• 유공압시스템학회:학술대회논문집
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• 2010.06a
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• pp.70-73
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• 2010

In order to provide theoretical analysis for the active roll stabilizer (ARS), the simulation model based on AMESim is developed in the paper. The simplified vehicle rolling motion model is derived firstly, and then the entire ARS control system model is constructed. Furthermore, the simulation is implemented to confirm the roll control effect. The simulation results show that the derived model can be used as theoretical analysis for developing components of ARS control system.

• Proceedings of the KIPE Conference
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• 2003.07a
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• pp.446-450
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• 2003

This paper makes more stronger than original model about sending station fault and saves total construction cost to replace established six-pulse bridge by each six thyristor for DC-transmission. Also, varying of controller for sending station has a robust characteristics for harmonics and unbalanced faults. This paper is verified by simulation using EMTDC program. Comparing with the results of original model, this paper is proved superiority.

• Proceedings of the KIEE Conference
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• 1997.07c
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• pp.1028-1031
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• 1997

This Paper Presents a new digital balance relaying technique in two Parallel transmission lines. To obtain relaying signals, selected model is simulated using EMTDC. Test results of the proposed method show efficacy.

• Proceedings of the KIEE Conference
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• 2000.07a
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• pp.292-294
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• 2000

This paper is presented the method peak load forecast based on multiple regression Model. Forecasting model was composed with the temperature-humidity and the discomfort index. Also the week periodicity was excluded from weekday change coefficient of two types. Forecasting result was good with about 3[%]. And, utility of presented forecast model using statistical tests has been proved. Therefore, This results establish appropriateness and fitness of forecast models using peak power demand forecasting.

• Transactions of Materials Processing
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• v.18 no.5
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• pp.385-391
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• 2009

An adhesively bonded power steering cylinder with a steel tube and an aluminum bracket was developed to reduce the weight of steering systems. To achieve the joint strength between the steel tube and of the aluminum bracket, the shape aluminum bracket re-designed by using the FE-analysis. Fracture behavior of the adhesive layer was considered by a cohesive zone model(CZM), which is based on the two-parameter fracture phenomenon with critical stress and fracture toughness. From the result of FE-analysis with CZM, re-designed power steering cylinder satisfied the desired joint strength for axial and torsion modes. And its joint strength was verified by the fracture test in each mode.

• Proceedings of the KIEE Conference
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• 1999.07e
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• pp.2013-2015
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• 1999

The pulsed plasma wire-plate reactor was modelled on the basis of experiment and EMTP simulation. The electrical phenomena in reactor is consistent with the model we suggested. Using this model, the influence of the reactor capacitance on the impedance matching between pulse generator and reactor can be analyzed. From this, we found that the energy of 95 % was delivered from pulse generator to reactor at the ratio of $C_p$/$C_r$ $\cong$ 30 %, where $C_p$ is pulse generator capacitance, $C_r$ is reactor capacitance.

• Journal of the Korean Magnetics Society
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• v.2 no.3
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• pp.228-232
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• 1992

Magnetic properties of grain aligned high $T_c\;Y_1Ba_2Cu_3O_{7-y}$ superconductor are inverstigated. Grain-aligned superconductors have magnetic anisotropy in the Cu-O layer like single crystals. The lower critical field $H_{c1},$ measured at the temperature range of 2 K up to 77 K, is found to be decreasing linearly as temperature goes up. Moreover, it decreaes more rapidly when the Cu-O layer is perpendicular to the external magnetic field. The temperature dependence of the magnetic susceptibility shows that the value of magnetic susceptibility, $4{\pi}\;X,$ is close to -1 at low temperature. The intra grain critical current density $J_c,$ obtained from the Bean's critical state model, is found to be comparable to that of single crystal superconductors.

• Korean Journal of Human Ecology
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• v.23 no.1
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• pp.137-148
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• 2014

The aim of this study was to determine whether the addition of soy isoflavones to dairy ice cream modifies diabetic biomarkers in the type 2 diabetic model mice. Forty male C57BL/6J-ob/ob mice were randomly divided into 4 groups and fed control diet (basal, 7% fat), MS diet (milk ice cream with sugar, 20% fat), MS-SI diet (MS ice cream with 0.01% soy isoflavones, 20% fat), or MF-SI diet (milk ice cream with 0.01% soy isoflavones, 5% fructooligosaccharide, 20% fat) for 12 weeks. Blood response area by glucose tolerance test, plasma levels of glucose, insulin, C-peptide, leptin, and blood $HbA_{1c}$ were not significantly different among all the groups. Concentrations of interleukin-6 and tumor necrosis factor-${\alpha}$ secreted from splenocytes induced by Concanavalin A were not significantly different among all the groups. In conclusion, soy isoflavones supplemented to ice cream did not alter diabetic biomarkers in diabetic type 2 model mice.

• Proceedings of the KIEE Conference
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• 2002.07d
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• pp.2331-2333
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• 2002

In this paper, we propose a new model with the common Control Rod Control System which can be applied to both Korea Standard Nuclear Power Plant model and Westinghouse model. The common model classified by one control rod assembly can solve the common-mode failure. We digitalize the new model and make existing analog models simplified.

• Clean Technology
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• v.20 no.1
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• pp.22-27
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• 2014

Under low pressures of $CF_4$ and $C_2F_6$ up to 20.7 kPa, the equilibrium adsorbed quantity on activated carbon was experimentally examined using the volumetric method at various temperatures between 293.15 K and 333.15 K. To give the best fit to the experimental data curve, the two step model (i.e., Langmuir model for the first layer adsorption and then Freundlich physisorption) is suggested. The method of initial slope yielded the enthalpy of adsorption for the first step while we could apply the Clausius-Clapeyron equation to find the heat of adsorption of the second step. They are 25.9 kJ/mol and 11.8 kJ/mol, respectively, with $CF_4$, and 38.7 and 38.2 kJ/mol with $C_2F_6$.