn caused by an ever-increasing overpotential at higher rates. Even if the overpotential of discharging reaction also increased at higher discharge rates, the discharging reaction took place in the range of 0.0-0.3 V that is far below the discharge cut-off (2.0 V). As a result, the discharge capacity was not affected by the discharge rate because all the lithium ions once intercalated are fully discharged even at high current condition. As the overpotential of lithium deposition reaction also increased at high current condition, the charge capacity of natural graphite could be enlarged by lowering the charging cut-off voltage below 0.0 V, There is, however, a limitation for the lowering of cut-off voltage because the resistance for lithium deposition is smaller than that of lithium intercalation into graphite. When the charge cut-off voltage was lowered down to -0.04 V under IC condition, lithium ions were inserted into graphite without lithium deposition such that the discharge capacity could be raised up to $11\%$.

• Proceedings of the KIEE Conference
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• 2002.07c
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• pp.1559-1561
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• 2002

적외선 확산반사형 결정화유리를 응용한 레이저 여기용 공진기를 제작하여 미세구조 분석 및 레이저 여기 효율특성을 조사하였다. 출발물질로는 Cordierite를 주결정상으로 하는 MAS(MgO, $Al_2O_3$, $SiO_2$) 3성분계 조성에 결정화 유도용 조핵제로 $TiO_2$를 첨가하였으며, 형성된 유리 용융물을 흑연제 몰드에 부어 공진기를 제조하였다. 용융물 중 일부를 2단계 열처리를 행하여 상분석을 실시한 결과 Cordierite($2MgO{\cdot}2Al_2O_3{\cdot}5SiO_2$)와 Rutile($TiO_2$)이 주결정상으로 관찰되었으며, 열처리 온도를 변화시켜 생성된 입자의 크기에 따른 확산반사율간의 관계를 조사한 결과, $1100{\sim}1200nm$에서 열처리된 시편의 경우 $500{\sim}2200nm$의 영역에서 95% 이상의 확산반사율을 나타내었다. 대표적인 고체레이저인 Nd:YAG의 경우, $700{\sim}900nm$ 파장이 주흡수대이며, 이를 결정화유리로 제조된 공진기의 레이저 효율특성실험에 이용하였다. 수냉 및 단일 펄스의 조건에서 $1.7{\sim}1.9%$의 효율을 나타내었다.

• The Journal of Natural Sciences
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• v.10 no.1
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• pp.1-7
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• 1998

A Lennard-Jones fluid layer adsorbed on a smooth solid surface was studied at coverages $\theta$ ~ 0.8 to 1.8 on an isotherm by performing intensive grand canonical Monte Carlo simulations. The results clearly show a picture of two-step melting process which used to be observed in recent thermodynamic measurements of argon monolayer melting on graphite. The observed melting process consist of an abrupt density change followed by a gradual transition. Snapshots of monolayer configurations indicate that the creation and dissociation of a dislocation pair are involved in the melting mechanism. Taking the effect of system size into account, it is suggested that, while the abrupt density change may be not related to the theory of Kosterlitz, Thouless, Halperin, Nelson, and Young (KTHNY), the second gradual transition is probably a KTHNY-type melting transition.

• Journal of Powder Materials
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• v.28 no.1
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• pp.13-19
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• 2021

Bulk graphite is manufactured using graphite scrap as the filler and phenolic resin as the binder. Graphite scrap, which is the by-product of processing the final graphite product, is pulverized and sieved by particle size. The relationship between the density and porosity is analyzed by measuring the mechanical properties of bulk graphite. The filler materials are sieved into mean particle sizes of 10.62, 23.38, 54.09, 84.29, and 126.64 ㎛. The bulk graphite density using the filler powder with a particle size of 54.09 ㎛ is 1.38 g/㎤, which is the highest value in this study. The compressive strength tends to increase as the bulk graphite density increases. The highest compressive strength of 43.14 MPa is achieved with the 54.09 ㎛ powder. The highest flexural strength of 23.08 MPa is achieved using the 10.62 ㎛ powder, having the smallest average particle size. The compressive strength is affected by the density of bulk graphite, and the flexural strength is affected by the filler particle size of bulk graphite.

• Journal of Adhesion and Interface
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• v.15 no.2
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• pp.63-68
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• 2014

Hollow mesoporous carbon nitride material with sphere shape was synthesized using polystyrene sphere as template and cyanamide as nitrogen and carbon atom sources via thermal treatment process. The process of the silica removal is not necessary because silica as template is not in use for the synthesis of hollow mesoporous carbon nitride material and any solvents are also not in use. The size of polystyrene spheres was about 170 nm. Hollow diameter and wall thickness were 82 nm and 13 nm, respectively, in hollow mesoporous carbon nitride sphere. Surface area, mesopore size and pore volume of hollow mesoporous carbon nitride material was $188m^2g^{-1}$, 3.8 nm and $0.35cm^3g^{-1}$, respectively. The wall in hollow sphere has graphitic structure. Hollow mesoporous carbon nitride material has potential applications in the area of fuel cell, catalysis, photocatalysis, electroemmision device, etc.

• Applied Chemistry for Engineering
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• v.19 no.2
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• pp.185-190
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• 2008

In order to increase the surface area of electrodes for electrosorption, porous carbon electrodes were fabricated by a wet phase inversion method. A carbon slurry consisting of a mixture of activated carbon powder (ACP), polyvinylidene fluoride (PVdF), and N-methyl-2-pyrrolidone (NMP) as a solvent was cast directly on a graphite sheet. The cast film was then immersed in pure water for phase inversion. The physical and electrochemical properties of the electrodes were investigated using scanning electron microscopy (SEM), porosimetry, and cyclic voltammetry. The SEM images verified that the pores of various sizes were formed uniformly on the electrode surface. The average pore sizes determined for the electrodes fabricated with various NMP contents ranged from 64.2 to 82.4 nm and the size increased as the NMP content increased. All of the voltammograms showed a typical behavior of charging and discharging characteristic at the electric double layer. The electrical capacitance ranged from 3.88 to $5.87F/cm^2$ depending on the NMP contents, and the electrical capacitance increased as the solvent content decreased. The experimental results showed that the solvent content is an important variable controlling pore size and ultimately the capacitance of the electrode.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.26 no.1
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• pp.8-13
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• 2016

A top-seeded solution growth (TSSG) is a method of growing SiC single crystal from the Si melt dissolved the carbon. In this study, multiphysics modeling was conducted using COMSOL Multiphysics, a commercialized finite element analysis package, to get analytic results about electromagnetic analysis, heat transfer and fluid flow in the Si melt. Experimental results showed good agreements with simulation data, which supports the validity of the simulation model. Based on the understanding about solution growth of SiC and our set-up, crystal growth was conducted on off-axis 4H-SiC seed crystal in the temperature range of $1600{\sim}1800^{\circ}C$. The grown layer showed good crystal quality confirmed with optical microscopy and high resolution X-ray diffraction, which also demonstrates the effectiveness of the multiphysics model to find a process condition of solution growth of SiC single crystal.

• Korean Chemical Engineering Research
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• v.56 no.6
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• pp.901-908
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• 2018

Graphite is used as a sample anode active material. However, since the maximum theoretical capacity is limited to $372mA\;h\;g^{-1}$, a new anode active material is required for the development of a high capacity lithium ion battery. The maximum theoretical capacity of Si is $4200mA\;h\;g^{-1}$, which is higher than that of graphite. However, it is not suitable for direct application to the anode active material because it has a volume expansion of 400%. In order to minimize the decrease of the discharge capacity due to the volume expansion, the Si was pulverized by the dry method to reduce the mechanical stress and the volume change of the reaction phase, and the change of the volume was suppressed by coating the carbon layers to the particle size controlled Si particles. And carbon fiber is grown like a thread on the particle surface to control secondary volume expansion and improve electrical conductivity. The physical and chemical properties of the materials were measured by XRD, SEM and TEM, and their electrochemical properties were evaluated. In this study, we have investigated the synthesis method that can be used as anode active material by improving cycle characteristics of Si.

• Proceedings of the Korean Vacuum Society Conference
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• 2015.08a
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• pp.134-134
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• 2015

최근 액체 플라즈마에 대한 주된 이슈는 방전에 의해 발생하는 히드록실라디칼(OH-)과 버블이다. 액체 플라즈마를 이용한 다양한 응용분야에서는 히드록실라디칼에 주목하고 있다. 액체 플라즈마는 그래핀 파생물의 용액 친화도 향상을 위해 이용될 수 있다. 흑연이 포함된 과산화수소(H2O2) 용액에서 전기적인 방전으로 만들어진 히드록실라디칼로 그래핀 파생물의 용액 친화도를 향상시킨다. 이는 잠재적인 프린팅(printing) 기술 발전에 기대된다. 그리고 이 라디칼은 폐수에서 발암성의 트라이클로로아세트산(CCl3COOH)을 탈 염소하고 분해하는 역할을 하여 액체 플라즈마가 새로운 수처리 기술로 부상되고 있다. 또한 인체에서는 살균 작용을 하는 것 뿐만 아니라 단백질 고리를 끊는 역할을 하여 전립선 수술과 같은 인체수술에 적용될 수 있다. 최근 액체 플라즈마를 이용한 돼지 각막 임상수술에서 레이저와 필적할 정도로 매우 정밀하게 수술된 연구결과가 발표되어 인체 각막수술 적용에 기대된다. 이처럼 액체 플라즈마를 이용한 대부분의 응용분야에서 히드록실라디칼의 역할이 중요하다. 액체 플라즈마의 또 다른 이슈인 버블은 2가지의 역할을 한다. 첫 번째로 방전소스의 역할이다. 액체 속에 담긴 얇은 전극에 전압을 인가하면 전극 주변에서 강한 전기장의 발생으로 줄열(joule heating)에 의해 버블이 생성된다. 전극에서 버블이 생성되었을 때, 서로 다른 유전율을 가진 두 물질로 나누어진다. (버블 안은 공기로 상대 유전율 ${\varepsilon}r{\fallingdotseq}=1$, 용액은 ${\varepsilon}r{\fallingdotseq}=80$이다.) 시스템에 인가된 전압이 항복 전압(breakdown voltage)을 넘어서면 유전율이 상대적으로 낮은 버블내부에 강한 전기장이 걸리게 되어 방전이 일어난다. 만약 버블이 존재하지 않는다면 방전을 위해서 매우 높은 전압이 필요하다. 따라서 버블은 플라즈마 방전의 소스역할을 한다. 두번째로 버블은 전극의 부식을 방지하는 역할을 한다. 전극 부식은 주로 전기분해로 인한 산화반응에 의해 발생하는데 버블을 전극에 오래 머무르게 하면 부식을 방지할 수 있다. 이처럼 액체 플라즈마 시스템에서 버블의 역할들은 상당히 중요하다. 일반적으로 버블은 시스템에 인가하는 전원, 전극 극성 그리고 전압크기에 따라 거동이 달라진다. 시스템에 AC파워를 인가하면 버블은 주파수가 높을수록 전극에서 떨어지는 속도가 빨라지는 특성을 보인다. 핀 전극 극성이 음극일 때는 양극일 때보다 버블이 더 잘 생성된다. 또한 인가전압크기에 따라 거동이 달라지며 시스템에 같은 전압을 인가하여도 크기가 항상 같지 않고, 거동도 일관성을 보이지 않은 랜덤적인 모습을 보인다. 본 연구에서는 이 랜덤적인 버블의 거동을 정리하고 응용분야에서 중요하게 여기는 히드록실라디칼 생성에 대해 공부하기 위해 염류 용액(saline solution)에 핀(pin)-면(plane) 전극 구조를 설치하여 10Hz 주파수(1% duty cycle)를 가진 0-600V 구형펄스로 실험하였다. 실험을 통한 결과로서 랜덤적인 버블의 거동을 전극에서 버블이 떨어지는 속도와 플라즈마 특성에 따라 슈팅모드(shooting mode)와 유지모드(keeping mode) 2가지 모드로 분류하였다. 슈팅모드에서는 버블이 핀 전극에서 성장하지 못하고 빠른 속도로 떨어지는 모드로 플라즈마 방전이 잘 이루어지지 않는다. 반면 유지모드에서는 버블이 핀 전극에서 떨어지지 않고 지속적으로 성장한다. 이 모드에서는 펄스 시간 동안 하나의 버블로 연속적인 방전이 가능하다. 방전이 일어날 때 발생하는 히드록실라디칼의 생성은 버블 내부의 쉬스와 관련이 있다. 이 라디칼을 만들기 위해서는 높은 에너지가 요구되기 때문에 버블 내부의 쉬스(sheath)에서 만들어진다. 펄스 동안 쉬스는 주로 핀 전극 주변에서 유지되며 히드록실라디칼은 이곳에서 주로 만들어진다. 따라서 버블과 함께 쉬스도 성장하는 버블유지모드에서 슈팅모드보다 히드록실라디칼이 더 많이 생성된다.