• Transactions of the Korean Society of Mechanical Engineers A
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• v.38 no.9
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• pp.1013-1018
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• 2014

Magnetic Abrasive Polishing (MAP) process is a nontraditional method for polishing the surface of workpiece by using the flexibility of tool. At present, a mixture of polishing abrasives and ferrous particles is used as the tool in the MAP process. Previously, an experiment was conducted with different sizes of polishing abrasives with an aim to improve the polishing accuracy. However, the sizes of ferrous particles are also expected to have a dominant effect on the process, warranting a study on the effect of the size of ferrous iron particles. In this study, an experiment was conducted using three different sizes of ferrous particles. Iron powder of average diameters 8, 78 and $250{\mu}m$ was used as ferrous particles. The effect of each ferrous particle size was evaluated by comparing the improvements in surface roughness. The particle size of a ferrous iron was found to play a significant role in MAP and particles of $78{\mu}m$ facilitated the best improvement in surface roughness.

• Proceedings of the Korean Society of Propulsion Engineers Conference
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• 2009.11a
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• pp.202-206
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• 2009

We studied the spray characteristics of the high-speed rotating fuel injection system. The diameter of in-line injection orifices are varied from 1mm to 5mm and the number of in-line injection orifices are varied from 3 to 12. Droplet size, velocity and spray distribution were measured by the PDPA(Phase Doppler Particle Analyzer) system and spray was visualized. From the test results, the liquid column generated from the injection orifice is mainly controlled by the rotational speeds. Also diameter of injection orifices and number of injection orifices have influence on the diameters of droplet. Consequently, we find out that the basic mechanism of controlling the droplet size is the liquid film thickness in the injection orifice.

• Journal of Korean Ophthalmic Optics Society
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• v.1 no.2
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• pp.7-11
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• 1996

The size of pupil with pupillary light reflex is determined by the amount of a luminance. and it is dependent with the distribution function of the retinal illuminance which is the amount of transmittance for the external light due to the size of pupil, and the detector of cone and rod due to the amount of the luminance. The change of the pupil size with the luminance can be expressed with the mathematical model $$y(x)={\alpha}+{\beta}\frac{1}{1+{e}{x}{p}(x-x_0)/{\theta}}$$ where ${\alpha}$ is the size of the pupil diameter in a maximum value of the luminance, ${\beta}$ is the deviation of the pupil's diameter between maximum and minimum, ${\theta}$ is the parameter showed the degree of a sensitivity. Comparing with the experimental value of P.Moon et al, We known that the equation of the model is very compatible.

• Proceedings of the KIEE Conference
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• 2002.07c
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• pp.1521-1523
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• 2002

본 논문에서는 1.58 ${\times}$ 0.82 ${\times}$ 0.94 $mm^3$크기의 H 형태의 솔레노이드형 RF 칩 인덕터를 코일의 직경과 권선수를 변화시키면서 제작하였고, 그들의 고주파 성능을 비교 분석하였다. 저손실 $Al_2O_3$재료를 코아로 $30{\mu}m{\sim}40{\mu}m$의 여러 직경을 가진 Cu를 코일로 사용하였다. 인덕터의 인덕턴스(L), 품질계수(Q), 저항(R), 임피던스(Z) 그리고 커패시턴스(C) 등의 주파수 특성은 HP4291B로 측정하였다. 실험결과 동일권선수에 대해 코일직경이 자을수록 L, Q, R, 그리고 Z등이 증가하였고, 그 증가폭은 권선수가 클수록 커지는 경향이 있음을 알 수 있었다. 그러나 코일직경이 작을수록 기생 커패시턴스 효과가 빨리 나타나 자기 공진주파수 효과가 감소하는 경향을 보이고 있음을 확인하였다. 코일직경이 $3{\mu}m$이고 권선수가 6인 경우에 대표적인 값들은 다음과 같다. L=31.4nH(at 250MHz), Q=49.6(at 700MHz), R=0.362${\Omega}$(at 1MHz)

• Tunnel and Underground Space
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• v.15 no.2 s.55
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• pp.137-144
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• 2005

An estimation technique of the joint diameter distribution using the least square method is suggested. When utilizing the technique by Song and Lee, the diameter distribution would be obtained only from the trace length distribution defined in an infinite window after the trace length distribution is estimated from the contained trace length distribution. With the new technique, however, the diameter distribution can be directly obtained from the sample histogram of the contained trace lengths. Compared with the previous technique, it shows a more accurate result for small sizes of joint samples and provides the joint geometry parameter of volumetric frequency. Verification of this new technique was completed by using Monte Carlo simulations.

• Journal of the Korean Society for Aeronautical & Space Sciences
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• v.37 no.5
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• pp.476-482
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• 2009

The effect of pintle shape on the thrust level of pintle-nozzle Solid Rocket Motor(PNSRM) was studied numerically using the Spalart-Allmaras turbulent model of Fluent. Mass flow rate of PNSRM was always less than theoretical value and the extent of decrease in mass flow rate grew in the large pintle because of increase in the relative boundary layer thickness between pintle body and nozzle wall. The bigger pintle size was, the more thrust of pintle tip pressure was obtained. Meanwhile the more thrust of nozzle and chamber pressure decreased. Hence, total thrust of big pintle was less than a small pintle under same throat area condition. Specific impulse was relatively flat for all pintle shape.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.22 no.1
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• pp.5-10
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• 2012

In general, the fabrications of the LEDs with mesa structure are performed grown by MOCVD method. In order to etch and separate each chips, the LEDs are passed the RIE and scribing processes. The RIE process using plasma dry etching occur some problems such as defects, dislocations and the formation of dangling bond in surface result in decline of device characteristic. The SAG method has attracted considerable interest for the growth of high quality GaN epi layer on the sapphire substrate. In this paper, the SAG method was introduced for simplification and fabrication of the high quality epi layer. And we report that the size of selective area do not affect the characteristics of original LED. The diameter of SAG circle patterns were choose as 2500, 1000, 350, and 200 ${\mu}m$. The SAG-LEDs were measured to obtain the device characteristics using by SEM, EL and I-V. The main emission peaks of 2500, 1000, 350, and 200 ${\mu}m$ were 485, 480, 450, and 445 nm respectively. The chips of 350, 200 ${\mu}m$ diameter were observed non-uniform surface and resistance was higher than original LED, however, the chips of 2500, 1000 ${\mu}m$ diameter had uniform surface and current-voltage characteristics were better than small sizes. Therefore, we suggest that the suitable diameter which do not affect the characteristic of original LED is more than 1000 ${\mu}m$.

• Clinical and Experimental Pediatrics
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• v.50 no.10
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• pp.970-975
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• 2007

Purpose : Accurate measurement of defect size is important in transcatheter closure of atrial septal defect (ASD). We performed this study to analyze the difference between the measured ASD size and balloon occlusive diameter (BOD) by transthoracic (TTE) or transesophageal echocardiography (TEE). Methods : We investigated 78 patients who underwent transcatheter closure of ASD. The defect size and the distance between the surrounding structures were measured by TTE and TEE. The BOD was measured by TEE during cardiac catheterization. Clinical characteristics and echocardiographic data were compared and analyzed. Results : The difference between BOD and diameter by TTE was $4.8{\pm}3.6mm$ on short axis view, $5.4{\pm}3.2mm$ on long axis view. The difference between BOD and diameter by TEE was $3.6{\pm}2.2mm$ on short axis view, $4.2{\pm}3.1mm$ on long axis view. The difference between BOD and the diameter of defects on TTE, TEE had statistically significant positive correlations with the age of the patients, distance between the, defect and posterior atrial septal wall, the distance between the defect and the mitral valve leaflet, and the diameter of defects and the length of the atrial septum on TTE (P<0.05). Conclusion : BOD of ASD can be estimated by the diameter on TTE and TEE. BOD is expected to measure larger, depending on the size of defects, the distance from surrounding structures and the location of defects on echocardiography. Our data offers important information on details of transcatheter ASD closure which can be helpful in predicting suitability and judging the procedural appropriateness during the procedure.

• Electrical & Electronic Materials
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• v.3 no.3
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• pp.187-194
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• 1990

광자기 메모리용 재료인 비정질 TbFe 박막을 대상으로 열자기 기록시 박막에 분포하는 온도와 이때 만들어지는 bit의 크기간에 상호관련성을 조사하였다. 레이저 조사에 의해 가열된 박막의 온도분포는 유한요소법을 이용한 열전달 해석에 의해 계산하였다. 레이저 가열종료 직전 박막 면에 분포하는 온도 contour로 부터 bit 크기를 예측하였다. 여기서 bit 크기는 온도 상승에 따라 보자력이 약화되어 외부자계와 박막반자장의 합력이 역자구를 만들어 준다고 가정하여 이 경계가 되는 온도(Tcrit)로 이루어지는 등온선의 크기로부터 정하였다. 열자기 기록 실험으로부터 기록 bit의 크기(Dmeas.)을 측정하여 레이저조사조건별로 예측한 bit크기(Dpred.)와 비교하였다. 특히, 레이저 pulse시간 변화에 따른 여러온도의 등온선 contour 직경변화를 조사하여 실측한 bit크기와 비교 검토함으로써 bit형성에 미치는 온도분포의 영향을 조사하였다. 이 결과 레이저 pulse시간이 길어지거나 레이저 power가 상대적으로 작을때 실측한 bit크기가 예측된 bit크기보다 커지는 것으로 나타났으며 이는 Tcrit 온도구배가 완만해질수록 bit경계가 되는 온도가 낮아지는 것으로 해석된다.

• Proceedings of the Korea Air Pollution Research Association Conference
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• 2002.11a
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• pp.434-435
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• 2002

에어로졸 입자의 크기 분포를 측정하는: 방법은 여러 가지가 있다. 이중 광학 입자계수기(Optical Particle Counter)는 직경 0.3-25$\mu\textrm{m}$의 입자의 산란광의 강도를 측정하여 입자의 크기별 개수를 측정하는 기기로 청정지역의 대기 중 부유하는 입자의 측정에 널리 사용되고 있다 (전영신 등, 1999). 본 연구에서는 기상청 기상연구소에서 측정한 광i부 입자계수기(HYAC/ROYCO 5230)의 측정자료를 이용하여 2001년도 1년간 서울의 대기 에어로졸의 특성과 경향을 분석하였다. 측정결과는 대기환경월보(환경부, 2001) (중략)