• 전기화학회지
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• 제2권3호
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• pp.123-129
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• 1999

리튬이온전지용 $LiCoO_2$ 전극의 super s black 도전재료의 함량에 따른 초기 충방전 특성을 1 mol/l $LiPF_6/EC+DEC(1:3\;by\;w/w)$의 전해액에서 리튬기준전극에 대하여 4.3 V에서 2.0 V의 전위 구간에 대하여 C/4 및 C/2율로 충방전하여 측정하였다. 최초의 충전과정에서 high impedance충전 특성을 보였으며, super s black도전재료를 $3\%w/w$ 사용한 경우, $0.5 mA/cm^2$ 전류밀도의 충전에서 high impedance의 해소에 따라 $3.82\;{\Omega}\;{\cdot}\;g-LiCoCo_2$의 저항 감소를 나타내었으며, $0.728\;{\Omega}{\cdot}g-LiCoCo_2$의 전극저항과 비교하여 약 7배 높은 값을 나타내었다. 제2차 충전에의 high impedance해소는 약 $63\;{\Omega}{\cdot}g-LiCoCo_2$으로서 전극저항의 $12\%$ 정도이며, 제1차 충전의 high impedance해소에 비하여 $1.7\%$의 수준으로 감소하였다. 제1차 충전 및 방전 비용량은 C/4방전율에서 각각 160-161 및 $153\~155mAh/g-LiCoO_2$으로, 쿨롱효율은 $95.4\~96.4\%$였으며, 비가역 비용량은 약 6 mAh/g-$LiCoO_2$였다. 충전종료 지점에서 측정한 비저항은 도전재료 함량 $2\~7\%w/w$범위에서 낮은 값을 나타내어 비가역 비용량 특성의 변화와 일치하였다. 도전재료의 함량 증가에 따라 용량밀도가 감소하였으며, C/4율 방전에서 super s black함량 $2\%w/w$와 $2.9\%w/w$의 도전재료를 사용한 전극의 용량밀도는 각각 447mAh/ml 및 431 mAh/ml였다

• 한국세라믹학회지
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• 제36권9호
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• pp.923-929
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• 1999

The cause of optical nonlinearity induced in thermally poled silica glass is believed to be the space charge polarization. Since the second order optical nonlinearity (electro-optic effect) can be used in optical switches the optical nonlinearity in silica glass has drawn a large attention. Space charge polarization occurs when an ionic conducting material is subjected to dc electric field by the blocking electrode. Thermal poling performed to induce the optical nonlinearity in silica glass is basically identical to the process generating space charge polarization. As a first step to understand the mechanism of space charge polarization in silica glass hence the induced optical nonlinearity the absorption currents as functions of time were measured for various types of silica glasses and analyzed by the theory of space charge polarization. It was found that the electrical relaxation exhibited a step by the space charge polarization in the relatively long time range and dielectric loss peak showed a maximum at a specific temperature which is depending on type of silica glass. It was turned out that this relaxation might be a cause of nonlinearity in electrical conductivity of silica glass.

• Transactions on Electrical and Electronic Materials
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• 제8권4호
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• pp.182-187
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• 2007

The use of the pulsed electro acoustic (PEA) method allowed us to perform the direct observations of spatio-temporal charge distributions in Electric double layer capacitors (EDLCs) based on polarizable nanoporous carbonaceous electrode. The negative charge density became the maximum, about $205C/m^3$ at the region where was near to collector layer in EDLCs for case $V_{DC}=2.5V$, while the positively charged density became the maximum, about $61.1C/m^3$ at the region where it was located around the cathode layer. The performance of the best sample was found to be better in terms of the charge density (Cs) and specific energy ($E_s$) with a maximum value of ${\sim}8.4F/g$ and 26 Wh/kg. The $C_s$ obtained from the PEA method agreed well with that from the energy conversion method. The PEA measurement used here is a very useful method to quantitively investigates the spatio-temporal charge distribution in EDLCs.

• Macromolecular Research
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• 제8권1호
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• pp.6-11
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• 2000

In this study, we examined the charging behavior of chopped carbon fibers during electro-flocking process, which is one of the key processes of the novel technique for fabricating conductive polymer composite films. Short carbon fibers (CF) during electroflocking were electrically charged by the combined effect of contact charging, corona charging and tribocharging. The specific charge built on CF surface was measured by using Faraday cup method. Specific charge increased not only with increasing electric field strength and potential impressed to mesh electrode as expected from theoretical considerations in literature, but with decreasing mesh opening size due to the improved contact charging condition. However, CF length was found unexpectedly to influence the amount of CF specific charge due to the agglomerated nature of CF flocks leading to the change in charging conditions.

• KIEE International Transactions on Electrophysics and Applications
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• 제3C권5호
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• pp.189-193
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• 2003

Initial irreversible capacity (IIC) can be defined by means of the initial intercalation Ah efficiency (IIE) and the initial irreversible specific capacity at the surface (IICs) with the linear-fit range of the intercalation so as to precisely express the irreversibility of an electrode-electrolyte system. Their relationship was IIC = Qc - Q$_{D}$ = (IIE$^{-1}$ - 1) Q$_{D}$ + IICs in the linear-fit range of IIE. Here, Qc and Qd signify charge and discharge capacity, respectively, based on a complete lithium ion battery cell. Charge indicates lithium insertion to carbon anode. Two terms of IIE and IICs depended on the types of active materials and compositions of the electrode and electrolyte but did not change with charging state. In an ideal electrode-electrolyte system, IIE and IICs would be 100%, 0 mAh/g for the electrode and mAh for the cell, respectively. These properties can be easily obtained by the Gradual Increasing of State of Charge (GISOC).OC).

• 화약ㆍ발파
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• 제27권2호
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• pp.33-41
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• 2009

비장약량 또는 장약계수는 어떤 발파에서 파괴대상이 되는 암석의 총 부피 당 또는 총 무게 당 폭약 소비량으로 정의된다. 암석 톤당 또는 입방미터 당 폭약 소비량의 변화는 언제나 암질변화에 대한 좋은 지표가 된다. 광산현장에서는 통상 광석(ore) 톤당 폭약 소비량을 암석에 대한 발파 용이성의 척도로 사용하는 반면, 건설현장에서는 암석 입방미터 당 폭약 소비량을 사용한다. 본 논문에서는 터널발파를 대상으로 하므로 건설현장에서 사용하는 비장약량의 정의를 채택하였다. 지금까지 다양한 터널발파 설계법들이 제안되어 있지만 이런 방법들을 현장에 적용하였을 때 잘 맞지 않는 경우가 많다. 그 이유는 무엇보다 각 나라나 지역별로 암질조건이 서로 상이하기 때문인 것으로 보이며, 이러한 문제는 발파의 설계자나 시공자에게 기술적으로 상당한 부담이 될 수도 있다. 그런데 만일 우리가 주어진 암석에 대한 적정 비장약량을 알고 있다면 발파설계가 매우 쉬워질 수 있을 것이다. 이런 측면에서 본 논문에서는 사전에 결정된 비장약량이 있는 경우 그 비장약량에 맞추어서 터널발파를 설계할 수 있는 알고리즘을 제안하였다. 이 알고리즘은 터널단면 상의 다양한 영역에 서로 다른 구속도를 부여하는 개념을 토대로 하고 있으며, 기존에 알려진 터널발파 설계방법들과 조합하여 사용할 수 있는 경험적인 설계방법이다.

• KIEE International Transactions on Electrophysics and Applications
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• 제4C권1호
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• pp.21-25
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• 2004

From the gradual increasing state of charge (GISOC) observations, electrochemical behavior of multi-walled carbon nanotube│(lM LiP $F_{6}$ , EC,DEC,DME 3:5:5 volume ratio)│lithium cells was evaluated using the galvanostatic charge-discharge process. A MWCNT delivers a specific charge capacity of 1,300 mAh/g in a Li cell when cycled up to an end voltage of 0 V (vs. Li/L $i^{＋}$ )at a constant current rate every 10 hours. However, in the present study, the specific discharge capacity obtained is 338 mAh/g, thus amounting to a coulombic efficiency of only 26％. Further, when the MWCNT│Li cells were tested using the GISOC method, two distinguishable linear-fit ranges were observed due to the intercalation/deintercalation of lithium, which were found to have II $E_1$, IIC $s_1$ and II $E_2$of 27.3％, 372 mAh/g, and 25.5％, respectively. Q $c_1$, could be calculated from the data of IIE and IICs of each range by the modified equation "II $C_{sum}$= $\Sigma$( $Q_{C}$- $Q_{D}$)=(II $E_{1}$$^{-1}$ ) $Q_{Dl}$ ＋(II $E_2$$^{-1}$ -1) ( $Q_{D2}$- $Q_{Dl}$ ) ＋ IIC $s_1$= $Q_{Cl}$ - $Q_{Dl}$ ". Results of the GISOC method could be converted to the results of galvanostatic charge-discharge process, irrespective of the state of charge of the cell or battery.ery.y.y.

• 산업기술연구
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• 제26권A호
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• pp.17-28
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• 2006

In underground drilling and blasting, particularly in small headings(generally under $20m^2$), the prospects for changes of blast parameters are usually more limited than those employed by large area tunnel(over $20m^2$). It is also well known that the consumption of explosives and specific drilling rate for small tunnel areas are exponentially increased also tunnel areas decrease. To confirm above results, some tests for two tunnels(irrigation water tunnel with $6.0m^2$ area, electric supplies tunnel with $15.0m^2$) are also carried out in this study. As a results, specific drilling rate and specific charge for irrigation water tunnel were decreased from 13.8 to $7.7m/m^3$ and from 4.88 to $2.56kg/m^3$ respectively. Those for electric supplies tunnel were also decreased from 8.0 to $4.9m/m^3$ and from 3.46 to $2.22kg/m^3$.

• 폴리머
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• 제25권5호
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• pp.719-727
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• 2001

유기광도전체에 있어서의 액정은 종래의 분자 배향성을 가지지 않는 비정성 고체계와는 달리 분자 배향성을 가지기 때문에 분자 사이의 질서도가 높아지게 되고, charge-carrier의 hopping을 방해하는 hopping site의 공간적인 틈이 작아져 고 이동도의 특성을 가질수 있다. 본 연구에서는 유기광도전체의 전하 수송층에 액정5CT를 혼합하여, charge-carrier수송특성에 있어서의 액정5CT의 영향을 관찰하였다. 액정5CT를 함유한 유기광도전체는 액정의 혼합비가 증가함에 따가 초기전위는 증가하였으며, 암감쇄는 감소하는 경향을 나타내었다. 감도는 5CT를 TNF와 OXD 각자에 대하여 40 wt%로 혼합한 시료의 경우에 가장 우수하게 나타났다. 형광거동을 관찰한 결과, 이는 전하수송재료와 액정5CT의 전하 수송착체에 의한 것으로, 액정5CT를 TNF와 OXD 각각에 대하여 40 wt%로 혼합한 시료의 경우가 다른 시료에 비해 전하 수송착체가 가장 잘 형성되어, 성공을 잘 수송하기 때문으로 나타났다.

• Clinical and Experimental Pediatrics
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• 제57권1호
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• pp.46-49
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• 2014

CHARGE syndrome has been estimated to occur in 1:10,000 births worldwide and shows various clinical manifestations. It is a genetic disorder characterized by a specific and a recognizable pattern of anomalies. The major clinical features are ocular coloboma, heart malformations, atresia of the choanae, growth retardation, genital hypoplasia, and ear abnormalities. The chromodomain helicase DNA-binding protein 7 (CHD7) gene, located on chromosome 8q12.1, causes CHARGE syndrome. The CHD7 protein is an adenosine triphosphate (ATP)-dependent chromatin remodeling protein. A total of 67% of patients clinically diagnosed with CHARGE syndrome have CHD7 mutations. Five hundred twenty-eight pathogenic and unique CHD7 alterations have been identified so far. We describe a patient with a CHARGE syndrome diagnosis who carried a novel de novo mutation, a c.3896T>C (p. leu1299Pro) missense mutation, in the CHD7 gene. This finding will provide more information for genetic counseling and expand our understanding of the pathogenesis and development of CHARGE syndrome.