• Title/Summary/Keyword: Absorbing materials

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A Study on the Improvement of Acoustic Absorption of Multiple Layer Perforated Panel Systems (다중 다공판 시스템의 흡음성능 향상에 관한 연구)

  • Lee, Dong-Hoon;Seo, Seong-Won;Hong, Byung-Kuk;Song, Hwa-Young
    • Transactions of the Korean Society for Noise and Vibration Engineering
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    • v.15 no.5 s.98
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    • pp.571-577
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    • 2005
  • The acoustic absorption of multiple layer perforated panel systems is largely reduced at the anti-resonance frequency. In order to improve the acoustic absorption at the anti-resonance frequency, the sound absorbing materials are inserted between perforated panels. By the insertion of absorbing materials, it is found that the multiple layer perforated panel system has better acoustic absorption at the anti-resonance frequency and more broadband frequency. Besides, it is shown that the absorption coefficients from the transfer matrix method agree well with the values measured by the two-microphone impedance tube method for various combinations of perforated panels, airspaces or sound absorbing materials.

An Experimental Study on the Absorption Performance of Steel-Wire Sound Absorbing Materials (금속와이어 흡음재의 흡음성능에 관한 실험적 연구)

  • 서성원;용호택;이동훈
    • Korean Journal of Air-Conditioning and Refrigeration Engineering
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    • v.15 no.5
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    • pp.413-421
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    • 2003
  • The acoustic performances of steel-wire sound absorbing materials with different thicknesses and bulk densities were investigated experimentally. The well-known two-cavity method was used to measure the characteristic impedance, propagation constant and absorption coefficient. The normal absorption coefficients measured by two-cavity method agreed well with those by the two-microphone impedance tube method. The experimental results showed that the magnitude of the absorption coefficient and the frequency range of the maximum absorption coefficient were controllable by changing the thickness and bulk density of the steel-wire. Therefore, the steel-wires obtained from the crushed tire chips could be used as a good absorbing material.

A Study on an Analysis of Noise Reduction Effects using the tentatively Installed Sound-absorbing Materials in Metro Tunnel (도시철도 터널내 흡음재 시험설치 및 소음저감효과 분석에 관한 연구)

  • Hong, Chul-Kee;Jeong, Ri-Taek;Kim, Byeong-Hong
    • Proceedings of the KSR Conference
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    • 2008.11b
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    • pp.125-131
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    • 2008
  • This research tries to analyze and investigate the effects of the noise reduction test for the sound-absorbing materials installed tentatively on Metro Line 5. Though the noise reduction effects of each sound-absorbing material showed that there was about $2{\sim}5\;dB$ compared with before and after of the tentative installation, it shows that the noise reduction effects are reducing because of the section change condition such as dust absorption and the rail abrasion as time passes after the tentative installation. Also, many difficulties are occurring in the maintenance of the orbit facilities because of the installation of sound-absorbing materials. Though various abroad products for noise reduction are imported like this, the researches for the noise reduction effect increase for this and the improvement direction are being required because of the poor circumstance of the efficiency aspect compared to the economic investment effect because those are not suited to the character of domestic Metro.

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Numerical Analysis and Verification of Sound Absorbing Properties of Perforated Plate (타공판의 등가 흡음 물성치 유도와 공명기로서의 흡음성능 해석)

  • Yoon, Gil-Ho;Kim, Ki-Hyun;Choi, Jung-Sik;Yun, Su-Hwan
    • Journal of the Computational Structural Engineering Institute of Korea
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    • v.28 no.2
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    • pp.139-144
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    • 2015
  • Recently, to realize sound-absorbing structures, we have to insert sound-absorbing materials into wall. These shapes are taken limitations because sound-absorbing materials should be fixed. Therefore, the sound absorption is changed by environment that used the sound-absorbing materials. On the other hand, we will take same effect without sound-absorbing material, if we change the shape of wall to sound absorbing structure. If we use this sound absorbing structure, we can get benefits by removing limitation of materials. Therefore we suggest perforated plate for effective sound-absorbing structure. We confirmed the function of sound-absorption of this structure using equivalent property. Then, we found the similarity between perforated plate and resonator. Also, we verify these theories through computer simulation by FEM(Finite Element Method). Finally, we validated that perforated plate has function of sound absorption without sound-absorbing material. This perforated plate is used for sound-absorbing material of buildings and transportations such as vehicle, train etc. Also, these results could be further used basic tool for design of sound-absorption structure.

Use of Wastepaper for Developing Environment-friendly Shock-absorbing Materials

  • Kim, Chul-Hwan;Song, Dae-Bin;Lee, Young-Min;Kim, Jae-Ok;Kim, Gyeong-Yun;Shin, Tae-Gi;Park, Chong-Yawl
    • Proceedings of the Korea Technical Association of the Pulp and Paper Industry Conference
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    • 2006.06b
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    • pp.471-474
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    • 2006
  • Environment-friendly shock-absorbing materials were made of wastepaper such as old corrugated containers (OCC) and old newspapers (ONP) with a vacuum forming method. The plate-like cushioning materials made of OCC and ONP respectively by vacuum forming showed superior shock-absorbing properties with lower elastic moduli compared to expanded polystyrene (EPS) and pulp mold. Even though the plate-like materials had many free voids in their fiber structure, their apparent densities (${\approx}0.1g/cm^{3}$) were a little higher than that of EPS (${\approx}0.03g/cm^{3}$) and much lower than that of pulp mold (${\approx}0.3g/cm^{3}$). However, the elastic moduli of the cushioning materials made of wastepaper were much lower than that of EPS or pulp mold. This finding implies that the cushioning materials made of OCC fibers containing more lignin than ONP show better shock-absorbing properties than ONP Moreover, the cushioning materials made of OCC and ONP respectively showed greater porosity than pulp mold. The addition of cationic starch to the cushioning materials contributed to an increase in the elastic modulus to the same level as that of EPS. Furthermore, the deterioration in fiber quality by repeated use of wastepaper played a great role in improving shock-absorbing ability.

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A Study on Radar Absorbing Structure for Aircraft (항공기용 전파흡수 구조 연구)

  • Han, Won-Jae;Jang, Byung-Wook;Park, Jung-Sun
    • Journal of Aerospace System Engineering
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    • v.4 no.3
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    • pp.24-28
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    • 2010
  • The purpose of this study is to define available microwave absorbing structure for aircraft from in the X-band(8.2~12.4GHz) frequencies. The electromagnetic wave absorption or shielding techniques is an important issue not only for military purpose but also for commercial purposes. Aircraft Radar Absorbing Structure(RAS) is absorbed or scattered propagation waves from the enemy radar. There are absorbing technologies at shaping design techniques and using Radar Absorbing Materials(RAM). RAM is more important because shaping design can't include perfect radar absorbing performance. In this study, based on material properties was introduced RAM and to analyze the each characteristics. Finally, we comparison appropriate RAM for aircraft.

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Investigation on the Utilization Possibility of Vitrified Slag for Sound Absorbing Material (용융고화슬래그를 이용한 흡음재료 활용가능성 검토)

  • Kim, Seong-Jung;Rie, Dong-Ho;Park, Hyun-Seo
    • Journal of the Korea Organic Resources Recycling Association
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    • v.8 no.3
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    • pp.97-103
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    • 2000
  • This study was performed to prove that vitrified slag can be utilized as sound absorbing materials by investigating on heavy metal elution and the properties of sound absorbing rate according to the thickness. The heavy metal elution experiment indicated that heavy metal was not eluted since it was fixed stable in the slag. Vitrified slag generally exhibited a maximum sound absorbing rate around at 600Hz-1kHz and 3kHz in the low and high frequency range, respectively. On the other hand, the absorbing rate increased beyond the range of 7kHz again. The sound absorbing rate varied a little according to the thickness of the material. However, Vitrified slag is likely to the effective as a sound absorbing wall material since it has a sound absorbing rate clover 80% in the low and high frequency region when used as a wall. The results obtained in this study showed that vitrified slag has the recyclable material properties and therefore, highly applicable to sound absorbing materials.

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Change of transmission characteristics of FSSs in hybrid composites due to residual stresses

  • Hwang, In-Han;Chun, Heoung-Jae;Hong, Ik-Pyo;Park, Yong-Bae;Kim, Yoon-Jae
    • Steel and Composite Structures
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    • v.19 no.6
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    • pp.1501-1510
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    • 2015
  • The frequency selective surface (FSS) embedded hybrid composite materials have been developed to provide excellent mechanical and specific electromagnetic properties. Radar absorbing structures (RASs) are an example material that provides both radar absorbing properties and structural characteristics. The absorbing efficiency of an RAS can be improved using selected materials having special absorptive properties and structural characteristics and can be in the form of multi-layers or have a certain stacking sequence. However, residual stresses occur in FSS embedded composite structures after co-curing due to a mismatch between the coefficients of thermal expansion of the FSS and the composite material. In this study, to develop an RAS, the thermal residual stresses of FSS embedded composite structures were analyzed using finite element analysis, considering the effect of stacking sequence of composite laminates with square loop (SL) and double square loop (DSL) FSS patterns. The FSS radar absorbing efficiency was measured in the K-band frequency range of 21.6 GHz. Residual stress leads to a change in the deformation of the FSS pattern. Using these results, the effect of transmission characteristics with respect to the deformation on FSS pattern was analyzed using an FSS Simulator.

Preparation and Characterization of Low Infrared Emissivity Bicomponent Fibers with Radar Absorbing Property (레이더 흡수특성이 있는 저적외선 방출 복합섬유의 제조 및 특성 연구)

  • Yu Bin;Qi Lu
    • Polymer(Korea)
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    • v.30 no.2
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    • pp.124-128
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    • 2006
  • Heavy weight of the camouflage materials was always the main problem. To solve it, the low infrared emissivity fibers with the radar absorbing property (LIFR) were prepared. The low infrared emissivity fibers (LIF) were firstly melt-spun by co-extrusion of polypropylene (PP) and PP/various fillers master-batches using general conjugate spinning. The infrared emissivity of LW with AA and ZnO was decreased respectively compared with that of pure polypropylene fibers. The infrared emissivity of LIF with 15 wt% Al and 2 wt% ZnO in the sheath-part can reach 0.58. To improve LIF radar absorbing property, LIFR was prepared by filling the 50 wt% ferrite and bronze in the core-part of LIF. The radar absorbing efficacy of LIFR was good and the infrared emissivity was low. For the characterization, fiber electron intensity instrument and differential scanning calorimetry (DSC) were used for the analysis of mechanical properties, thermal and crystallization behavior of the spun-fibers. Scanning electron microscopy (SEM) was carried out to observe the particle distribution of the bicomponent fibers.

Noise Barrier Design for Increased Sound Absorption (흡음률 증가를 위한 방음벽 구조)

  • Kim Hyun-Sil;Kim Jae-Seung;Kang Hyun-Joo;Kim Bong-Ki;Kim Sang-Ryul
    • Proceedings of the Acoustical Society of Korea Conference
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    • autumn
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    • pp.367-370
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    • 2001
  • Various shapes of the noise barrier frame and construction of the sound absorbing panels are studied. It is found that insertion of the sound absorbing panel into barrier frame results in the decrease of the sound absorption coefficient, while the empty frame shows a peak around 250Hz. Using double sound absorbing panels with air gap can increase sound absorption coefficient up to NRC 0.85.

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