• 한국항해항만학회지
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• 제27권4호
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• pp.455-463
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• 2003

저질의 부유 현상이 일련의 쇄파라고 하는 파동 현상에 어떠한 형태로 연동하는가를 면밀히 조사하기 위하여 현지해안의 쇄파대내에 주 관측지점을 설치하고 부유사 농도와 유속, 수위변동 등의 관련 파랑 제원을 계측하였다. 분석을 위해 수위변동, 유속변동치의 부유사 농도에 대한 상관관계를 조사하였으며, 상관이 탁월한 주기대에 대한 ensemble 평균 분석으로 유속 및 수위변동의 위상에 따른 부유사 농도의 변화와의 관계를 명백히 하여 다음의 결론을 얻었다. 1) 부유사의 농도 변동은 유속 및 수위변동의 에너지가 가장 큰 장주기 성분(100s)에 있어서 보다 오히려, 관측지점이 절(node)이 되는 1차mode의 장주기중복파(60s) 및 배(anti-node)가 되는 2차 mode의 중복파(30s)의 주기성분에서 상관이 높았으며, 2)또한, 1차 mode의 장주기중복파의 유속 성분이 해안으로 향하여 가속하는 위상 즉, 수면 경사가 상대적으로 해안선측보다 외해측이 높은 위상에서 부유사 농도가 가장 높아짐을 명백히 하였다.

• 한국지구물리탐사학회:학술대회논문집
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• 한국지구물리탐사학회 2005년도 공동학술대회 논문집
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• pp.287-291
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• 2005

P파 및 SH파 굴절법 토모그래피와 표면파 분산자료 역산을 통하여 2차원 P파와 S파 속도단면을 얻었다. 두 방법으로 구한 S파 속도단면을 비교한 결과, 두 단면의 전체적인 양상은 서로 비슷하지만, 표면파 역산으로 구한 S파 속도단면이 전반적으로 작은값을 갖는다. SH파는 잡음에 매우 취약하고, P파와 PS 전환파의 도달 이후에 기록되어 초동선택이 어려운 문제가 있으며, 표면파의 분산곡선 역산은 균질한 수평지구모델을 가정하므로, 수평적 변화 심한 곳에서는 정확한 지하구조를 밝히는데 한계가 있음을 확인할 수 있었다.

• Smart Structures and Systems
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• 제18권2호
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• pp.335-354
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• 2016

This contribution presents an extended one-dimensional theory for piezoelectric beam-type structures with non-ideal electrodes. For these types of electrodes the equipotential area condition is not satisfied. The main motivation of our research is originated from passive vibration control: when an elastic structure is covered by several piezoelectric patches that are linked via resistances and inductances, vibrational energy is efficiently dissipated if the electric network is properly designed. Assuming infinitely small piezoelectric patches that are connected by an infinite number of electrical, in particular resistive and inductive elements, one obtains the Telegrapher's equation for the voltage across the piezoelectric transducer. Embedding this outcome into the framework of Bernoulli-Euler, the final equations are coupled to the wave equations for the longitudinal motion of a bar and to the partial differential equations for the lateral motion of the beam. We present results for the wave propagation of a longitudinal bar for several types of electrode properties. The frequency spectra are computed (phase angle, wave number, wave speed), which point out the effect of resistive and inductive electrodes on wave characteristics. Our results show that electrical damping due to the resistivity of the electrodes is different from internal (=strain velocity dependent) or external (=velocity dependent) mechanical damping. Finally, results are presented, when the structure is excited by a harmonic single force, yielding that resistive-inductive electrodes are suitable candidates for passive vibration control that might be of great interest for practical applications in the future.

• 한국세라믹학회지
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• 제40권4호
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• pp.393-397
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• 2003

To investigate the effect of AIN c-axis orientation on the resonance performance of film bulk acoustic wave resonators, solidly mounted resonators with crybtallographically different AIN piezoelectric films were prepared by changing only the bottom electrode surface conditions. As increasing the degree of c-axis texturing, the effective electromechanical coupling coefficient ($\kappa$$\_$eff/)$^2$ in resonators increased gradually. The least 4 degree of full width at half maximum in an AIN(002) rocking curve, which corresponds to $\kappa$$^2$$\_$eff/ of above 5%, was measured to be necessary for band pass filter applications in wireless communication system. The longitudinal acoustic wave velocity of AIN films varied with the degree of c-axis texturing. The velocity of highly c-axis textured AIN film was extracted to be about 10200 n/s by mathematical analysis using Matlab.

• Journal of Advanced Marine Engineering and Technology
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• 제33권6호
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• pp.965-974
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• 2009

The current study reviews the formula used to calculate the stability of an artificial reef in the breaking wave zone of coastal waters. A comparison was carried out between the existing formula and a new formula that takes into account the water particle velocity in the breaking wave zone. Water particle velocity was analyzed using the Fluent (CADMAS-SURF) software program. The new formula took into various factors, including the difference in the drag coefficient due to the direction of the current and the ratio of distance between two reefs. The drag coefficient of the artificial reef due to the direction of the current was 0.84 when the distance ratio was 0.5. When the artificial reef was placed at 45 degree angle to the current, the product of the drag coefficient and the project area were 40 to 46 % greater than when the reef was placed at 90 degree angle. Our results regarding the stability of an artificial reef indicate that the new formula provides the designers of artificial reefs with a more rational and economic design rationale rather than the existing formula.

• 비파괴검사학회지
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• 제17권4호
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• pp.227-236
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• 1997

탄성파 전파 과정의 정량적인 이해와 그 가시화는 결함 탐지는 물론이고, 재료의 물성 평가에 매우 중요하다. 대상 재료가 이방성을 지닐 경우에 탄성파 전파 과정은 복잡해져서 전파 과정의 해석 및 가시화 작업은 탄성파를 이용하는 결함 탐지 및 재질 평가에서는 필수적이다. 이방성 재료에서는 탄성파의 속도가 방향에 따라서 달라짐은 물론이고, 위상 속도와 군 속도의 방향이 어긋나서 파면이 진행하는 방향과 에너지가 진행하는 방향이 달라진다(beam skewing 효과). 특히 복합재료와 같이 이방성이 큰 재료에서는 이 효과가 매우 크게 나타나므로 탄성파를 이용한 시험 결과를 해석하고자 할 때에는 반드시 전파 과정을 이해해야 한다. 이방성 재료에 대해 해석적인 접근에는 한계가 있어서 유한차분법(finite difference method: FDM)과 같은 수치 해석 방법이 유용하게 사용되고 있다. 본 연구에서는 탄성파 전파 과정을 해석할 수 있는 2차원 FDM 프로그램을 개발하고, 이를 이용하여 이방성 재료에서의 탄성파 전파에 대한 전산 시뮬레이션 결과를 비교 분석한다.

• 한국지반공학회:학술대회논문집
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• 한국지반공학회 2008년도 춘계 학술발표회 초청강연 및 논문집
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• pp.7-13
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• 2008

To obtain a shear-wave velocity profile in geotechnical practice, various seismic investigation methods which have their own strength and weakness are being frequently used. Generally, geotechnical site have lateral variation of the properties, so it is needed to determine 2-dimensional shear wave velocity imaging of the site. In this study, harmonic wavelet analysis of wave (HWAW) method is applied to determination of 2-D $V_s$ imaging. HWAW method which is based on time-frequency analysis using harmonic wavelet transform have been developed to determine phase and group velocities of waves. HWAW method uses the signal portion of the maximum local signal/noise ratio to evaluate the phase velocity to minimize the effects of noise. HWAW method determine detailed local $V_s$ profile because one experimental setup which consists of one pair of receivers with spacing of 1~3m is used to determine the dispersion curve of the whole depth. So, 2-D Vs imaging with relatively high resolution can be determined through a series of HWAW test. In order to estimate the applicability of HWAW method, field tests were performed in 4 sites. Through field applications and comparison with other test results, the good accuracy and applicability of the proposed method were verified.

• Advances in nano research
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• 제16권2호
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• pp.187-200
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• 2024

This study focuses on wave propagation analysis in the curved nanobeam exposed to different thermal loadings based on the Nonlocal Strain Gradient Theory (NSGT). Mechanical properties of the constitutive materials are assumed to be temperature-dependent and functionally graded. For modeling, the governing equations are derived using Hamilton's principle. Using the proposed model, the effects of small-scale, geometrical, and thermo-mechanical parameters on the dynamic behavior of the curved nanobeam are studied. A small-scale parameter, Z, is taken into account that collectively represents the strain gradient and the nonlocal parameters. When Z<1 or Z>1, the phase velocity decreases/increases, and the stiffness-softening/hardening phenomenon occurs in the curved nanobeam. Accordingly, the phase velocity depends more on the strain gradient parameter rather than the nonlocal parameter. As the arc angle increases, more variations in the phase velocity emerge in small wavenumbers. Furthermore, an increase of ∆T causes a decrease in the phase velocity, mostly in the case of uniform temperature rise rather than heat conduction. For verification, the results are compared with those available for the straight nanobeam in the previous studies. It is believed that the findings will be helpful for different applications of curved nanostructures used in nano-devices.

• 한국세라믹학회지
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• 제32권3호
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• pp.341-348
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• 1995

An analysis of the use of temperature profiles in the determination of the kinetic parameters of combustion synthesis of Ti5Si3 were investigated. From profile analysis, an apparent activation energy of 12KJ/mol was calculated. The Maximum heating rate achieved during 10wt% Ti5Si3 reaction by the product dilution method was approximately $1.5\times$104 K/s. Coupling this value with the measured wave velocity of 7.02 cm/s yields a maximum thermal gradient of 2.14$\times$103 K/cm. The value of tr (=t*) was calculated to be 1.2$\times$10-1 s and the value of td (=tx) was calculated to be 32.89 s. Using the definition of t* and the measured wave velocity, the effective thermal diffusivity, $\alpha$, was calculated to be 0.59$\times$10 $\textrm{cm}^2$/s. From these analysis, the power function, G, was also calculated.

• Advances in aircraft and spacecraft science
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• 제10권3호
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• pp.203-222
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• 2023

The detonation combustion is a supersonic combustion process follows on shock wave oscillations in detonation tube. In this paper numerical studies are carried out combined effect of blockage ratio and spacing of obstacle on detonation wave propagation of hydrogen-air mixture in pulse detonation combustor. The deflagration to detonation transition of stoichiometric (ϕ=1)fuel-air mixture in channel has been analyzed for effect of blockage ratio (BR)=0.39, 0.51, 0.59, 0.71 with spacing of 2D and 3D. The reactive Navier-Stokes equation is used to solve the detonation wave propagation mechanism in Ansys Fluent platform. The result shows that fully developed detonation wave initiation regime is observed near smaller vortex generator ratio of BR=0.39 inside the combustor. The turbulent rate of reaction has also a great significance role for shock wave structure. However, vortices of rapid detonation wave are appears near thin boundary layer of each obstacle. Finally, detonation combustor demonstrates the superiority of pressure gain combustor with turbulent rate of reaction of 0.6 kg mol/m3 -s inside the detonation tube with obstacle spacing of 12 cm, this blockage enhanced the turbulence intensity and propulsive thrust. The successful detonation wave propagation speed is achieved in shortest possible time of 0.031s with a significance magnitude of 2349 m/s, which is higher than Chapman-Jouguet (C-J) velocity of 1848 m/s. Furthermore, stronger propulsive thrust force of 36.82 N is generated in pulse time of 0.031s.