• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 1997년도 춘계학술대회 논문집
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• pp.107-110
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• 1997

LiMn$_2$O$_4$ is prepared by reacting stoichiometric mixture of LiOH . $H_2O$ and MnO$_2$ (mole ratio 1 ; 1) and heating at 80$0^{\circ}C$, $700^{\circ}C$ for 24h, 36h, 48h, 60h and 72h. We obtained through X-ray diffraction that lattice parameter varied as function of calcined temperature and time. Cathode active materials calcined at 80$0^{\circ}C$ for 36h, (111)/(311) peak ratio was 0.37. It showed good charge/discharge characteristics. When (111)/(311) peak ratio was 0.37, it was that crystal structure is formed very well. In the result of charge/discharge test, when heated at 80$0^{\circ}C$ for 36h, charge/discharge characteristics of LiMn$_2$O$_4$ is the best.

• Journal of Electrochemical Science and Technology
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• 제2권1호
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• pp.14-19
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• 2011

Quasi-equilibrium profiles are analyzed through galvanostatic intermittent titration technique (GITT) and potentiostatic intermittent titration technique (PITT) to study the charge/discharge mechanism in multicomponent olivine structure ($LiMn_{1/3}Fe_{1/3}Co_{1/3}PO_4$). From GITT data, the degree of polarization is evaluated for the three regions corresponding to the redox couples of $Mn^{2+}/Mn^{3+}$, $Fe^{2+}/Fe^{3+}$ and $Co^{2+}/Co^{3+}$. From PITT data, the current vs. time responses are examined in each titration step to find out the mode of lithium de-intercalation/intercalation process. Furthermore, lithium diffusivities at specific compositions (x in $Li_xMn_{1/3}Fe_{1/3}Co_{1/3}PO_4$) are also calculated. Finally, total capacity ($Q^{total}$) and diffusional capacity ($Q^{diff}$) are obtained for some selected voltage steps. The entire study consistently confirms that the charge/discharge mechanism of multicomponent olivine cathode is associated with a one-phase reaction rather than a biphasic reaction.

• 한국정보디스플레이학회:학술대회논문집
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• 한국정보디스플레이학회 2003년도 International Meeting on Information Display
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• pp.722-725
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• 2003

In AC plasma display, it is very important to quantify the wall voltage induced by the wall charge accumulated on the dielectric surface. If we know the quantities of the wall voltage in each period of every sequence; reset period, address period and sustain period, then it helps us to design the optimal driving waveform for high efficiency plasma display. We develop a new method to measure the wall voltage with VDS (Versatile Driving Simulator) system. From this method the wall voltage induced by a wall charge profiles just after the reset discharge of every cells in plasma display panel can be investigated and analyzed successfully. It is noted that the wall voltage profiles are influenced by the space charge and then they are stabilized as time goes by. It is also noted that both the remaining wall charge at the previous sequence and space charges contribute to wall voltage quantities just after the reset discharge. It is noted that the wall charges contribute dominantly after a few hundreds microseconds, while the space charges have been decayed within 100 ${\mu}s$ just after the reset discharge.

• Journal of Biosystems Engineering
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• 제31권2호
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• pp.108-114
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• 2006

This study was conducted to design and fabricate a controller for variable-rate application of granular fertilizer based on physical and chemical information, to analyze the performance of the controller and characteristics of a discharger. The result of the study are summarized as follows: 1. The charge ratios of discharger by accumulation heights of fertilizer in hopper were examined, and the variations in charge ratio were $72.58{\sim}93.33%$ and $63.14{\sim}94.42%$ for the fertilizers Super 21 and Sinsedae, respectively. The charge ratio also decreased as the rotational speed of discharger increased. 2. The coefficient of variation of discharge amount by rotational speed and discharge time of discharger were in the range of $2.94{\sim}11.23%$ and $2.82{\sim}10.80%$ for the fertilizer of Super 21 and Sinsedae. Except the rotational speed of 12 rpm, the coefficient of variation for discharge amount were relatively small with 4% more or less 3. In order to evaluate the rotational speed of discharger, the control signal in the range of $0{\sim}5V$ was subdivided into the 50 steps by 0.1V. The regression equation for the rotational speed of discharger was Y=55.984X-79.174(X: input voltage, V, Y: discharger speed, RPM) and the $R^2$ was 0.99. 4. In order to evaluate the performance of the controller for variable-rate application of granular fertilizer, settling time to unit step input was examined. The settling time varied from 0.8sec to 1.4 sec.

• 한국산학기술학회논문지
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• 제10권2호
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• pp.230-236
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• 2009

본 논문에서는 신재생 에너지 활용을 위한 그늘막 형태의 연계 계통형 태양광 발전 시스템을 제안한다. 제안하는 발전 시스템은 성하기에 해수욕장을 찾는 피서객들에게 상용전원과 연계 계통하여 최대 전력 수요를 충족시킬 뿐 만 아니라 그늘막으로서의 기능을 갖도록 설계하였다. 태양전지에서 생성된 전기를 낮 시간 동안 축전지에 충전하면 이를 야간에 전등이나 선풍기등에 이용할 수 있다. 축전지를 충전할 때 축전지의 성능을 유지하려면 충방전컨트롤러가 필요하다. 제안하는 축전지 충방전 컨트롤러는 고성능 마이크로프로세서를 사용하여 정확하고 안정된 동작을 하도록 설계하였고 사용자의 편의를 위해 디지털 표시기 및 축전지 교체시기 경보장치등을 갖추고 있다. 제안하는 발전 시스템을 영동 지역 해수욕장에 설치하고 실험을 통하여 전력 생산능력과 발전 성능을 확인하였다.

• Design & Manufacturing
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• 제2권5호
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• pp.39-42
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• 2008

The Paper discussed the effects of working electric current and pulse when using super hardend alloy drill as corona electrode. The discharge effect can be obtained very precisely in the ranges of 1A - 2A in working current. $12{\mu}s-14{\mu}s$ in dis charge pulse on time width and $8{\mu}s-10{\mu}s$ in discharge pulse off time.

• 전기화학회지
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• 제4권3호
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• pp.113-117
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• 2001

탄소계 전극을 사용하는 EDLC(Electric Double Layer Capacitor)용의 축전용량과 충방전속도는 전해질의 종류, 충방전 조건 그리고 탄소계 물질의 물리화학적 성질에 따라 크게 달라질 수 있다. 이에 본 연구에서는 dip coating method에 의해 제조된 EDLC용 활성탄소 전극에서 유기 전해질의 종류를 달리하여 충방전 실험과 전기화학적인 실험을 시행하였다. 또한 충전전류밀도와 방전전류밀도의 변화에 따른 비축전 용량의 변화를 조사하였고, 최적 유기전해질의 조건에서 leakage current 특성, 자가방전 특성 그리고 시간전압곡선을 기존의 $1M-Et_4NBF_4/PC$와 비교하였다 활성탄, 소전극으로 비표면적이 $2000m^2/g$인 MSP-20을 사용하고 유기전해질로는 $1M-LiPF_6/PC-DEC(1:1)$를 사용한 EDLC에서 130 F/g 정도의 우수한 비축전 용량을 나타내었고 저항면에서도 가장 낮은 수치를 나타내었다 $1M-LiPF_6/PCDEC(1:1)$를 사용한 EDLC는 15분동안 0.0004A의 낮은 leakage current와 100시간 경과 후 0.8V의 우수한 자가 방전 특성 그리고 IR-drop이 적은 선형의 시간-전압곡선을 보여주었다.

• 한국전기전자재료학회논문지
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• 제28권10호
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• pp.636-641
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• 2015

In this study, the partial discharge degradation properties for 2-core PVC cable($2cores{\times}1.5mm^2$ cross section, length of 10 cm, 20 cm, 30 cm) following immersion with the salt water that the 2%, 4%, 8% of NaCl is dissolved in 100 g of distilled water for 48 and 96 hours has been measured. The results of this study are as follows. When the degradation time in salt water of 2% NaCl is 48 hours, it found that the number of partial discharge increased as about 40 pps, 50 pps, 90 pps with increasing the length of cable to 10 cm, 20 cm, 30 cm. In case the concentration and degradation time is same, the inception and extinction voltage decreased with increasing the length of cable. When the degradation time in salt water is 96 hours and the length of cable is 20 cm, it found that the number of partial discharge decreased as 3,000 pps, 500 pps, 100 pps with increasing the concentration of NaCl to 2%, 4%, 8%.

• 한국정보디스플레이학회:학술대회논문집
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• 한국정보디스플레이학회 2002년도 International Meeting on Information Display
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• pp.609-612
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• 2002

A new reset waveform is proposed for reducing the reset period. A square pulse is applied to the address electrode while reset pulse ramps and before a discharge between the sustain electrodes occurs. The square pulse induces a discharge between the address electrode and the X electrode, and the induced wall charge is opposite to the applied ramp pulse. Thus, the next discharge between the sustain electrodes becomes weaker. The weaker discharge lowers background luminance and improves contrast ratio. Thus, the new reset waveform can reduce ramp up time in the ramp reset waveform The experimental results show that the ramp up time can be reduced by about 90% compared with the conventional ramp reset waveform.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2000년도 영호남학술대회 논문집
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• pp.103-107
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• 2000

The relationships between driving voltage and the wall charge distribution in the address period of surface discharge type AC Plasma Display Panel have been investigated. The quantity of wall charge on each electrode are detected simultaneously from the electrode current after applying only one addressing discharge pulse. The wall charge Qy on the scan electrode Y is nearly the sum of Qx on the address electrode X and Qz on the sustain electrode Z. The Qy increased with the driving voltage regardless of the kind of electrode, whereas the address time Td decreased, Qz and Qy are increased considerably with the blocking voltage Vz, whereas Qx is decreased. The increase rate of Qx, Qy and Qz for increase in Vz was $-13{\times}10^{-2}$ (pc/Vz), and $60{\times}10^{-2}$ (pc/Vz) and $70{\times}10^{-2}$(pc/Vz), respectively.