• Composites Research
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• v.20 no.5
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• pp.1-6
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• 2007

This study was performed to make a comparison on low-velocity impact behavior between graphite/epoxy composite laminate and steel plate. In order to validate the proposed scheme fur the impact behavior of the plate, the Karas's impact model was used. The impact models for this comparative study are the graphite/epoxy composite plate having $[0/90/45/-45/-45/45/90/0]_{8S}$ laminate sequence and the steel plate with a steel ball impactor. The low-velocity impact behaviors for two types of plates were comparatively investigated and performed by considering different impactor velocities and weights respectively. In this investigation, it was found that the composite laminate has impact energy absorption effect due to more flexible behavior than the steel plate, and also it has better characteristics on impact damage and weight.

• Proceedings of the Acoustical Society of Korea Conference
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• autumn
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• pp.307-310
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• 2000

평판에서 발생되는 램파가 물체 내에 존재할 수 있는 미세 결함과의 상호작용에 의해 비선형 음향효과를 발생시키는지 관찰하고 이로부터 결함의 존재 유$\cdot$무를 확인하고자 했다. 이차원의 판형 매질로서 $2000{\times}110{\times}2{\cal}mm^3$인 강철판을 사용했으며 결함은 강철판의 임의의 위치에 인위적으로 미세틈새를 형성하여 모델화시켰다. 488kHz의 저주파수 연속파와 톤버스트 형태의 1MHz 고주파수 음파를 입사시켰다. 결함의 유$\cdot$무에 따른 강철판에서의 수신음파에 대한 주파수 응답을 통하여 비선형 음향반응인 배진동 주파수와 합$\cdot$차 주파수의 발생을 관측함으로써 매질 내의 결함 유$\cdot$무를 판별하고자 했다. 결함이 존재할 경우, 존재하지 않을 경우와 비교했을 때 배진동 주파수는 진폭이 15dB, 합$\cdot$차주파수는 진폭이 18dB이상 증가됨을 관찰함으로써 평판에서의 결함의 존재 유$\cdot$무를 확인할 수 있었다.

• Nuclear Engineering and Technology
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• v.25 no.4
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• pp.529-538
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• 1993

A stochastic way using continuous time Markov process is presented to model the one-dimensional nuclide transport in fractured rock matrix as an extended study for previous work ［1］. A nuclide migration model by the continuous time Markov process for single planar fractured rock matrix, which is considered as a transient system where a process by which the nuclide is diffused into the rock matrix from the fracture may be no more time homogeneous, is compared with a conventional deterministic analytical solution. The primary desired quantities from a stochastic model are the expected values and variance of the state variables as a function of time. The time-dependent probability distributions of nuclides are presented for each discretized compartment of the medium given intensities of transition. Since this model is discrete in medium space, parameters which affect nuclide transport could be easily incorporated for such heterogeneous media as the fractured rock matrix and the layered porous media. Even though the model developed in this study was shown to be sensitive to the number of discretized compartment showing numerical dispersion as the number of compartments are decreased, with small compensating of dispersion coefficient, the model agrees well to analytical solution.