• Title/Summary/Keyword: Wave-Trapping

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A Study on Particle Displacement Distributions of Energy-trapped Piezoelectric Resonators and Filters Utilizing the Harmonic Modes (고차진동을 이용하는 에너지포획형 압전 공진자와 필터의 변위분포에 관한 연구)

  • 이개명
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.11 no.11
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    • pp.954-962
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    • 1998
  • Energy-trapped thickness vibrations of piezoelectric substrates are utilized in fabricating resonators and filters which have their operating frequencies in HF band. Normalized particle displacement distributions of the fundamental thickness shear vibration mode and overtone modes into the thickness direction in energy-trapped resonators and double-coupled filters were obtained by solving the wave equation and calculating the solved equations. These results show that as the number order of the harmonic mode in a energy-trapped resonator becomes larger, the degree of energy-trapping in the resonator increase, and if the conditions for energy-trapping become sufficiently weak, the energy-trapping effect of the harmonic mode which has the lower order disappears the earlier. Above simulation results were proved by the experiments.

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Study on the One-Strip Electrode Ceramic Filter Using the Energy Trapping Effect (에너지트랩 효과를 이용한 단일전극 세라믹 필터에 관한 연구)

  • 송준태;정인영
    • The Transactions of the Korean Institute of Electrical Engineers
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    • v.40 no.1
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    • pp.73-81
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    • 1991
  • In order to simulate the ceramic filter in the state of the one-strip electrode, the theory has been analyzed and a computer program has been developed using the energy trapping effect. The ceramic filters were fabricated using the PZT-4 specimen. The necessary condition that the ceramic filter has the energy trapping effect is that the electroded portion frequency should be smaller than the unelectroded portion frequency when the wave number is zero. Each of the average differences of the resonant point and bandwidth between by the theoretical calculations and by experiment results was 5.6[%] and 3.72[%]. It is considered that the one-strip ceramic filter having a desired characteristics and the lowest difference can be fabricated easily by means of the simulation developed in this paper and the fabrication methods.

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Submerged Porous Plate Wave Absorber

  • PARK W.T.;LEE S.H.;KEE S.T.
    • Journal of Ocean Engineering and Technology
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    • v.19 no.4 s.65
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    • pp.9-14
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    • 2005
  • In the present paper, the wave absorbing performance of the fully submerged horizontal porous plates has been investigated, numerically and experimentally. The submerged porous system is composed of multi-layered horizontal porous plates that are clamped at the vertical setwall, which are slightly inclined and placed vertically, in parallel, with spacing. The hydrodynamic interaction of incident waves with the rigid porous multi-layered plates was formulated within the context of linear wave-body interaction theory and Darcy's law. In order to validate the effectiveness of the present computing code, the numerical results were compared with the analytical and experimental results. It is found that triple horizontal porous plates with slight inclination, if properly tuned for wave energy dissipation against the standing waves in front of the vertical wall, can have high performances in reducing the reflected wave amplitudes against the incident waves over a wide range of wave frequency.

An array effect of wave energy farm buoys

  • Kweon, Hyuck-Min;Lee, Jung-Lyul
    • International Journal of Naval Architecture and Ocean Engineering
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    • v.4 no.4
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    • pp.437-446
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    • 2012
  • An ocean buoy energy farm is considered for Green energy generation and delivery to small towns along the Korean coast. The present study presents that the floating buoy-type energy farm appears to be sufficiently feasible for trapping more energy compared to affixed cylinder duck array. It is also seen from the numerical results that the resonated waves between spaced buoys are further trapped by floating buoy motion.Our numerical study is analyzed by a plane-wave approximation, in which evanescent mode effects are included in a modified mild-slope equation based on the scattering characteristics for a single buoy.

Three-Dimensional Simulation of Seismic Wave Propagation in Elastic Media Using Finite-Difference Method (유한차분법을 이용한 3차원 지진파 전파 모의)

  • 강태섭
    • Proceedings of the Earthquake Engineering Society of Korea Conference
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    • 2000.10a
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    • pp.81-88
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    • 2000
  • The elastic wave equation is solved using the finite-difference method in 3D space to simulate the seismic wave propagation. It is based on the velocity-stress formulation of the equation of motion on a staggered grid. The nonreflecting boundary conditions are used to attenuate the wave field close to the numerical boundary. To satisfy the stress-free conditions at the free-surface boundary, a new formulation combining the zero-stress formalism with the vacuum one is applied. The effective media parameters are employed to satisfy the traction continuity condition across the media interface. With use of the moment-tensor components, the wide range of source mechanism parameters can be specified. The numerical experiments are carried out in order to test the applicability and accuracy of this scheme and to understand the fundamental features of the wave propagation under the generalized elastic media structure. Computational results show that the scheme is sufficiently accurate for modeling wave propagation in 3D elastic media and generates all the possible phases appropriately in under the given heterogeneous velocity structure. Also the characteristics of the ground motion in an sedimentary basin such as the amplification, trapping, and focusing of the elastic wave energy are well represented. These results demonstrate the use of this simulation method will be helpful for modeling the ground motion of seismological and engineering purpose like earthquake hazard assessment, seismic design, city planning, and etc..

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Design of Light Trapping System of Thin Film Solar Cell Using Phase Field Method (페이즈 필드법을 이용한 박막형 태양전지의 광포획층 설계)

  • Heo, Namjoon;Yoo, Jeonghoon
    • Transactions of the Korean Society of Mechanical Engineers A
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    • v.38 no.9
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    • pp.973-978
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    • 2014
  • This study focused on the design of the reflecting layer of a light trapping system fora thin film solar cell using topology optimization based on the phase field method. Therefore, incident light was caused to propagate in the desired direction by reflecting it from this layer, which is the design domain. The same method was applied to the conceptual design of an infrared stealth structure in near infrared range. The results using the phase field method were compared with those using the density method. The design objective was to maximize the Poynting vector value representing the energy flux, which was measured in a measuring domain to control the reflected wave direction. A finite element analysis and optimization process were performed using the commercial package COMSOL combined with the MATLAB programming.

PERISTALTIC PUMPING OF AN ELLIS FLUID IN AN INCLINED ASYMMETRIC CHANNEL

  • A. SMALL;P. NAGARANI;M. NARAHARI
    • Journal of applied mathematics & informatics
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    • v.41 no.1
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    • pp.51-70
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    • 2023
  • The flow of an incompressible Ellis fluid in an inclined asymmetric channel, driven by peristaltic waves was studied under low Reynolds number and long wavelength assumptions. The wave on each side of the channel are assumed to be an infinite train of sinusoidal waves, both having the same constant wave speed and wavelength however, they vary in wave amplitude, channel half width and phase angle. We derived expressions for the axial and transverse velocities, volume flow rate, pressure rise per unit wavelength and streamlines. The effects of varying the wave amplitudes, the phase angle, the channel width, the angle of inclination of the channel as well as the fluid parameters on the flow were analyzed. Trapping conditions were determined and the presence of reflux highlighted using the streamlines for the necessary channel and fluid conditions. By varying the fluid parameters, changes in the fluid that deviated from the Newtonian case resulted in a reduction in the axial velocity in the neighborhood of the center of the channel and a simultaneous increase in the velocity at the periphery of the channel. A nonlinear relation was observed with the pressure rise and the volume flow rate. This nonlinear relation is more pronounced with an increase in the absolute value of the volume flow rate. For Newtonian fluids a linear relation exists between these two variables. The fluid parameters had little effects on the streamlines. However, variations of the wave amplitudes, volume flow, channel width and phase angle had greater effects on the streamlines and hence the trapped region.

Effectiveness of a Wave Resonator under Short-period Waves and Solitary Waves (공진장치를 이용한 단주기파랑과 고립파의 제어)

  • Lee, Kwang Ho;Jeong, Seong Ho;Jeong, Jin Woo;Kim, Do Sam
    • KSCE Journal of Civil and Environmental Engineering Research
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    • v.30 no.1B
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    • pp.89-100
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    • 2010
  • The performance evaluation of a conventional Wave Resonator at the entrance of harbors against solitary wave has been performed using 3D numerical wave flume. A wave resonator has been designed for the attenuation of the transmitted wave energy by trapping the short periodic incident waves only. In this study, however, the controlled performance of the wave resonator by its various widths has been numerically investigated for solitary waves. Source distribution method based on the Green function and the 3D one-field Model for immiscible TWO-Phase flows (TWOPM-3D) using 3D numerical wave flume were used for the short-periodic waves and the solitary waves, respectively, and these models were verified through the comparisons with the previous experimental and numerical results by other researchers. It was confirmed that the wave resonator is effective enough to control the solitary waves as well as the periodic waves when it compares with the case of no resonance system. Further, it was found that there is the optimal width of a wave resonator to attenuate the target solitary waves.

Vibration analysis of characteristics and valveless Type Piezoelectric micro-pump (VALVELSS 압전펌프 진동 해석 및 특성)

  • Lim, Jong-Nam;Oh, Jin-Heon;Lim, Kee-Joe;Kim, Hyun-Hoo
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2009.06a
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    • pp.185-185
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    • 2009
  • Micropump is very useful component in micro/nano fluidics and bioMEMS applications. Using the flexural vibration mode of PZT bar, a piezopump is successfully made. The PZT bar is polarized with thickness direction. The proposed structure for the piezo-pump consists of an input and an output port, piezoelectric ceramic actuator, actuator support, diaphragm. The traveling flexural wave along the bar is obtained by dividing two standing waves which are temporally and spatially phase shifted by 90 degrees from each other. Fluid is drawn into a forming chamber, eventually the forming chamber closes trapping the fluid therein. The finite elements analysis on the proposed pump model is carried out to verify its operation principle and design by the commercial FEM software. Components of piezopump were made, assembled, and tested to validate the concepts of the proposed pump and confirm the simulation results. The performance of the proposed piezopump the highest pressure level of 83.4kHz.

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Design and Characteristics of valveless micro-pump for small liquid delivery (미소유체 밸브리스 압전펌프의 설계 및 특성)

  • Lim, Jong-Nam;Oh, Jin-Heon;Lim, Kee-Joe;Kim, Hyun-Hoo
    • Proceedings of the KIEE Conference
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    • 2009.07a
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    • pp.1275_1276
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    • 2009
  • Micropump is very useful component in micro/nano fluidics and bioMEMS applications. Using the flexural vibration mode of PZT bar, a piezopump is successfully made. The PZT bar is polarized with thickness direction. The proposed structure for the piezo-pump consists of an input and an output port, piezoelectric ceramic actuator, actuator support, diaphragm. The traveling flexural wave along the bar is obtained by dividing two standing waves which are temporally and spatially phase shifted by 90 degrees from each other. Fluid is drawn into a forming chamber, eventually the forming chamber closes trapping the fluid therein.

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