4 research outputs found

    Application of psectral element method for the vibration analysis of passive constrined layer damping beams

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    ์ˆ˜๋™๊ฐ์‡  ์ ์ธต๋ณด์˜ ์ง„๋™ํ•ด์„์„ ์œ„ํ•œ ์ŠคํŽ™ํŠธ๋Ÿด์š”์†Œ๋ฒ•์˜ ์ ์šฉ์— ๊ด€ํ•œ ์—ฐ๊ตฌํ˜„๋Œ€์ค‘๊ณต์—…(์ฃผ

    Flow Noise Analysis of Hull Appendages Using Lattice Boltzmann Method

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    ์„ ์ฒด ๋ถ€๊ฐ€๋ฌผ์—์„œ ๋ฐœ์ƒํ•˜๋Š” ์œ ๋™์†Œ์Œ์€ ์ž์ฒด์†Œ์Œ ๊ด€์ ์—์„œ ์†Œ๋‚˜์˜ ์„ฑ๋Šฅ๊ณผ ์ง๊ฒฐ๋˜๊ณ , ์ถ”์ง„๊ธฐ ๋ฐ ๋ฐฉํ–ฅํƒ€์™€ ์ƒํ˜ธ์ž‘์šฉ์„ ํ†ตํ•ด 2์ฐจ ์†Œ์Œ์›์„ ์•ผ๊ธฐํ•ด ๊ทผ์ ‘์žฅ ๋ฒ”์œ„์˜ ์—„๋ฐ€ํ•œ ๋ถ„์„์ด ์š”๊ตฌ๋œ๋‹ค. ํ•˜์ง€๋งŒ ์œ ๋™์†Œ์Œ ํ•ด์„์— ์ ์šฉ๋˜๋Š” ๊ธฐ์กด์˜ ์Œํ–ฅ์ƒ์‚ฌ๋ฒ•์€ ์Œํ–ฅ ์‹ ํ˜ธ์˜ ์ „ํŒŒ๋ฅผ ์ง์ ‘ ๋ชจ์‚ฌํ•˜์ง€ ์•Š๋Š” ๊ฐ„์ ‘๋ฒ•์— ํ•ด๋‹นํ•ด ํšŒ์ ˆ, ๋ฐ˜์‚ฌ, ์‚ฐ๋ž€ ํŠน์„ฑ์„ ๊ณ ๋ คํ•  ์ˆ˜ ์—†์œผ๋ฉฐ, ๊ทผ์ ‘์žฅ ํ•ด์„์ด ์ œํ•œ์ ์ด๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ๊ฒฉ์ž ๋ณผ์ธ ๋งŒ ๊ธฐ๋ฒ•์„ ์ ์šฉํ•ด ์ˆ˜์ค‘ํ™˜๊ฒฝ ์œ ๋™์†Œ์Œ์˜ ์ „ํŒŒ๊ณผ์ •์„ ์ง์ ‘ ๋ชจ์‚ฌํ•˜์˜€๋‹ค. ๊ฒฉ์ž ๋ณผ์ธ ๋งŒ ๊ธฐ๋ฒ•์€ ๋ถ„์ž์˜ ์ถฉ๋Œ๊ณผ ํ๋ฆ„ ๊ณผ์ •์„ ํ†ตํ•ด ์œ ๋™์†Œ์Œ์„ ํ•ด์„ํ•˜๋Š” ๊ธฐ๋ฒ•์œผ๋กœ, ์••์ถ•์„ฑ๊ณผ ๋‚ฎ์€ ์†Œ์‚ฐ์œจ, ๋‚ฎ์€ ๋ถ„์‚ฐ์œจ์˜ ํŠน์„ฑ์„ ๊ฐ€์ง€๊ณ  ์žˆ์–ด ์†Œ์Œํ•ด์„์— ์ ํ•ฉํ•˜๋‹ค. ์„ ์ฒด ๋ถ€๊ฐ€๋ฌผ ํ˜•์ƒ์„ ๋Œ€์ƒ์œผ๋กœ RANS ํ•ด์„์„ ํ†ตํ•ด ์œ ๋™์†Œ์Œ์›์„ ๋„์ถœํ•˜๊ณ , ์œ ๋™-์Œํ–ฅ ๊ฒฝ๊ณ„๋ฉด์„ ์ ์šฉํ•œ ๊ฒฉ์ž ๋ณผ์ธ ๋งŒ ๊ธฐ๋ฒ•์œผ๋กœ ์œ ๋™์†Œ์Œ์˜ ์ „ํŒŒ๊ณผ์ •์„ ์ง์ ‘์ ์œผ๋กœ ๋ชจ์‚ฌํ–ˆ๋‹ค. ๋„์ถœ๋œ ๊ฒฐ๊ณผ๋ฅผ ์ˆ˜์Œ์ ์˜ ์œ„์น˜์— ๋”ฐ๋ผ FW-H ๊ฒฐ๊ณผ ๋ฐ ์œ ์ฒด๋™์••๋ ฅ ๊ฒฐ๊ณผ์™€ ๋น„๊ต๋ฅผ ํ†ตํ•ด ๊ทผ์ ‘์žฅ์—์„œ ํƒ€ ๊ธฐ๋ฒ• ๋Œ€๋น„ ๊ฒฉ์ž ๋ณผ์ธ ๋งŒ ๊ธฐ๋ฒ•์˜ ์œ ์šฉ์„ฑ์„ ํ™•์ธํ–ˆ๋‹ค. The flow noise generated by hull appendages is directly related to the performance of the sonar in terms of self-noise and induces a secondary noise source through interaction with the propeller and rudder. Thus, the noise in the near field should be analyzed accurately. However, the acoustic analogy method is an indirect method that is not used to simulate the propagation of an acoustic signal directly; therefore, diffraction, reflection, and scattering characteristics cannot be considered, and near-field analysis is limited. In this study, the propagation process of flow noise in water was directly simulated by using the lattice Boltzmann method. The lattice Boltzmann method could be used to analyze flow noise by simulating the collision and streaming processes of molecules, and it is suitable for noise analysis because of its compressibility, low dissipation rate, and low dispersion rate characteristics. The flow noise source was derived using Reynolds-averaged Navier-Stokes equations for the hull appendages, and the propagation process of the flow noise was directly simulated using the lattice Boltzmann method by applying the developed flow-acoustic boundary conditions. The derived results were compared with Ffowcs Williams-Hawkings results and hydrodynamic pressure results based on the receiver location to verify the usefulness of the lattice Boltzmann method within the near-field range in comparison with other techniques.N

    A Study on Vortex-Induced Vibration Characteristics of Hydrofoils considering High-order Modes

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    ์„ ๋ฐ•, ์ž ์ˆ˜ํ•จ์ด ์ถ”์ง„ํ•˜๋ฉด ์ˆ˜์ค‘๊ตฌ์กฐ๋ฌผ ํ›„๋ฅ˜์— ์™€๋ฅ˜๊ฐ€ ๋ฐœ์ƒํ•˜๊ณ  ์ด์— ๋”ฐ๋ฅธ ์™€๋ฅ˜๊ธฐ์ธ ๊ตฌ์กฐ์ง„๋™์ด ์œ ๋ฐœ๋œ๋‹ค. ์ตœ๊ทผ ์„ ๋ฐ•, ์ž ์ˆ˜ํ•จ์˜ ๊ณ ์†ํ™” ๋ฐ ๋Œ€ํ˜•ํ™” ์ถ”์„ธ์— ๋”ฐ๋ผ ๊ณ ์ฐจ๋ชจ๋“œ์—์„œ ์œ ๋ฐœ๋˜๋Š” ์™€๋ฅ˜๊ธฐ์ธ ์ง„๋™ ๋ฐ ํ”ผ๋กœํŒŒ๊ดด์— ๋Œ€ํ•œ ์ค‘์š”์„ฑ์ด ๊ฐ•์กฐ๋˜๊ณ  ์žˆ๋‹ค. ๊ณ ์† ์œ ์†ํ™˜๊ฒฝ์˜ ์™€๋ฅ˜๋Š” ์ €์† ์œ ์†ํ™˜๊ฒฝ ๋Œ€๋น„ ํฐ ์ง„๋™์„ ์œ ๋ฐœํ•˜๋ฏ€๋กœ ์ด์— ๊ด€ํ•œ ์—ฐ๊ตฌ๊ฐ€ ํ•„์š”ํ•˜๋‹ค. ๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์ˆ˜์ค‘๋‚ ๊ฐœ ๊ณ ์ฐจ๋ชจ๋“œ์—์„œ ์œ ๋ฐœ๋˜๋Š” ์™€๋ฅ˜๊ธฐ์ธ ์ง„๋™์„ ์˜ˆ์ธกํ•˜๊ธฐ ์œ„ํ•œ ํ•˜์ด๋ธŒ๋ฆฌ๋“œ ์œ ์ฒด๊ตฌ์กฐ์—ฐ์„ฑ ํ•ด์„ ๋ฐฉ๋ฒ•๋ก ์„ ์ œ์‹œํ•˜์˜€๋‹ค. ๊ณ ์ฐจ๋ชจ๋“œ๋ฅผ ๊ณ ๋ คํ•œ ํ•˜์ด๋ธŒ๋ฆฌ๋“œ ์œ ์ฒด๊ตฌ์กฐ์—ฐ์„ฑ ํ•ด์„์„ ์ˆ˜ํ–‰ํ•˜์—ฌ ์™€๋ฅ˜๊ธฐ์ธ ์ง„๋™์„ ๋„์ถœํ•˜๊ณ  ์‹คํ—˜๊ฒฐ๊ณผ์™€ ๋น„๊ตํ•จ์œผ๋กœ์จ ๋ฐฉ๋ฒ•๋ก ์„ ๊ฒ€์ฆํ•˜์˜€๋‹ค. ์ตœ์ข…์ ์œผ๋กœ ์™€๋ฅ˜๊ธฐ์ธ ์ง„๋™์œผ๋กœ๋ถ€ํ„ฐ ๋„์ถœ๋œ ์ตœ๋Œ€ von Mises ์‘๋ ฅ์„ ๋…ธ๋ฅด์›จ์ด ์„ ๊ธ‰์—์„œ ์ œ์‹œํ•œ S-N ์„ ๋„์— ์ ์šฉํ•จ์œผ๋กœ์จ ๊ณ ์ฐจ๋ชจ๋“œ ์œ ์ฒด๊ตฌ์กฐ์—ฐ์„ฑ ํ•ด์„์˜ ํšจ์šฉ์„ฑ์„ ํ™•์ธํ•˜์˜€๋‹ค. ๊ณ ์ฐจ๋ชจ๋“œ๋ฅผ ๊ณ ๋ คํ•˜์—ฌ ์™€๋ฅ˜๊ธฐ์ธ ์ง„๋™์‘๋‹ต์„ ๋„์ถœํ•  ๊ฒฝ์šฐ ์œ ์ฒด๊ตฌ์กฐ์—ฐ์„ฑ์— ์˜ํ•œ ๋ฝ์ธ(Lock-in) ํŠน์„ฑ์„ ํ™•์ธํ•˜์˜€์œผ๋ฉฐ ๊ณ ๋ คํ•˜์ง€ ์•Š์€ ๊ฒฝ์šฐ ๋Œ€๋น„ ์ง„๋™์‘๋‹ต๊ณผ ์ตœ๋Œ€ von Mises ์‘๋ ฅ์—์„œ 10๋ฐฐ ์ด์ƒ์˜ ์ฐจ์ด๋ฅผ ๋ณด์˜€๋‹ค. ํ–ฅํ›„์—๋Š” ์™ธํŒ”๋ณด ๊ฒฝ๊ณ„์กฐ๊ฑด ๋ฐ ํ˜•์ƒ์— ๋Œ€ํ•œ ํ™•์žฅ์—ฐ๊ตฌ๊ฐ€ ํ•„์š”ํ•˜๋‹ค.N

    Noise Attenuation Characteristics of Resonator Arrangement Considering the Flow

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    The characteristics of the periodic arrangement of resonators is found to be capable of controlling reflection and transmission as a band gap phenomenon owing to the unusual sound wave caused by the periodic arrangement. In this study, the periodic arrangement of resonators was designed to analyze the noise attenuation in the frequency range of the band gap. Experiments were performed to verify the acoustic characteristics of the resonator arrangement considering the flow. CFD simulations considering the flow were performed to obtain the sound pressure level and pressure distribution, and flow analysis was performed on the designed resonator model using an unsteady compressible Navier-stokes equation. The analysis results of the periodic arrangement of the resonator were verified by comparison with the experimental results of the designed model.N
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