• Journal of Magnetics
• /
• v.21 no.2
• /
• pp.266-272
• /
• 2016

Transcranial magnetic stimulation devices has been used mainly for diagnostic purposes by measuring the functions of the nervous system rather than for treatment purposes, and has a problem of considerable energy fluctuations per repeated pulse. The majority of strokes are caused by ischemia and result in brain tissue damage, leading to problems of the central nervous system including hemiparesis, dysfunction of language and consciousness, and dysfunction of perception. Control is difficult and the size is large due to the difficulty of digitalizing the energy stored in a capacitor, and there are many heavy devices. In addition, there are many constraints when it is used for a range of purposes such as head and neck diagnosis, treatment and rehabilitation of nerve palsy, muscle strengthening, treatment of urinary incontinence etc. Output stabilization and minimization of the energy variation rate are required as the level of the transcranial magnetic stimulation device is dramatically improved and the demand for therapeutic purposes increases. This study developed a compact, low cost transcranial magnetic stimulation device with minimal energy variation of a high repeated pulse and output stabilization using a real time capacitor charge discharge voltage. Ischemia was induced in male SD rats by closing off the common carotid artery for 5 minutes, after which the blood was re-perfused. In the cerebrum, the number of PARP reactive cells after 24 hours significantly decreased (p < 0.05) in the TMS group compared to the GI group. As a result, TMS showed the greatest effect on necrosis-related PARP immuno-reactive cells 24 hours after ischemia, indicating necrosis inhibition, blocking of neural cell death, and protection of neural cells.

• Polymer(Korea)
• /
• v.33 no.4
• /
• pp.353-357
• /
• 2009

Spray drying is an effective and stable process, which has been widely used to produce pharmaceutical powders. In the traditional spray drying process, it was not quite easy to control the aggregation and the size of particles. Particularly, the preparation of polymeric particles was relatively hard compared to the preparation of food and pharmaceutical ingredients, typically organic materials of small molecular weights. In this study, modification of a conventional spray dryer was tried to use electrical charge and co-axial nozzles to prepare polymeric particles. Poly(ethylene glycol) and poly (D,L-lactide-co-glycolide) were used as the inner polymeric materials, and lactose as the outer shell materials. The results showed that electrohydrodynamic spray-dried particles had a relatively uniform size and particle morphology, and the aggregation of particles could be suppressed compared to the conventional spray-dried particles. The electrohydrodynamic spray-dried powders consisted of spherical particles of $2{\sim}5{\mu}m$ diameters.

• Journal of the Korean Ceramic Society
• /
• v.37 no.11
• /
• pp.1051-1057
• /
• 2000

TiO$_2$와 CeO$_2$박막을 Si 위에 증착한 후 MOCVD법에 의해 PbTiO$_3$박막을 증착하여 MFIS 구조를 형성하였다. 절연층의 후열처리가 절연층 및 MFIS 구조의 전기적 특성에 미치는 영향을 관찰하기 위해 산소분위기와 $600^{\circ}C$~90$0^{\circ}C$의 온도범위에서 후 열처리를 행하였고, C-V 특성 및 누설전류 특성을 분석하였다. CeO$_2$와 TiO$_2$박막의 유전상수는 증착 직후 6.9와 15였으며, 90$0^{\circ}C$ 열처리를 행한 후 약 4.9와 8.8로 감소하였다. 누설전류밀도 역시 증착 직후 각각 7$\times$$10^{-5}$ A/$ extrm{cm}^2$와 2.5$\times$$10^{-5}$ A/$\textrm{cm}^2$에서 90$0^{\circ}C$ 열처리를 거친 후에 약 4$\times$$10^{-8}$ A/$\textrm{cm}^2$와 4$\times$$10^{-9}$ A/$\textrm{cm}^2$로 감소하였다. Ellipsometry 시뮬레이션을 통해 계산된 계면층의 두께는 90$0^{\circ}C$에서 약 115$\AA$(CeO$_2$) 및 140$\AA$(TiO$_2$)까지 증가하였다. 계면층은 MFIS 구조에서 강유전층에 인가되는 전계를 감소시켜 항전계를 증가시켰고, charge injection을 방지하여 Al/PbTiO$_3$/CeO$_2$(90$0^{\circ}C$, $O_2$)/Si 구조의 경우 $\pm$2 V~$\pm$10 V의 측정범위에서 memory window가 계속 증가하는 것을 보여주었다.

• Journal of the Korean Ceramic Society
• /
• v.52 no.5
• /
• pp.366-373
• /
• 2015

Sol-gel binder was prepared by hydrolysis and condensation reaction using boehmite sol and methyltrimethoxysilane as a function of aging-time. The coating slurry was composed of a plate-shape alumina in the sol-gel binder for the EPD process, in which particles dispersed in the slurry were deposited on the electrode under an electric field due to the surface charge. We studied the effects of three parameters: the content of boehmite, the aging time, and the applied voltage, on the physical, thermal, and electrical properties of the hybrid composite films by EPD. The amount of boehmite was 10 ~ 20 wt% and the aging time was 0.5 ~ 72, with a fixed amount of plate-shape alumina of 10 wt%. The condition of applied voltage was 5 ~ 30 V with a distance of 2 cm between the electrode during the EPD process. We confirmed that a structure of hybrid composite films of well-ordered plate alumina was deposited on the substrate when the film was prepared using a sol-gel binder composed of 15 wt% boehmite with 1 hr aging time and EPD at 10 V. The process shows a weight loss of 7% at $500^{\circ}C$ in TGA and a breakdown voltage of 8 kV at $87{\mu}m$.

• Journal of the Korean Ceramic Society
• /
• v.47 no.5
• /
• pp.461-466
• /
• 2010

In this study, $Al_2O_3/TaAlO_4/SiO_2$ (A/TAlO/S) structures with tantalum aluminate charge trap layer were fabricated for Nand flash memory device. We evaluated the memory window and retention characteristic as the thickness of the tunnel oxide was varied among 3 nm, 4 nm, and 5 nm. All tunnel oxide thicknesses were measured by ellipsometer and TEM (Transmission Electron Microscope). The A/TAlO/S multi-layer film consisted of 5 nm tunnel oxide showed the best result of memory window of 1.57 V and retention characteristics. After annealing the 5 nm tunnel oxide A/TAlO/S multi-layer film at $900^{\circ}C$. The memory window decreased to 1.32 V. Moreover, the TEM images confirmed that the thickness of multi-layer structure decreased 14.3% after annealing and the program conditions of A/TAlO/S multi-layer film decreased from 13 V to 11 V for 100 ms. Retention properties of both as-deposited and annealed films stably maintained until to $10^4$ cycles.

• KEPCO Journal on Electric Power and Energy
• /
• v.1 no.1
• /
• pp.33-38
• /
• 2015

Energy storage systems (ESSs) have been utilized widely in the world to optimize the power operation system and to improve the power quality. As lithium secondary batteries are the main power supplier for ESSs, it is very important to predict its cycle and power degradation behavior. In particular, the power, one of the hardest electrochemical properties to measure, needs lots of resources such as time and facilities. Due to these difficulties, computer modelling of lithium secondary batteries is applied to predict the DC-IR and power value during charging and discharging as a function of state of charge (SOC) by using pulse-based measurement methods. Moreover, based on the hybrid pulse power characteristics (HPPC) and J-Pulse (JEVS D 713, Japan Electric Vehicle Association Standards) methods, their electrochemical properties are also compared and discussed.

• Proceedings of the KIEE Conference
• /
• 2007.07a
• /
• pp.38-39
• /
• 2007

Recently, utility network is becoming more and more complicated and huge due to IT(Information Technology) and OA(Office Automation) devices. In addition to, demands of power conversion devices which have non-linear switching devices are getting more and more increased. Voltage sag from sudden increasing loads is also one of the major problems inside of the utility network. In order to compensate the voltage sag problem, power compensation devices systems could be a good solution method. In case of voltage sag, it needs an energy source to overcome the energy caused by voltage sag. Superconducting Magnet Energy Storage (SMES) is a very good promising source due to the high response time of charge and discharge. This paper presents a real-time simulation algorithm for the SMES by using Real Time Digital Simulator (RTDS). With this algorithm users can easily do the simulation of utility power network applied by SMES system with the SMES coil modeled in RTDS.

• Proceedings of the Korean Institute of Surface Engineering Conference
• /
• 2015.05a
• /
• pp.32-32
• /
• 2015

Electrophoretic paint (E-paint) was investigated on four different magnesium substrates: as-extruded AZ61 (AZ61), heat-treated AZ61 (AZ61-H), as-extruded TZ61 (TZ61) and heat-treated TZ61 (TZ61-H), to elucidate the effect of heat treatment and alloying elements on the deposition and corrosion resistance of E-paint. It was found that, a rapid increase of voltage, indicating that the deposition of E-paint had started, was observed after an induction time of 0.39 min for AZ61-H, 0.43 min for AZ61, 0.51 min for TZ61-H and 0.58 min for TZ61. The amount of E-paint deposited on the four samples was approximately similar, but the electrical charge used for the deposition process on the heat-treated samples was smaller than that on the as-extruded samples. The current efficiencies of E-paint on AZ samples (AZ61 and AZ61-H) were higher than those of TZ samples (TZ61 and TZ61-H), and on the heat-treated samples were higher than on as-extruded samples. All E-paintings on the four magnesium substrates had an excellent adhesion without any paint detached by tape peel-test. However, many large blisters were formed on the surface of AZ samples, and none, or very small blisters were observed on TZ samples after immersion test in DI-water for 500 h at $40^{\circ}C$. Under salt spray test (SST) conditions, E-paint on AZ samples showed blistering adjacent to scribes, while blistering of E-paint occurred on intact areas of TZ samples. The E-paint on heat-treated samples showed much better corrosion resistance than that on as-extruded samples. The ranking of greater to lesser corrosion resistance of the E-paint on these four different magnesium substrates is indicated by the order: AZ61-H > AZ61 > TZ61-H > TZ61.

• Proceedings of the KIEE Conference
• /
• 2007.07a
• /
• pp.1988-1989
• /
• 2007

Polyethylene is widely used as the insulator for power cable. To investigate the conduction mechanism for power cable insulation under ac high field, it is very important to acquire the dissipation current under actual running field. Recently, we have developed the unique system, which make possible to observe the nonlinear dissipation current waveform. In this system, to observe the nonlinear properties with high accuracy, capacitive current component is canceled by using inverse capacitive current signal instead of using the bridge circuit for canceling it. We have already reported that the dissipation currents of $40\;{\mu}m$ thick LDPE film at 10 kV/mm and over 140 Hz, it starts to show nonlinearity and odd number's harmonics were getting large. To investigate the conduction mechanis ms in this region, especially space charge effect, various kinds of estimation, such as time variations of instantaneous resistivity for one cycle, FFT spectra of dissipation current waveforms and so on, has been examined. As the results of these estimations, it was found that the dissipation current will depend on not only the instantaneous value of electric field but also the time differential of applied electric field due to taking a balance between applied field and internal field. Furthermore, two large peaks of dissipation current for each half cycle were observed under certain condition. In this paper, to clarify the reason why it shows two peaks for each half cycle, the film thickness dependences of dissipation current waveforms were observed by using the three different thickness LDPE films.

• Transactions of the Korean Society of Mechanical Engineers B
• /
• v.20 no.6
• /
• pp.2023-2035
• /
• 1996

In the present study, the characteristics of the electrical deformation of a bubble and a drop under a uniform electric field have been investigated to understand EHD heat transfer enhancement by an electric field. The deformation of the bubble and the drop have been studied theoretically using an electric normal stress acting on their interfaces and assured by the numerical analysis and the experiment. From the variation of bubble volume and free energy, it is found that a bubble is compressed in an electric field and free energy had larger value with increasing W and the permittivity of a dielectric fluid. The electric normal stress induced on the interface of the bubble and the drop is different. Because of the surface charge induced at the drop interface, the electric normal stress acting on the drop is much larger than that of the bubble. The drop is, therefore, deformed much more than the bubble. In addition, the experimental and numerical results show that the aspect ratio and the contact angle of the bubble increase with increasing W.