• 대한조선학회논문집
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• 제39권3호
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• pp.64-74
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• 2002

선체 휘핑 해석 전용 프로그램은 모멘텀 슬래밍 이론을 사용하여 비선형 유체충격력을 추정하였으며, Timoshenko 보이론에 기초하여 선체 hull girder를 탄성체로 모델링하고 있다. 개발된 프로그램에 대하여 슬래밍 충격력의 효과, 유탄성해석의 효과 그리고, 선속, 파고, 파장 등 각종 설계 변수가 미치는 효과 등에 관한 검증 계산을 수행하였고, 실제 선박 설계에의 적용 예를 보임으로써 본 프로그램의 설계 활용성을 확인하였다. 본 프로그램은 각종 입출력자료의 GUI 처리 및 선박 운동에 대한 시뮬레이션 제공 등 다양한 기능과 특성을 가지고 있다.

• Maxillofacial Plastic and Reconstructive Surgery
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• 제39권
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• pp.2.1-2.6
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• 2017

Background: All clinicians are aware of the difficulty of installing a dental implant in posterior maxilla because of proximate position of maxillary sinus, insufficient bone width, and lower bone density. This study is to examine which factors will make the implantation in the posterior maxilla more difficult, and which factors will affect the postoperative implant stability in this region. Methods: Five hundred seventy-three fixtures on the maxilla posterior were included for this study from all the patients who underwent an installation of the dental implant fixture from January 2010 to December 2014 at the Department of Oral and Maxillofacial Surgery in Pusan National University Dental Hospital (Yangsan, Korea). The postoperative implant stability quotient (ISQ) value, fixture diameter and length, presence of either bone graft or sinus lift, and graft material were included in the reviewed factors. The width and height of the bone bed was assessed via preoperative cone beam CT image analysis. The postoperative ISQ value was taken just before loading by using the OsstellTM $mentor^{(R)}$ (Integration Diagnostics AB, Gothenburg, Sweden). The t test and ANOVA methods were used in the statistical analysis of the data. Results: Mean ISQ of all the included data was 79.22. Higher initial bone height, larger fixture diameter, and longer fixture length were factors that influence the implant stability on the posterior edentulous maxilla. On the other hand, the initial bone width, bone graft and sinus elevation procedure, graft material, and approach method for sinus elevation showed no significant impact associated with the implant stability on the posterior edentulous maxilla. Conclusions: It is recommended to install the fixtures accurately in a larger diameter and longer length by performing bone graft and sinus elevation.

• 비파괴검사학회지
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• 제20권6호
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• pp.545-554
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• 2000

충격에 의해 복합 재료 내에 발생하는 층간 박리를 정량적으로 평가하기 위한 비파괴 방법중에서 Compton X-ray 역산란 기술은 초음파에 비해 비접촉식이며 박리 층간의 상호간섭이 없어 복합재료 판면의 박리 층의 위치와 크기를 검사하는데 효과적인 방법으로 사용되어 왔다. 그러나 X-ray역산란 기술에 있어서 복합재료의 박리 층과 같은 미세한 결함의 측정을 위해 측정 정도를 높이면 역산란 양의 감소로 인해 신호 대 잡음 비(SNR)가 급격히 감소하여 결함검출 가능성이 크게 저하된다. 본 논문에서는 복합재료의 특성을 고려한 X-ray 역산란 모델을 기초로 적응필터를 사용하여 결함신호를 비선형 감쇄, 빔 경화(X-ray hardening), 비균질 특성과 같은 잡음 신호로부터 분리, 추출하는 방법을 제시하였다. 이렇게 분리된 결함신호로부터 정량적인 결함(박리)의 위치와 크기를 수학적 산란 모델과의 비교를 통해 최소 자승법을 이용하여 결정하였다.

• Wind and Structures
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• 제19권4호
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• pp.443-465
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• 2014

Hyperbolic thin-shell cooling towers have complicated vibration modes, and are very sensitive to the effects of group towers and wind-induced vibrations. Traditional aero-elastic models of cooling towers are usually designed based on the method of stiffness simulation by continuous medium thin shell materials. However, the method has some shortages in actual engineering applications, so the so-called "equivalent beam-net design method" of aero-elastic models of cooling towers is proposed in the paper and an aero-elastic model with a proportion of 1: 200 based on the method above with integrated pressure measurements and vibration measurements has been designed and carried out in TJ-3 wind tunnel of Tongji university. According to the wind tunnel test, this paper discusses the impacts of self-excited force effect on the surface wind pressure of a large-scale cooling tower and the results show that the impact of self-excited force on the distribution characteristics of average surface wind pressure is very small, but the impact on the form of distribution and numerical value of fluctuating wind pressure is relatively large. Combing with the Complete Quadratic Combination method (hereafter referred to as CQC method), the paper further studies the numerical sizes and distribution characteristics of background components, resonant components, cross-term components and total fluctuating wind-induced vibration responses of some typical nodes which indicate that the resonance response is dominant in the fluctuating wind-induced vibration response and cross-term components are not negligible for wind-induced vibration responses of super-large cooling towers.

• Coupled systems mechanics
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• 제2권3호
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• pp.231-253
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• 2013

The impact of spar-nacelle-blade coupling on edgewise dynamic responses of spar-type floating wind turbines (S-FOWT) is investigated in this paper. Currently, this coupling is not considered explicitly by researchers. First of all, a coupled model of edgewise vibration of the S-FOWT considering the aerodynamic properties of the blade, variable mass and stiffness per unit length, gravity, the interactions among the blades, nacelle, spar and mooring system, the hydrodynamic effects, the restoring moment and the buoyancy force is proposed. The aerodynamic loads are combined of a steady wind (including the wind shear) and turbulence. Each blade is modeled as a cantilever beam vibrating in its fundamental mode. The mooring cables are modeled using an extended quasi-static method. The hydrodynamic effects calculated by using Morison's equation and strip theory consist of added mass, fluid inertia and viscous drag forces. The random sea state is simulated by superimposing a number of linear regular waves. The model shows that the vibration of the blades, nacelle, tower, and spar are coupled in all degrees of freedom and in all inertial, dissipative and elastic components. An uncoupled model of the S-FOWT is then formulated in which the blades and the nacelle are not coupled with the spar vibration. A 5MW S-FOWT is analyzed by using the two proposed models. In the no-wave sea, the coupling is found to contribute to spar responses only. When the wave loading is considered, the coupling is significant for the responses of both the nacelle and the spar.

• 대한토목학회논문집
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• 제28권1A호
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• pp.39-49
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• 2008

본 연구에서는 교량의 노면조도 및 교량과 차량 사이의 상호작용을 고려한 수치해석방법을 사용하여 여러 매개변수에 대한 강판형교의 동적응답을 연구하였다. 대상교량은 건설교통부에서 제정한 "도로교 상부구조 표준도"에 수록되어 있는 지간이 20 m, 30 m와 40 m인 단순 강판형교를 사용하고, 여러 종류의 도로에 대하여 생성시킨 노면조도를 사용하였다. 차량은 2축과 3축 덤프트럭 및 5축 트랙터-트레일러인 표준트럭(DB-24)을 3차원으로 모델링하고, 교량은 주형을 보요소로, 콘크리트 바닥판은 쉘요소로 이상화시켰으며 주형과 콘크리트 바닥판 사이는 Rigid Link를 사용하여 3차원으로 모델링하였다. 이와 같은 차량 및 노면조도를 사용하여 강판형교의 지간별, 통행 차종별 및 노면조도별 충격계수와 DLA를 구하고 각국의 설계기준과 비교 검토하였다.

• 한국식품영양과학회지
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• 제42권11호
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• pp.1857-1863
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• 2013

전자선 조사된 마늘분말을 혼합하여 불고기소스를 제조한 후 살균처리($85^{\circ}C$, 30 min)와 혼합비(1, 3, 5%)에 따른 열발광(thermoluminescence, TL)특성을 서로 다른 연구기관에서 확인하였다. 비 조사 마늘분말이 혼합된 소스의 TL 발광곡선은 자연방사선에 의해 $300^{\circ}C$ 이후에서 나타났다. 그러나 조사원료(1 kGy, 10 kGy)가 혼합된 소스의 경우 $150{\sim}250^{\circ}C$에서 나타났으며, 원료의 혼합량 및 조사선량이 낮을수록 발광곡선의 강도는 감소하였다. TL ratio($TL_1/TL_2$)는 조사 원료가 혼합된 시료구에서도 모두 0.1 이하로 나타나 조사여부 판정은 어려웠으며, 살균 처리 후에는 발광강도는 감소하고 발광온도범위는 고온영역으로 이동하여 낮은 혼합시료(1 kGy 조사 마늘분말, 1%)에서는 판별이 어려운 것으로 확인되었다. 조사 원료가 소량 혼입된 가공식품의 판별 시에는 TL 발광곡선의 형태와 최대 발광온도를 복합적으로 고려하여 조사여부를 확인하여야 할 것으로 판단되었다.

• 한국의학물리학회지:의학물리
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• 제29권1호
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• pp.1-7
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• 2018

The $TomoTherapy^{(R)}$ beam-delivery method creates helical beam-junctioning patterns in the dose distribution within the target. In addition, the dose discrepancy results in the particular region where the resonance by pattern of dose delivery occurs owing to the change in the position and shape of internal organs with a patient's respiration during long treatment times. In this study, we evaluated the dose pattern of the longitudinal profile with the change in respiration. The superior-inferior motion signal of the programmable respiratory motion phantom was obtained using AbChes as a four-dimensional computed tomography (4DCT) original moving signal. We delineated virtual targets in the phantom and planned to deliver the prescription dose of 300 cGy using field widths of 1.0 cm, 2.5 cm, and 5.0 cm. An original moving signal was fitted to reflecting the beam delivery time of the $TomoTherapy^{(R)}$. The EBT3 film was inserted into the phantom movement cassette, and static, without the movement and with the original movement, was measured with signal changes of 2.0 s, 4.0 s, and 5.0 s periods, and 2.0 mm and 4.0 mm amplitudes. It was found that a dose fluctuation within ${\pm}4.0%$ occurred in all longitudinal profiles. Compared with the original movement, the region of the gamma index above 1 partially appeared within the target and the border of the target when the period and amplitude were changed. Gamma passing rates were 95.00% or more. However, cases for a 5.0 s period and 4.0 mm amplitude at a field width of 2.5 cm and for 2.0 s and 5.0 s periods at a field width of 5.0 cm have gamma passing rates of 92.73%, 90.31%, 90.31%, and 93.60%. $TomoTherapy^{(R)}$ shows a small difference in dose distribution according to the changes of period and amplitude of respiration. Therefore, to treat a variable respiratory motion region, a margin reflecting the degree of change of respiration signal is required.

• Imaging Science in Dentistry
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• 제50권3호
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• pp.227-236
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• 2020

Purpose: Image artifacts caused by patient motion cause problems in cone-beam computed tomography (CBCT) because they lead to distortion of the 3-dimensional reconstruction. This prospective study was performed to quantify patient movement during CBCT acquisition and its influence on image quality. Materials and Methods: In total, 412 patients receiving CBCT imaging were equipped with a wireless head sensor system that detected inertial, gyroscopic, and magnetometric movements with 6 dimensions of freedom. The type and amplitude of movements during CBCT acquisition were evaluated and image quality was rated in 7 different anatomical regions of interest. For continuous variables, significance was calculated using the Student t-test. A linear regression model was applied to identify associations of the type and extent of motion with image quality scores. Kappa statistics were used to assess intra- and inter-rater agreement. Chi-square testing was used to analyze the impact of age and sex on head movement. Results: All CBCT images were acquired in a 10-month period. In 24% of the investigations, movement was recorded (acceleration: >0.10 [m/s²]; angular velocity: >0.018 [°/s]). In all examined regions of interest, head motion during CBCT acquisition resulted in significant impairment of image quality (P<0.001). Movement in the horizontal and vertical axes was most relevant for image quality (R²>0.7). Conclusion: Relevant head motions during CBCT imaging were frequently detected, leading to image quality loss and potentially impairing diagnosis and therapy planning. The presented data illustrate the need for digital correction algorithms and hardware to minimize motion artefacts in CBCT imaging.

• 한국의학물리학회지:의학물리
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• 제24권4호
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• pp.220-229
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• 2013

Respiratory-induced dynamic tumors render free-breathing cone-beam computed tomography (FBCBCT) images with motion artifacts complicating the task of quantifying the internal target volume (ITV). The purpose of this paper is to study the visibility of the revealed ITV when the imaging dose parameters, such as the kVp and mAs, are varied. The $Trilogy^{TM}$ linear accelerator with an On-Board Imaging ($OBI^{TM}$) system was used to acquire low-imaging-dose-mode (LIDM: 110 kVp, 20 mA, 20 ms/frame) and high-imaging-dose-mode (HIDM: 125 kVp, 80 mA, 25 ms/frame) FBCBCT images of a 3-cm diameter sphere (density=0.855 $g/cm^3$) moving in accordance to various sinusoidal breathing patterns, each with an unique inhalation-to-exhalation (I/E) ratio, amplitude, and period. In terms of image ITV contrast, there was a small overall average change of the ITV contrast when going from HIDM to LIDM of $6.5{\pm}5.1%$ for all breathing patterns. As for the ITV visible volume measurements, there was an insignificant difference between the ITV of both the LIDM- and HIDM-FBCBCT images with an average difference of $0.5{\pm}0.5%$, for all cases, despite the large difference in the imaging dose (approximately five-fold difference of ~0.8 and 4 cGy/scan). That indicates that the ITV visibility is not very sensitive to changes in imaging dose. However, both of the FBCBCT consistently underestimated the true ITV dimensions by up to 34.8% irrespective of the imaging dose mode due to significant motion artifacts, and thus, this imaging technique is not adequate to accurately visualize the ITV for image guidance. Due to the insignificant impact of imaging dose on ITV visibility, a plausible, alternative strategy would be to acquire more X-ray projections at the LIDM setting to allow 4DCBCT imaging to better define the ITV, and at the same time, maintain a reasonable imaging dose, i.e., comparable to a single HIDM-FBCBCT scan.