• 대한방사선치료학회지
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• 제30권1_2호
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• pp.83-95
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• 2018

목 적 : 폐암의 호흡동조방사선치료(Respiratory Gated Radiotherapy, RGRT)계획수립 후 표적 주변에 위치하고 있는 정상장기의 경우에는 움직임과 용적변화가 고려되지 않은 상태에서 선량평가가 이루어지는 경우가 많다. 본 연구에서는 적응형방사선치료(Adaptive Radiotherapy, ART)에서 많이 사용되는 변형영상정합(Deformable Image Registration, DIR)을 이용하여 호흡동조방사선치료 시 특정 위상에서의 정상장기의 움직임을 반영한 4차원-선량평가를 진행하였으며, 3차원 선량평가와의 차이를 연구하였다. 또한, 폐암의 치료계획평가 시 환자 호흡에 따른 정상장기의 움직임과 용적변화에 대한 분석 및 고려가 필요한 지 알아보고자 한다. 대상 및 방법 : 호흡동조방사선치료를 받은 폐암 환자 10명을 대상으로 하였다. Eclipse(Ver 13.6 Varian, USA)로 최고 위상 CT영상에 그려진 구조물을 모든 위상영상에 Propagation($Eclipse^{TM}$)이나 Segmentation Wizard($Eclipse^{TM}$)의 메뉴로 동일하게 설정하였으며, Center-to-Center 방식으로 구조물의 움직임 및 용적을 분석하였다. 또한, 4차원 선량평가를 위해 VELOCITY 프로그램(VELOCITY Ver 4.0, Varian, USA)을 이용하여 각 위상의 영상과 선량분포를 최고 위상 CT영상에 변형하였으며, 선량을 합산하여 정상장기의 4차원 선량평가를 실시하고, 3차원 선량평가와 비교분석을 하였다. 또한, 4차원 선량분포의 검증을 위해 $QUASAR^{TM}$ Phantom(Modus Medical Devices)과 $GAFCHROMIC^{TM}$ EBT3 Film(Ashland, USA)을 사용하여 4차원 감마분석을 시행하였다. 결 과 : 들숨과 날숨 구간의 움직임은 우측 폐가 축 방향 $0.989{\pm}0.34cm$로 가장 컸으며, 척수가 측 방향 -0.001 cm로 가장 작았다. 30~70 % 구간의 움직임은 식도가 축 방향 $0.52{\pm}0.21cm$로 가장 컸으며, 척수가 전후방향 $0.013{\pm}0.01cm$로 가장 작았다. 용적은 우측 폐가 33.5 %로 가장 큰 변화율을 보였다. 3차원 선량평가와 4차원 선량평가에서의 PTV 선량균질지수(Conformity Index, CI) 값과 처방선량지수(Homogeneity Index, HI) 값의 차이는 각각 최대 0.076, 0.021, 최소 0.011, 0.0으로 평가되었다. 정상장기의 경우 4차원 선량평가에서 0.0045~2.76 % 차이를 보였다. 모든 환자의 4차원 감마통과율은 평균 $98.1{\pm}0.42%$로 확인되었고, 모두 기준 95 %를 통과하였다. 결 론 : 모든 환자의 PTV 선량균질지수 값은 4차원 선량평가 시 더 유의한 값임을 확인할 수 있었으며, 처방 선량지수는 두 선량평가에서 차이를 보이지 않았다. 호흡에 의한 움직임이 고려된 4차원 선량분포에서 PTV 경계부분이 채워져 3차원 선량분포에서보다 선량이 더욱 균질한 것을 확인할 수 있었다. 정상장기의 4차원 선량평가에서 0.004~2.76 % 차이가 있었으며, 척수를 제외한 모든 정상장기에서 두 평가방법의 차이유의를 확인할 수 있었다. 정상장기의 3차원 선량평가 시 과소평가가 이루어 질 수 있다는 사실을 본 연구를 통해 알 수 있었으며, 호흡에 의한 정상장기의 선량변화가 예상되는 경우 변형영상정합을 이용한 4차원 선량평가를 고려할 수 있을 것이다. 변형영상정합을 이용한 4차원 선량평가는 환자의 호흡에 의한 정상장기의 움직임과 용적 변화를 반영하는 조금 더 현실적인 선량평가방법이 될 것이라고 사료된다.

• Smart Structures and Systems
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• 제9권3호
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• pp.231-251
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• 2012

The stochastic optimal control for a piezoelectric spherically symmetric shell subjected to stochastic boundary perturbations is constructed, analyzed and evaluated. The stochastic optimal control problem on the boundary stress output reduction of the piezoelectric shell subjected to stochastic boundary displacement perturbations is presented. The electric potential integral as a function of displacement is obtained to convert the differential equations for the piezoelectric shell with electrical and mechanical coupling into the equation only for displacement. The displacement transformation is constructed to convert the stochastic boundary conditions into homogeneous ones, and the transformed displacement is expanded in space to convert further the partial differential equation for displacement into ordinary differential equations by using the Galerkin method. Then the stochastic optimal control problem of the piezoelectric shell in partial differential equations is transformed into that of the multi-degree-of-freedom system. The optimal control law for electric potential is determined according to the stochastic dynamical programming principle. The frequency-response function matrix, power spectral density matrix and correlation function matrix of the controlled system response are derived based on the theory of random vibration. The expressions of mean-square stress, displacement and electric potential of the controlled piezoelectric shell are finally obtained to evaluate the control effectiveness. Numerical results are given to illustrate the high relative reduction in the root-mean-square boundary stress of the piezoelectric shell subjected to stochastic boundary displacement perturbations by the optimal electric potential control.

• 대한전자공학회논문지SD
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• 제42권5호
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• pp.15-22
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• 2005

본 논문에서는 생명체의 구조를 모방하여, 디지털시스템에서 자가검출과 자가치유가 가능한 구조를 제안한다. 자가치유시스템은 인공 셀의 2차 배열과 여분의 인공 셀로 구성된다. 인공 셀은 멀티플렉서를 기본으로 한 로직블록(logic block)과 로직블록을 제어하기 위한 게놈블록(genome block)으로 구성된다. 인공 셀은 자가검출이 가능하도록 DCVSL (differential cascode voltage switch logic)구조로 설계된다. 만약 인공 셀에서 고장이 발생하면, 자가 검출되고 고장 난 인공 셀이 속한 열은 bypass기능만을 가지고 치유를 위해, 여분 셀과 이웃 셀을 이용하여 시스템을 재구성한다. 하이닉스 $0.35{\mu}m$공정을 이용해 $1.14{\times}0.99mm^2$의 코어면적을 가지는 2비트 업다운카운터를 제작하였고 회로시뮬레이션과 칩 테스트를 통해 검증하였다.

• Applied Microscopy
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• 제47권3호
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• pp.203-207
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• 2017

A homogeneous $KNbO_3$ (KN) phase was formed by sintering at $1,040^{\circ}C$ for 1 hour, without formation of the $K_2O$-deficient secondary phase even though suffering the minor loss of $K_2O$. KN liquid phase was formed during sintering and abnormal grain growth occurred in this specimen. The detailed microstructural observations on KN during sintering were carried out using high resolution transmission electron microscopy. The ledged structures were found at the KN grain boundary and the abnormal grain growth was performed by the lateral migration of these ledges in the presence of the liquid phase. The liquid pockets were found in the KN grains. They have various external shapes mainly due to the kinetic factors. They have atomically flat interfaces with some ledges with one atomic height. The slight deficient $K_2O$ by evaporation might somewhat reduce the melting point of KN from the reported at $1,058^{\circ}C$. The liquid pockets play an important role in supplying the liquid phase during the abnormal grain growth in the sintering process of KN ceramics.

• Applied Microscopy
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• 제24권3호
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• pp.55-66
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• 1994

This study was carried out to investigate the histological changes of sperm cells in testis, obtained from 100 of 3-year-old male rainbow trout (Oncorhynchus mykiss) collected and analysed from March in 1992 to February in 1993. Especially, the ultrastructural changes of spermatogonia, primary and secondary spermatocytes, spermatids, and spermatozoa were examined to describe the reproductive cycles of this species. The results obtained in this study were as follows: The ultrastructures of the gonadotrophs largely parallel the cyclical changes in the testes. Each nest of cells belongs to one spermatogenetic stage, although nests at different stages can be found within the one lobule. At first keterochromatin is dispersed and then is condensed. In mature gamete, the nucleus is dense and homogeneous. The nuclear membrane appeared at the beginning of differentiation. In spermatogonia, Sertoli cells are located at the periphery of their cytoplasm. In the primary spermatocytes, the small mitochondria are abundant over the outer cytoplasm. During cell differentiation, the cytoplasm decreases and the nucleus increases. In spermatids, the protein masses moved towards the posterior part of the nucleus. In late spermatids, the two large mitochondria are located over the cytoplasm. In spermatozoa, two spheroidal mitochondria (about 145nm long) are situated in parallel between the nucleus and the axoneme. Spermatozoa mitochondria are assembled into an organized sheath surrounding the outer dense fibres and axoneme of the flagellar midpiece. The two centrioles are quite separate and the central pair and sheath complex of the flagellum is inserted into the base of the distal centriole.

• Carbon letters
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• 제26권
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• pp.18-24
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• 2018

Pollution of chloride ion-reinforced concrete can trigger active corrosion processes that reduce the useful life of structures. Multifunctional materials used as a counter-electrode by electrochemical techniques have been used to rehabilitate contaminated concrete. Cement-based pastes added to carbonaceous material, fibers or dust, have been used as an anode in the non-destructive Electrochemical Chloride Extraction (ECE) technique. We studied the performance of the addition of Carbon Fiber (CF) in a cement-graphite powder base paste used as an anode in ECE of concretes contaminated with chlorides from the preparation of the mixture. The experimental parameters were: 2.3% of free chlorides, 21 days of ECE application, a Carbon Fiber Volume Fraction (CFVF) of 0.1, 0.3, 0.6, 0.9%, a lithium borate alkaline electrolyte, a current density of $4.0A/m^2$ and a cement/graphite ratio of 1.0 for the paste. The efficiency of the ECE in the traditional technique using metal mesh as an anode was 77.6% and for CFVF of 0.9% it was 90.4%, with a tendency to increase to higher percentages of the CFVF in the conductive cement-graphite paste, keeping the pH stable and achieving a homogeneous ECE in the mass of the concrete contaminated with chlorides.

• 한국재료학회지
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• 제25권9호
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• pp.480-486
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• 2015

$Pb_{1-x}MoO_4:Er^{3+}/Yb^{3+}$ phosphors with various doping concentrations of $Er^{3+}$ and $Yb^{3+}$ ($x=Er^{3+}+Yb^{3+}$, $Er^{3+}=0.05$, 0.1, 0.2, and $Yb^{3+}=0.2$, 0.45) are successfully synthesized using a microwave sol-gel method, and the up-conversion photoluminescence properties are investigated. Well-crystallized particles, which are formed after heat treatment at $900^{\circ}C$ for 16 h, exhibit a fine and homogeneous morphology with particle sizes of $2-5{\mu}m$. Under excitation at 980 nm, the $Pb_{0.7}MoO_4:Er_{0.1}Yb_{0.2}$ and $Pb_{0.5}MoO_4:Er_{0.05}Yb_{0.45}$ particles exhibit a strong 525 nm emission band, a weak 550 nm emission band in the green region, and a very weak 655 nm emission band in the red region. The Raman spectra of the doped particles indicate the presence of strong peaks at higher and lower frequencies induced by the disordered structures of $Pb_{1-x}MoO_4$ through the incorporation of the $Er^{3+}$ and $Yb^{3+}$ ions into the crystal lattice, which results in the unit cell shrinkage accompanying the new phase formation of the $MoO_{4-x}$ group.

• Earthquakes and Structures
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• 제14권4호
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• pp.313-322
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• 2018

The present study is dedicated to investigate the SH body-as well as Love-waves propagation effects in porous media with uncertain porosity and permeability. A unified formulation of the governing equations for one-dimensional (1-D) wave propagation in anisotropic porous layered media is presented deterministically. The uncertainties around the above two cited parameters are taken into account by random fields with the help of Monte Carlo Simulations (MCS). Random samples of the porosity and the permeability are generated according to the normal and lognormal distribution functions, respectively, with a mean value and a coefficient of variation for each one of the two parameters. After performing several thousands of samples, the mathematical expectation (mean) of the solution of the wave propagation equations in terms of amplification functions for SH waves and in terms of dispersion equation for Love-waves are obtained. The limits of the Love wave velocity in a porous soil layer overlaying a homogeneous half-space are obtained where it is found that random variations of porosity change the zeros of the wave equation. Also, the increase of uncertainties in the porosity (high coefficient of variation) decreases the mean amplification function amplitudes and shifts the fundamental frequencies. However, no effects are observed on both Love wave dispersion and amplification function for random variations of permeability. Lastly, the present approach is applied to a case study in the Adapazari town basin so that to estimate ground motion accelerations lacked in the fast-growing during the main shock of the damaging 1999 Kocaeli earthquake.

• Steel and Composite Structures
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• 제28권5호
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• pp.589-606
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• 2018

The previous studies reflected the significant effect of neutral-axis position and coupling of in-plane and out-of-plane displacements on behavior of functionally graded (FG) nanobeams. In thin FG beam, this coupling can be eliminated by a proper choice of the reference axis. In shear deformable FG nanobeam, not only this coupling can't be eliminated but also the position of neutral-axis is dependent on through-thickness distribution of shear strain. For the first time, in this paper it is avoided to guess a shear strain shape function and the exact shape function and consequently the exact position of neutral axis for arbitrary gradation of higher order nanobeam are obtained. This paper presents new methodology based on differential transform and collocation methods to solve coupled partial differential equations of motion without any simplifications. Using exact position of neutral axis and higher order beam kinematics as well as satisfying equilibrium equations and traction-free conditions without shear correction factor requirement yields to better results in comparison to the previously published results in literature. The classical rule of mixture and Mori-Tanaka homogenization scheme are considered. The Eringen's nonlocal continuum theory is applied to capture the small scale effects. For the first time, the dependency of exact position of neutral axis on length to thickness ratio is investigated. The effects of small scale, length to thickness ratio, Poisson's ratio, inhomogeneity of materials and various end conditions on vibration and buckling of local and nonlocal FG beams are investigated. Moreover, the effect of axial load on natural frequencies of the first modes is examined. After degeneration of the governing equations, the exact new formulas for homogeneous nanobeams are computed.

• Wind and Structures
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• 제5권2_3_4호
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• pp.177-192
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• 2002

Computation solutions for the flow around a cube, which were generated as part of the Computational Wind Engineering 2000 Conference Competition, are compared with full-scale measurements. The three solutions shown all use the RANS approach to predict mean flow fields. The major differences appear to be related to the use of the standard $k-{\varepsilon}$, the MMK $k-{\varepsilon}$ and the RNG $k-{\varepsilon}$ turbulence models. The inlet conditions chosen by the three modellers illustrate one of the dilemmas faced in computational wind engineering. While all modeller matched the inlet velocity profile to the full-scale profile, only one of the modellers chose to match the full-scale turbulence data. This approach led to a boundary layer that was not in equilibrium. The approach taken by the other modeller was to specify lower inlet turbulent kinetic energy level, which are more consistent with the turbulence models chosen and lead to a homogeneous boundary layer. For the $0^{\circ}$ case, wind normal to one face of the cube, it is shown that the RNG solution is closest to the full-scale data. This result appears to be associated with the RNG solution showing the correct flow separation and reattachment on the roof. The other solutions show either excessive separation (MMK) or no separation at all (K-E). For the $45^{\circ}$ case the three solutions are fairly similar. None of them correctly predicting the high suctions along the windward edges of the roof. In general the velocity components are more accurately predicted than the pressures. However in all cases the turbulence levels are poorly matched, with all of the solutions failing to match the high turbulence levels measured around the edges of separated flows. Although all of the computational solutions have deficiencies, the variability of results is shown to be similar to that which has been obtained with a similar comparative wind tunnel study. This suggests that the computational solutions are only slightly less reliable than the wind tunnel.