• 한국복합재료학회:학술대회논문집
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• 한국복합재료학회 2000년도 추계학술발표대회 논문집
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• pp.110-114
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• 2000

The Interlaminar fracture behavior of hybrid composite with non-woven carbon tissue was investigated under Mode I (DCB) and Mode II (ENF) loading condition. Hybrid composites were manufactured by means of inserting a non-woven tissue between prepreg layers. Two kinds of specimens were prepared from [0]$_{24}$ and [$0_{12}/0_{12}$]. Where, the symbol "/" means that a non-woven carbon tissue was located at 0/0 mid-plane of the specimen. The interlaminar fracture toughness of hybrid composites was compared with that of CFRP. The fracture surfaces of the specimens were observed using optical microscope and SEM, and the failure mechanism was discussed. The hybrid laminates, which are made by inserting non-woven carbon tissue between layers, were shown to be effective to remarkably improve Mode II fracture toughness.toughness.

• Journal of Mechanical Science and Technology
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• 제17권6호
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• pp.796-804
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• 2003

The use of fracture mechanics has traditionally concentrated on crack growth under an opening mechanism. However, many service failures occur from cracks subjected to mixed-mode loading. Hence, it is necessary to evaluate the fatigue behavior under mixed-mode loading. Under mixed-mode loading, not only the fatigue crack propagation rate is of importance, but also the crack propagation direction. In modified range 0.3$\leq$a/W$\leq$0.5, the stress intensity factors (SIFs) of mode I and mode II for the compact tension shear (CTS) specimen were calculated by using elastic finite element analysis. The propagation behavior of the fatigue cracks of cold rolled stainless steels (STS304) under mixed-mode conditions was evaluated by using K$\_$I/ and $_{4}$ (SIFs of mode I and mode II). The maximum tangential stress (MTS) criterion and stress intensity factor were applied to predict the crack propagation direction and the propagation behavior of fatigue cracks.

• 한국생산제조학회지
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• 제21권2호
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• pp.276-282
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• 2012

This study looked for Mode status of each for fatigue crack growth behavior about the repeat load of mode I and the static load of mode II. The experiment was performed in the state of the repetition frequency of the sine wave 10Hz, the stress ratio 0.1, maximum load 300kg.f, a static load 0, 100, 200, 300kg.f, As the experimental results, in mode of static load, while the load value increases, the crack growth rate is slower as the energy of a crack mixing grows. Mode I and the power mode II get an influence each other in the direction of crack propagation path, but as they eventually get closer to the breaking point of the crack growth, it is dominated by the mode I.

• 한국의학물리학회지:의학물리
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• 제27권3호
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• pp.169-174
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• 2016

The aim of this study is to investigate the delivery accuracy of intensity-modulated radiation therapy (IMRT) plans in the two-headed mode of the ViewRay$^{TM}$ system in comparison with that of the normal operation treatment plan of the machine. For this study, a total of eight IMRT plans and corresponding verification plans were generated (four head and neck, two liver, and two prostate IMRT plans). The delivered dose distributions were measured using ArcCHECK$^{TM}$ with the insertion of an ionization chamber. We measured the delivered dose distributions in three-headed mode (normal operation of the machine), two-headed mode with head 1 disabled, two-headed mode with head 2 disabled, and two-headed mode with head 3 disabled. Therefore, a total of four measurements were performed for each IMRT plan. The global gamma passing rates (3%/3 mm) in three-headed mode, head 1 disabled, head 2 disabled, and head 3 disabled were $99.9{\pm}0.1%$, $99.8{\pm}0.3%$, $99.6{\pm}0.7%$, and $99.7{\pm}0.4%$, respectively. The difference in the gamma passing rates of the three- and two-headed modes was insignificant. With 2%/2 mm, the rates were $96.6{\pm}3.6%$, $97.2{\pm}3.5%$, $95.7{\pm}6.2%$, and $95.5{\pm}4.3%$, respectively. Between three-headed mode and head 3 disabled, a statistically significant difference was observed with a p-value of 0.02; however, the difference was minimal (1.1%). The chamber readings showed differences of approximately 1% between three- and two-headed modes, which were minimal. Therefore, the treatment plan delivery in the two-headed mode of the ViewRay$^{TM}$ system seems accurate and robust.

• 한국입자에어로졸학회지
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• 제9권1호
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• pp.7-21
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• 2013

Twelve-hour size-resolved atmospheric aerosols were measured to determine size distributions of water-soluble organic carbon(WSOC) during daytime and nighttime, and to investigate sources and formation pathways of WSOC in individual particle size classes. Mass, WSOC, ${NO_3}^-$, $K^+$, and $Cl^-$ at day and night showed mostly bimodal size distributions, peaking at the size range of $0.32-0.55{\mu}m$(condensation mode) and $3.1-6.2{\mu}m$(coarse mode), respectively, with a predominant condensation mode and a minor coarse mode. While ${NH_4}^+$ and ${SO_4}^{2-}$ showed unimodal size distributions which peaked between 0.32 and $0.55{\mu}m$. WSOC was enriched into nuclei mode particles(< $0.1{\mu}m$) based on the WSOC-to-mass and WSOC-to-water soluble species ratios. The sources and formation mechanisms of WSOC were inferred in reference to the size distribution characteristics of inorganic species(${SO_4}^{2-}$, ${NO_3}^-$, $K^+$, $Ca^{2+}$, $Na^+$, and $Cl^-$) and carbon monoxide. Nuclei mode WSOC was likely associated with primary combustion sources during daytime and nighttime. Among significant sources contributing to the condensation mode WSOC were homogeneous gas-phase oxidation of VOCs, primary combustion emissions, and fresh(or slightly aged) biomass burning aerosols. The droplet mode WSOC could be attributed to aqueous oxidation of VOCs in clouds, cloud-processed biomass burning aerosols, and small contributions from primary combustion sources. From the correlations between WSOC and soil-related particles, and between WSOC and sea-salt particles, it is suggested that the coarse mode WSOC during daytime is likely to condense on the soil-related particles($K^+$ and $Ca^{2+}$), while the WSOC in the coarse fraction during nighttime is likely associated with the sea-salt particles($Na^+$).

• 한국광학회지
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• 제19권3호
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• pp.169-174
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• 2008

열처리에 의한 광섬유 코어의 모드 확산과 모드 진화 현상을 이용하여 일반 통신용 단일모드 광섬유와 하이텔타(high ${\Delta}$) 광섬유 사이의 접속 손실을 줄일 수 있는 기법들을 제시하였다. 실험결과는 하이텔타 광섬유의 적절한 열처리를 통해 기계적 접속 손실이 2.3 dB에서 0.1 dB까지 감소함을 나타내었다. 반면 융착접속 후 접속 부위에 전기 방전이나 산소 불꽃으로 열을 인가하는 방법으로 $0.2{\sim}0.4dB$ 정도의 접속 손실을 달성하였다.

• Journal of Periodontal and Implant Science
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• 제31권3호
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• pp.531-542
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• 2001

Periodontal debridement is most important procedure in periodontal treatment, because periodontal disease is the biofilm infection. The use of ultrasonic instrument has many clinical advantages compared to classical hand instrument. The introduction of newly developed ultrasonic scaler tips made the use of ultrasonic scaler popular. However the study of tooth substance removal according to the working parameters of ultrasonic scaler with newly developed tips is not sufficient. The purpose of this study is to evaluate the effects of working parameters of piezoelectric ultrasonic scaler with curette tip on casting gold removal. The working parameters was standardized by the sledge device which controls lateral force(0.5 N, 1.0 N, 2.0 N) and power setting was adjusted 2, 4, 8 in P mode and S mode and instrumentation time was 5 seconds. The defect depth and width were measured with profile meter and defect surface was examined by SME. The depth of defect was significantly large in S mode( $39.58{\pm}19.35{\mu}m$) compared to P mode( $8.37{\pm}6.98{\mu}m$). There was significant decrease of depth of defect between 1.0N($32.87{\pm}27.18{\mu}m$) and 2.0N( $14.86{\pm}15.04{\mu}m$). The area of defect was also significantly large in S mode($4482.42{\pm}3551.71{\mu}m^2$) compared to P mode( $922.06{\pm}960.32{\mu}m^2$). There was significant decrease of area of defect between 1.0N($3889.12{\pm}3936.00{\mu}m$) and 2.0N( $974.66{\pm}986.01{\mu}m$). The change of mode did not effect on the width of the defect. The change of power setting did not effect on the depth, width, and area of defect. In spite of limitation of this study it could be concluded that the use of piezoelectric ultrasonic scaler with curette tip on S mode could make significant tooth substance loss.

• Tuberculosis and Respiratory Diseases
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• 제42권3호
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• pp.351-360
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• 1995

연구배경: 압력보조는 환자의 흡기시 정해진 양의 양압을 보조하여 상시호흡량을 증가시키거나, 호흡일을 경감시키는 목적으로 쓰이는 기계환기법으로 본 연구는 자발적 호흡이 허용되는 SIMV 및 CPAP 양식에서 PS를 사용할 경우 환자의 호흡역학상 어떤 차이가 있는지 알아보고자 하였다. 방법: 중환자실에 입원하여 호흡부전으로 기계환기중인 환자로 임상적으로 안정되었고 자발적 호흡횟수가 분당 12회 이상인 환자 14명을 대상으로, 먼저 CPAP(3 cm $H_2O$) 양식하에서 0, 5, 10 및 15 cm $H_2O$의 PS를 순서대로 적용하면서 CP-100 pulmonary monitor(Bicore, USA)를 이용하여 호흡역학 지수들을 측정하고 이어서 SIMV 양식으로 바꾸어 같은 방법으로 호흡역학 지수들을 측정하였다. 결과: 1) CPAP 및 SIMV 방식하에서 PS가 호흡역학에 미친 공통된 효과 CPAP 양식하에서 PS를 증가시킴에 따라 상시호흡량은 증가하였고, WOB과 PTP는 감소하였다. SIMV 방식하에서도 PS를 증가시킴에 따라 상시호흡량은 증가하였고, WOB과 PTP 역시 유의하게 감소하였다. 2) CPAP 및 SIMV 방식하에서 PS가 호흡역학에 미치는 효과의 차이 CPAP 방식하에서 PS를 증가시킴에 따라 분당호흡수는 유의한 변동이 없었고, $P_{0.1}$과 $T_1/T_{TOT}$은 유의하게 감소되었다. SIMV 방식하에서 PS를 증가시킴에 따라 분당호흡수는 유의하게 감소한 반면, $P_{0.1}$과 $T_1/T_{TOT}$은 유의한 변동이 없었다. 3) CPAP+PS 양식에서 SIMV 단독양식에서와 같은 상시호흡량을 얻는 상태에서의 호흡역학의 비교 동일 환자에서 CPAP+PS 양식으로 SIMV 단독양식에서의 상시호흡량이 얻어지는 상태에서 분당호흡수 WOB, $P_{0.1}$ 등에는 양 방식 간에 차이가 없었으나 PTP와 $T_1/T_{TOT}$은 CPAP+PS 양식이 유의하게 낮았다. 결론: 기계호흡에서 압력보조의 사용은 CPAP 및 SIMV 양식 모두에서 상시호흡량을 증가시키고, 환자의 호흡일, 호흡근 산소소모량 지수를 감소시켰으며, 분당호흡수의 감소는 SIMV 방식에서만 관찰되었고, 중추성호흡추진력의 감소와 호흡근의 지구력지수의 호전은 CPAP 방식에서만 관찰되었다. 한편 상시호흡량이 같은 수준에서의 CPAP+ PS 방법은 SIMV 법에 비해 호흡근의 일효율이 더 높고 호흡근의 지구력지수가 더 우수하였다. 따라서, 기계적환기 유지기나 이탈과정의 환자에서 압력보조의 겸용은 환자의 호흡역학 상태를 개선하는 것으로 사료된다.

• 전기전자학회논문지
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• 제19권2호
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• pp.260-264
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• 2015

본 논문에서는 부하전류를 감지하여 스위칭 방식과 선형 방식의 레귤레이터를 동작하기 위한 mode selector를 제안한다. 제안된 mode selector는 선형 방식과 스위칭 방식으로의 모드 전환이 가능하며, 경부하 조건에서 낮은 효율을 갖는 스위칭 방식의 레귤레이터의 단점을 보완하고자 제안되었다. 경부하 조건에서는 선형 방식의 레귤레이터로 mode를 전환함으로써 경부하 상태에서도 높은 효율을 제공할 수 있다. 설계한 mode selector는 동부 하이텍의 $0.18{\mu}m$ CMOS 공정을 이용하였다.

• 대한방사선기술학회지:방사선기술과학
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• 제40권2호
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• pp.213-218
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• 2017

최근 고위험 임신군이 증가함에 따라 과거에 비해 음향파워 세기가 높은 도플러초음파 이용이 산전 진단에서 점차 증가하고 있으며, 여러 기관에서 가이드라인을 설정하여 과도한 노출을 자제하고 있다. 따라서 본 연구에서는 장시간 초음파검사 실시에 따른 검사모드 별 체표면의 온도변화를 알아보고 열효과에 영향을 받지 않는 노출시간을 고찰해 보고자 하였다. 시간경과에 따른 B mode, C mode, PD mode 별 초음파를 조사한 부위와 조사하지 않은 부위의 온도변화를 측정하여 차이를 비교하였으며 B mode는 초음파 조사 후 10분, 50분에서, C mode는 20분부터, PD mode는 30분부터 온도변화에 유의한 차이를 나타내었다(p<0.01). 측정시점에 따라 3개의 mode에서 모두 온도상승에 차이를 보였으며(p<0.000), PD mode가 가장 온도변화에 민감한 반응을 나타내었다. 또한 초음파 노출시간이 증가함에 따라 온도상승 시간이 짧아짐을 알 수 있었다. 따라서 배아나 태아를 관찰하기 위한 초음파검사 시 과도한 검사시간을 피하여 진단목적으로만 신속하게 사용할 것을 권고한다.