• KEPCO Journal on Electric Power and Energy
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• v.1 no.1
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• pp.1-8
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• 2015

When the line and switchgear of the substation system are disconnected, ferro-resonance can occur. This happens even if the capacitive reactance and inductive reactance are not equal, which are not common resonance conditions. Resonance conditions vary depending on the busbar configuration environment. Although the damping resistance method applying the existing saturable reactor to cope with ferro-resonance has been successfully applied on site, there can be loss of normal function during long-term operation. The reason is because the rise in the operating frequency of saturable reactors means the saturation number is increased. Therefore, it can no longer function as saturable reactor since the resistor having inadequate capacity is burned out. To address this problem, in this paper, an EMTP-based simulation test was performed by designing and applying a dual reactor method, which adds an extended divergence reactor to the 1st side of the VT. The test result confirms that when the divergence reactor is inserted, the voltage and current values obtained at the 1st side and 2nd side of the VT as well as current values of divergence reactor part were stabilized from the transient phenomena and return to normal values. When compared with existing measures, although this method is similar in adding having a reactor added to a system regarding ferro-resonance, it has the advantage of being able to prevent ferro-resonance in advance since the reactor is added before the system is saturated. In addition, because it does not use damping resistance, it can extend the equipment life and stabilize its operation. Therefore, there are a lot of differences in terms of its operating characteristics and achivement of goal between the conventional method and new divergence reactor method.

• Journal of Magnetics
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• v.5 no.1
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• pp.9-12
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• 2000

Electron spin resonance and magnetization measurements were carried out on $La_0.7Ca_0.3MnO_3$ in the ferromagnetic as well as paramagnetic phases. Evidence of an inhomogeneous magnetic structure, consisting of ferro-magnetic microregions embedded in an antiferromagnetic matrix near $T_c$, as well as similar local magnetic structures above and below $T_c$, were found.

• Proceedings of the KIEE Conference
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• 2007.11b
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• pp.18-20
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• 2007

A coupling capacitor voltage transformer (CCVT) is used in an extra high voltage power system to obtain the standard low voltage signal for protection and measurement. To suppress the effects of ferro-resonance more effectively, a three winding CCVT is used. This paper proposes an algorithm for compensating the secondary voltage of the three winding CCVT. With the secondary voltage of the three winding CCVT, the secondary and tertiary currents are obtained; the primary winding current is obtained by considering non-linear characteristics of the core; the voltage across the capacitor and the inductor are calculated and then added to the measured voltage to compensate the secondary voltage. Test results indicate that the algorithm can reduce the errors of the three winding CCVT significantly.

• Proceedings of the Korean Institute of Navigation and Port Research Conference
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• 2000.11a
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• pp.89-92
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• 2000

Liquid Phase Epitaxy 법을 이용하여 La이 첨가된 YIG(Yitrium Ion Garnet)막을 성장시켰다. X선 회절 분석을 이용하여 La의 첨가량을 변화시키며 제조된 막의 격자상수를 조사한 결과, La의 첨가량이 증가함에 따라 성장된 막의 격자상수도 증가하였으며 Y/La이 20인 경우, 막의 격자상수가 기판으로 사용한 GGG의 격자상수와 일치하였다. VSM(Vibration Sample Magnetometer)를 이용하여 구한 막의 포화자화 값은 La의 첨가량과 관계없이 순수한 YIG의 경우와 같은 값인 1750정도로 거의 일정하였다. FMR(FerroMagnetic Resonance) 측정장치를 이용한 막의 강자성 공명선폭을 측정결과 막의 공명선폭은 La의 첨가량과 관계없이 모든 경우에 순수한 YIG보다 감소하였다. 실험범위내의 La의 첨가에 대해서 기판과의 격자불일치가 순수한 YIG의 경우보다 감소하기 때문이다. La의 첨가량이 많은 조건에서 성장시킨 막은 공명선폭이 크고 두께의 증가에 따라서 선폭이 증가하였으며, YLa가 20과 30일 때 성장시킨 막에서는 공명선폭의 절대값도 작고 두께에 따른 공명선폭의 변화도 관찰되지 않았다.

• Proceedings of the KIEE Conference
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• 1999.07c
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• pp.1152-1154
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• 1999

Recently. due to the drastic development of communication method between substations for pilot protective relaying system. The power line carrier(PLC) application is getting obsolete. Consequently, the coupling capacitor voltage transformer (CCVT) loses its necessity for the carrier coupling function, and so wound voltage transformer(VT) can be used to substitute CCVT for voltage signal. However, VT has been reported to give rise to ferro-resonance phenomena, so sufficient consideration on applying the VT to line side is required. This study introduces probable technical problems in using the VT on T/L side, and carries out feasibility study on the basis of modeling results by EMTP(Electro-magnetic transient program)

• Proceedings of the KIEE Conference
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• 2003.07a
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• pp.485-487
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• 2003

본 논문은 기설 WSI제 CVT에 대해 전자 과도해석 프로그램((EMTP : Electromagnetic Transient Program)을 통한 모의실험으로 철공진현상 제동저항 크기($0.5{\Omega}$)를 선정하고, 기설 154kV 및 345kV CVT의 철공진방지회로를 제동저항 단독취부 형태에서 과포화리액터와 제동저항을 직렬회로로 구성하여 취부하는 방식으로 개선한 후 실증시험 및 현장적용 시험을 통해 CVT 쳔공진현상 제동여부 확인 및 외함온도 변화추이 비교하여 개선효과를 제시함으로써 WSI제 CVT 고장예방에 기어코자 한다.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2000.11a
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• pp.89-92
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• 2000

Liquid Phase Epitaxy 법을 이용하여 La이 첨가된 YIG(Yitrium Ion Garnet)막을 성장시켰다. X선 회절 분석을 이용하여 La의 첨가량을 변화시키며 제조된 막의 격자상수를 조사한 결과, La의 첨가량이 증가함에 따라 성장된 막의 격자상수도 증가하였으며 Y/La이 20인 경우, 막의 격자상수가 기판으로 사용한 GGG의 격자상수와 일치하였다. VSM(Vibration Sample Magnetometer)를 이용하여 구한 막의 포화자화 값은 La의 첨가량과 관계없이 순수한 YIG의 경우와 같은 값인 1750정도로 거의 일정하였다. FMR(Ferro Magnetic Resonance) 측정장치를 이용한 막의 강자성 공명선폭을 측정결과 막의 공명선폭은 La의 첨가량과 관계없이 모든 경우에 순수한 YIG보다 감소하였다. 실험범위내의 La의 첨가에 대해서 기판과의 격자불일치가 순수한 YIG의 경우보다 감소하기 때문이다. La의 첨가량이 많은 조건에서 성장시킨 막은 공명선폭이 크고 두께의 증가에 따라서 선폭이 증가하였으며, Y/La가 20과 30일 때 성장시킨 막에서는 공명선폭의 절대값도 작고 두께에 따른 공명선폭의 변화도 관찰되지 않았다.

• Proceedings of the KIEE Conference
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• 2008.07a
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• pp.1246-1247
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• 2008

With recent advanced in portable electric devices, wireless sensor, MEMS and bio-Mechanics device, the new typed power supply, not conventional battery but self-powered energy source is needed. Particularly, the system that harvests from their environments are interests for use in self powered devices. For very low powered devices, environmental energy may be enough to use power source. Therefore, in other to made piezoelectric energy harvesting device, PMN-PZT thick film was formed by the screen printing method on the Ag/Pd coated alumina substrate. The layer was 8 layers and slurry where a-terpineol, ethycellulose, ferro B-75001 as Vehicle, PMN-PZT powder used are fabricated by ball mill. The output power quality was be also investigated by changing the load resistance, weight and frequency. The made piezoelectric energy harvesting device was resulted from the conditions of 33$k{\Omega}$, 0.25g, 197Hz respectively. The thick film was prepared at the condition of 2.75Vrms, and its power was 230${\mu} W$ and its thickness was 56${mu}m$. The piezoelectric energy harvesting device output voltage was increased, when the load weight, load resistance was increasing and resonance frequency was diminishing. The other side, resonance frequency was diminished, when the weight was increasing. And output power was continuously it changed by load resistance, output voltage, weight and resonance frequency.

• Journal of the Korean Magnetics Society
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• v.11 no.6
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• pp.239-244
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• 2001

Recently, RF inductor having researched by many workers, we fabricated and investigated properties of RF inductors. In order to improve the Q-factor (Quality), we try to apply the patterned Fe$_{78.81}$Ta$_{8.47}$N$_{12.71}$ soft magnetic thin film of 5000 which shows magnetic anisotropy of 30 Oe. Thus, patterned magnetic film was artificially increased magnetic anisotropy lead to increasing of ferro-magnetic resonance frequency up to GHz band. Coil as part of inductor was fabricated by lift off process. The dimension of RF inductor was designed 47un, rectangular shape, and measured properties. In the case of Ti/Ag air core type inductor shows Q of 9, inductance of 8.4 nH at 2 GHz. Magnetic film employed inductor shows inductance of 9 nH and FMR resonance frequency was 700 MHz.

• Proceedings of the KIEE Conference
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• 2006.07a
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• pp.266-267
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• 2006

A coupling capacitor voltage transformer (CCVT) is used in extra high voltage and ultra high voltage transmission systems to obtain the standard low voltage signal for protection and measurement. To obtain the high accuracy at the power system frequency, a tuning reactor is connected between a capacitor and a voltage transformer (VT). Thus, no distortion of the secondary voltage is generated when no fault occurs. However, when a fault occurs, the secondary voltage of the CCVT has some errors due to the transient components resulting from the fault. This paper proposes an algorithm for compensating the secondary voltage of the CCVT in the time domain. With the values of the secondary voltage of the CCVT, the secondary and the primary currents are obtained; then the voltage across the capacitor and the tuning reactoris calculated and then added to the measured secondary voltage. The proposed algorithm includes the effect of the non-linear characteristic of the VT and the influence of the ferro-resonance suppression circuit. Test results indicate that the algorithm can successfully compensate the distorted secondary voltage of the CCVT irrespective of the fault distance, the fault inception angle and the fault impedance.