• 한국광학회지
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• 제35권1호
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• pp.18-23
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• 2024

미술관 등 전시 공간에서의 조명은 바닥보다는 주로 전시물이 붙어 있는 벽면에 비춰져야 한다. 일반적으로 사용되는 LED 조명은 LED에 확산판이 결합된 형태로서 각도별 배광 분포가 일정한 램버시안 광원에 가까우며, 수직 입사가 이뤄지는 바닥면에 조명이 집중된다. 따라서 이러한 일반적 형태의 조명 방법은 벽면을 조명하기에는 적합하지 않으며, 벽면에 조명을 집중시키기 위해서는 각도별 배광 분포 중 각도가 큰 영역에서의 광량이 커지도록 해야 한다. 본 연구에서는 광원에서의 발산각을 180도로 확산시키기 위해 초광각 변환기를 사용하는 조명 광학계에 대해 논의하고자 한다.

• Current Optics and Photonics
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• 제8권1호
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• pp.30-37
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• 2024

Implemented at the Geochang Observatory in South Korea, our slope detection and ranging (SLO-DAR) system features a 508 mm Cassegrain telescope (f /7.8), incorporating two Shack-Hartmann wave-front sensors (WFS) for precise measurements of atmospheric phase distortions, particularly from nearby binary or double stars, utilizing an 8 × 8 grid of sampling points. With an ability to reconstruct eight-layer vertical atmospheric profiles, the system quantifies the refractive index structure function (C_n²) through the crossed-beam method. Adaptable in vertical profiling altitude, ranging from a few hundred meters to several kilometers, contingent on the separation angle of binary stars, the system operates in both wide (2.5 to 12.5 arcminute separation angle) and narrow modes (11 to 15 arcsecond separation angle), covering altitudes from 122.3 to 611.5 meters and 6.1 to 8.3 kilometers, respectively. Initial measurements at the Geochang Observatory indicated C_n² values up to 181.7 meters with a Fried parameter (r₀) of 8.4 centimeters in wide mode and up to 7.8 kilometers with an r₀ of 8.0 centimeters in narrow mode, suggesting similar seeing conditions to the Bohyun Observatory and aligning with a comparable 2014-2015 seeing profiling campaign in South Korea.

• 인터넷정보학회지
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• 제11권3호
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• pp.47-51
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• 2010

• 한국고분자학회지:고분자과학과기술
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• 제8권2호
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• pp.201-210
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• 1997

• Journal of Oral Medicine and Pain
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• 제23권2호
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• pp.143-155
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• 1998

This study was performed to investigate the factor that might affect mandibualr body rotation. For the study, 115 patients with temporomandibular disorders and 35 dental students without angy signs and symptoms of temporomandibular disorders were randomly selected as the patient group and the contreol group, respectively. Preferred chewing side, Angle' classification, lateral guidance pattern, and affected side were clinically recorded, and the amount of Mandibular body rotational torque movement was measured in wide opening and closure, in right and left excursion with vertical and lateral distance in frontal plane, right and left rotational angel in horizontal and in frontal plane. Masticatory muscle activity of anteriorocclusal contact pattern on maximal hard biting were also observed synchronously with BioEMG and T-Scan , respectively. The observed items were muscle activity of anterior temporalis and superficial masseter, and tooth contact status related to contact number, force, duration, and occlusal unbalance between right and left arch. The data collected were analyzed by SAS statistical program. The results of this study were as follows : 1. Mean value of vertical distance in frontal plane in wide opening and closure was more in control subjects than in patients, but there was no difference for rotational angle. In right excursion, rotational angles were greater in patient group than in control group. 2. Comparison among the subjects by preferred chewing side did not reveal any significant difference, but comparison among patients by affected side showed more rotational amount in bilaterally affected patients than in unilaterally affected patients. 3. Comparison among the subjects by Angle's classification or lateral guidance pattern revealed no difference. There was also no difference between preferred chewing side and contralateral side, and between affected side and contralateral side. 4. Positive correlation in madibular rotational torque movements were observed among vertical distance, total horizontal rotation angle, electromyographic activity of anterior temporalis, tooth contact number, and tooth contact force but total frontal rotation angle almost did not show any correlation with other variables except vertical distance.

• The Journal of the Acoustical Society of Korea
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• 제25권3E호
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• pp.115-122
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• 2006

The bistatic scattering of an incident wave by a hemi-spherically capped cylinder is of particular interest because it has rarely been studied until the present day. The configuration of a hemi-spherically capped cylinder is similar to naval underwater weapons (submarines, mines, torpedos, etc.), but which is not exactly the same. This paper describes a novel laboratory experiment aimed at direct measurement of bistatic scattering by a hemi-spherically capped cylinder. Bistatic scattering by a hemi-spherically capped cylinder was measured in an acoustic water tank (5m long, 5m wide, 5m deep) using a high frequency projector (120kHz) and hydrophone. Measurements of monostatic scattering were also made under the same conditions. The bistatic scattering pattern by a hemi-spherically capped cylinder was measured against the incident angles $(0^{\circ},\;15^{\circ},\;20^{\circ},\;30^{\circ},\;45^{\circ},\;60^{\circ},\;90^{\circ})$ in order to verify various scattering pattern characteristics by the change of incident angle. The results indicate that the bistatic scattering TS at a wide scattering angle is much stronger than the mono static scattering TS. In bistatic scattering, the forward scattering TS is significantly stronger than the backward scattering TS, and the forward scattering pattern is also broader. In case of seven incident angles, the maximum value of forward scattering TS is about 14dB stronger than that of backward scattering TS. It is also found that forward scattering varies with the incident angle of sound to a much less extent than backscattering, and it is not seriously affected by the incident angle. These features could be the advantages of using forward scattering for detecting underwater targets at long range and increasing detection area and probability.

• 한국농공학회지
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• 제15권2호
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• pp.2980-3001
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• 1973

Nozzle is a part of sprayer and is consists of several elements; swirl plate, vortexchamber, cap and body. The travelling distance of sprayed particles is important in the wide reach nozzle. The factors to influence the travelling distance of the sprayed particles may be the helical angle of swirl plate, the distance of vortex hamber, the slope and the size of cap hole. The study was conducted to examine the effects of these factors on the travelling distance. The results of this study are summarized as follows; 1) There was higher positive correlation(+0.96) between the maximum travelling distance for which amount of sprayed particles was 5cc/cm min. and centro-position of the travelling distance. 2) There was a higher positive correlation(+0.85) between total discharge of sprayed particles and the centro-position of the travelling distance. 3) Main effects and interaction effects of helical angle, pressure, vortex chamber distance and cap slope were significantly affected the travelling distance of sprayed particles. 4) Main effects of helical angle, pressure and cap slope were especially highly significant to influence the travelling disance. 5) Helical angle, pressure, vortex chamber distance and cap slope influenced spraying forward velocity of dise hole, among which cap slope and pressure of nozzle was the most important factors. 6) Effect of change of helical angle on the travelling distance of sprayed particles, was generally a quadratic, the least value of the distance being showed about $45^{\circ}$ and the largest at about $15^{\circ}\;and\;55^{\circ}$, the decreasing rate of the change between $15^{\circ};and\;25^{\circ}$ was very small. 7) Effect of change of pressure on the travelling distance sprayed particles was generally a linear, the increasing rate of the charge was about 1.68, which was the most effective compared to the change of the other factors. 8) Effect of change of vortex chamber distance on the spraying distance was also generally a linear, the increasing rate being about 0.16, which was the least effective. 9) Effect of change of cap slope on the travelling distance was also generally a linear, the increasing rate was about 0.61 and its effect was about medium.

• 대한기계학회:학술대회논문집
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• 대한기계학회 2008년도 추계학술대회B
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• pp.2454-2459
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• 2008

The objective of this paper is to find out the most effective injection angle for the purpose of deicing through SC/Tetra, a commonly used CFD software. Nowadays, vehicles are developed giving priority to an improved interior which emphasizes a pleasant environment and thermal comfort without decreasing the basic performance. Clear visibility is one of the most important phenomenon. The primary factors which affect the efficiency of deicing are 3D geometry of Defrost Nozzle, the inlet velocity and temperature of the flow and the injection angle. However in this paper, all these parameters are optimized by changing the injection angle. A wide range of injection angle from 5 degree to 50 degree have been considered for analysis. A very good defrosting performance has been achieved with 45 degree injection angle which can satisfy the condition of NHTSA.

• 한국정보과학회논문지:소프트웨어및응용
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• 제36권8호
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• pp.653-663
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• 2009

본 논문에서는 세 대의 카메라를 이용하여 사각지대를 효과적으로 제거하기 위한 파노라믹 비전 시스템(panoramic vision system)을 제안한다. 차량의 후방에는 광각 카메라를 사용하여 후방 거울(rear-view mirror)로부터 보이지 않는 사각지대를 제거하며, 나머지 두 대의 카메라는 측면 거울(side-view mirror)의 아래에 설치하여 측면 거울로 보지 못하는 사각지대를 제거한다. 좀 더 효과적인 사각지대 제거를 위해서 세 대의 카메라에서 얻어지는 영상을 정합하는 방법을 제공한다. 먼저, 후방 카메라에서 얻은 영상을 보정하고, 보정된 영상에서 focus-of-contraction(FOC)을 구한다. 그 뒤에 측방 카메라의 영상과 후방 카메라의 영상 사이의 호모그래피(homography)를 구한다. 그 다음으로 영상을 차도와 배경 영역으로 분리하고, 호모그래피를 사용하여 분리한 차도를 정합하고, 가상의 평면에 배경을 투영하여 최종정합을 완성한다. 마지막으로 정합된 영상을 보다 효과적으로 보여주기 위한 실린더 파노라마 영상, 가상의 Top-view 시스템, 그리고 차량의 다양한 정보와 함께 사각지대 영상을 보여주는 통합 정보 가시화 영상을 생성하여 제공한다.

• 전자공학회논문지
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• 제50권6호
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• pp.131-137
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• 2013

광각 카메라는 단 초점 렌즈를 장착하여 넓은 시야의 이미지를 처리하는데, 렌즈의 광학 문제로 인해 이미지에 베럴 왜곡(barrel distortion)이 발생한다. 본 논문에서는 베럴 왜곡을 실시간 디지털 신호처리를 통해 보정하기 위한 낮은 복잡도의 프로세서 구조를 제시하고 이를 실제 구현하여 유효성을 검증하였다. 제안하는 왜곡 보정 프로세서는 하드웨어 복잡도를 낮추기 위해서, 좌표 위치 보정에 필요한 계산을 점증적(incremental)으로 수행한다. 또한, 높은 보정 속도를 달성하기 위해 파이프 라인 구조로 설계하였다. 설계된 보정 프로세서는 $0.11{\mu}m$ complementary metal-oxide semiconductor(CMOS) 공정을 사용하여 14.3K의 논리 게이트로 구현되었다. $2048{\times}2048$ 픽셀 영상에 대하여, 최대 314MHz의 동작 주파수로 초당 74.86번의 속도로 보정이 가능하다.