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http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/34033完整後設資料紀錄
| DC 欄位 | 值 | 語言 |
|---|---|---|
| dc.contributor.advisor | 陳國在(Kuo- Tzay Chen) | |
| dc.contributor.author | Wei-Han Huang | en |
| dc.contributor.author | 黃韋翰 | zh_TW |
| dc.date.accessioned | 2021-06-13T05:52:11Z | - |
| dc.date.available | 2007-07-11 | |
| dc.date.copyright | 2006-07-11 | |
| dc.date.issued | 2006 | |
| dc.date.submitted | 2006-07-04 | |
| dc.identifier.citation | 【1】Philip M. Morse,Richard H. Bolt,and Richard L.Brown “Acoustic Impedance and Sound Absorption”,J. Acoust. Soc. Am.Vol.12,No.2,pp.217-227,(1940).
【2】Leo L.Beranek,”Acoustic Impedance of Porous Materials”, J.Acoust.Soc.Am. Vol.13,No.3,pp.248-260,(1942). 【3】Bolt, R. H.,“On the design of perforated facings for acoustic materials”,J.Acoust.Soc.Am,Vol.19,No.5, 917-921.(1947). 【4】 Ingard,K.U.,Bolt,R.H.,“Absorption Characteristics of Acoustic Material with Perforated Facings”,J. Acoust. Soc.Am.,Vol.23,No.5,pp.533-540,(1951) 【5】Callaway,D.B.,Ramer,L.G.,“The use of perforated facings in designing low frequency resonant absorbers,”J. Acoust. Soc.Am.,Vol.24,No.3, pp. 309-312.(1952) 【6】Ingard,K.U.,“Perforated facing and sound absorption”, J. Acoust.Soc.Am, Vol.26, No.2, pp. 151-154.(1954) 【7】M.A.Delany and E.N.Bazley,“Acoustic properties of fibrous absorbent materials”,Appl. Acoust. 3,pp.105-116, (1970). 【8】Davern,W.A.,“Perforated facings backed with porous materials as sound absorbers-an experimental study”, Applied Acoustics, England,Vol.10,pp.85-112.(1977). 【9】 Maa,D.Y ,“Microperforated panel wide – band absorber”, Noise Control Eng.J,Vol29,pp.77–84,(1987). 【10】 Maa,D.Y,“Potential of microperforated panel absorber”, J. Acoust. Soc. Am. 104 (5),pp.2861-2866,(1998). 【11】佟峻桓,多孔纖維材質吸音特性之分析研究,台大造船所碩士論文,(1999) 【12】 Song, B.H. and Bolton, J.S.“A Transfer-Matrix Approach For Estimating the Characteristic Impedance and Wave Numbers of Limp and Rigid Porous Materials, J. Acoust. Soc. Am., 107 (3), pp.1131-1152,(2000) 【13】 Seybert,A.F.,and Ross, D. F.,Experimental Determination of Acoustic Properties Using a Two-Microphone Random Excitation Technique, J. Acoust. Soc. Am., Vol.61,NO.5, pp.1362-1370(1977). 【14】 Tao, Z.; Herrin, D. W.; Seybert, A. F.,“Measuring Bulk Properties of Sound-Absorbing Materials Using the Two-Source Method,”Society of Automotive Engineers, Inc,(2003) 【15】 F. C. Lee and W. H. Chen,“Acoustic transmission analysis of multi-layer absorbers,”Journal of Sound and Vibration pp. 248,(2001) 【16】 Utsuno, H., Tanaka, T., Fujikawa, T. and Seybert, A.F., “Transfer Function Method for Measuring Characteristic Impedance and Propagation Constant of Porous Materials,” J. Acoust. Soc. Am, 86 (2), pp.637-643 (1989) 【17】 Kang, J., Fuchs, H.V., “Predicting the absorption of open weave textiles and micro-perforated membranes backed by an air space”, J. of Sound and Vibration, 220, (5), 905-920,(1999) 【18】Bolt, R. H., “On the design of perforated facings for acoustic materials”, J. Acoust. Soc. Am, Vol.19, No.5, 917-921.(1947). 【19】Beranek, L.L. and Vér, I.L., Noise and Vibration Control Engineering, John Wiley & Sons, Inc., 214-219 (1992). 【20】阻抗管法吸音率測定法, CNS 13208 【21】(ASTM) E1050-90, “Standard test method for impedance and absorption of acoustical materials using a tube, two microphones, and a digital frequency analysis method',Revised 1990. 【22 】吳明翰, 穿孔鋼板吸音特性之研究, 成大建築所碩士論文,(2003) | |
| dc.identifier.uri | http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/34033 | - |
| dc.description.abstract | 本文目的在探討改變穿孔直徑、穿孔率、背後空氣層厚度以及背貼材料厚度和不同材料的流動阻率時,微穿孔板以及穿孔板背貼多孔性吸音材料之吸音效果。為了分析此兩種吸音結構的吸音理論,結合聲波在不同介質的傳輸矩陣,得到材料表面阻抗及吸音率的計算公式,並在阻抗管中進行實驗,結果理論計算和實驗结果符合良好,最後再從理論上,改變上述結構參數,以計算其對吸音率的影響。
本研究所得之結論有以下幾點: 一、 對微穿孔板設計而言,針對低頻及吸收頻寬,孔徑0.4mm、穿孔 率1%、板厚1mm以及較大的空氣層厚度會有較佳的吸音率。 二、雙層比單層微穿孔板結構在低頻吸音效果更好且吸收頻寬更大。 三、對於穿孔板背貼多孔性吸音材料,因為多孔性吸音材料在高頻的 吸音率較好,所以適當地調整孔徑、穿孔率等結構參數,可使吸音結構在高低頻皆能有理想的吸音率。 四、背貼吸音材時,穿孔板的穿孔率要大於20%以上時,吸音才有一 定效果。 五、微穿孔板的聲學特性是由板本身的結構參數所決定;穿孔板孔徑 較大且當穿孔率大於20%,聲學特性主要由空腔内的吸音材料决定。 | zh_TW |
| dc.description.abstract | This study is mainly to discuss the sound absorption effects of mirco-perforated panels and perforated panels backing with porous materials when changing the diameters of the apertures,the perforation,the thickness of air layers,the thickness of backing materials and the flow resistivities of different materials.In order to analyze these two absorptive structures,assocating the transfer matrices of sound wave in different media,and we can get the formulas of surface impedances and sound absorption coefficients,and then we do experiments in the impenance tubes.It shows that the theory and the experiment result can match well. Finally, we change parameters of the sound absorptive structers and calculating the influence of the sound absorption coefficients from the theory.
There are some conclusions as follow: 1.For designing mirco-perforated panels,the diameter is 0.4mm,the perforation is 1%,the panel thickness is 1mm,and the larger air layer will get advance in sound absorption coefficients in low frequency and sound absorption bandwidth. 2.The double layer of the mirco-perforated panels will have better sound absorption effects and can broaden the frequency range of sound absorption. 3.For perforated panels backing with porous materials,because the porous materials have higher sound absorption coefficient in high frequency,we can adjust the structure parameter,ex: the diameters of the apertures,the perforation...etc,that can make structures have ideal sound absorption effects in both low and high frequency. 4.The perforation must be over 20%, and then the sound absorption have some level effect when perforated panels backing with porous materials. 5.The acoustic characteristic of the mirco-perforated panels is decided by the structure parameters of panels themselves,and when the diameters of the apertures are larger and over 20%, the acoustic characteristic is decided by the absorptive materials in air layer. | en |
| dc.description.provenance | Made available in DSpace on 2021-06-13T05:52:11Z (GMT). No. of bitstreams: 1 ntu-95-R92525022-1.pdf: 882639 bytes, checksum: 75119c2eb3345a0040e1eec58fe96e56 (MD5) Previous issue date: 2006 | en |
| dc.description.tableofcontents | 誌謝(Ⅰ)
中文摘要(Ⅱ) Abstract(Ⅲ) 目錄(Ⅵ) 圖目錄(Ⅸ) 表目錄(ⅩⅢ) 第一章 緒論(1) 1.1 前言(1) 1.2 研究目的(2) 1.3 研究方法(2) 1.4 文獻回顧(3) 第二章 理 論 分 析(4) 2.1 流體運動方程式(4) 2.2 穿孔板吸音原理(8) 2.3 多孔吸音材吸音原理(12) 2.3.1 多孔吸音材理論(14) 2.3.2 多孔性吸音材的特徵阻抗和波數(15) 第三章 聲波在不同介質中的傳播(18) 3.1 傳輸矩陣法的理論(18) 3.2 微穿孔板傳輸阻抗的量測(20) 3.3 傳輸矩陣法應用在多層吸音材料(22) 3.3.1 單一材料(25) 3.3.2 組合材料(27) 第四章 實驗方法與過程(35) 4.1 吸音率之定義(35) 4.2 垂向聲學特性之求得(36) 4.3 轉移函數法求吸音材料反射係數(39) 4.4 儀器配置(42) 第五章 實驗與計算結果(44) 5.1 理論值和實驗值之比較(44) 5.2 改變參數對微穿孔板的影響(48) 5.3 改變參數對穿孔板背貼多孔性吸音材的影響(60) 5.4 小結(74) 第六章 結論與未來展望 (75) 6.1結論(75) 6.2未來展望(77) 參考文獻(78) | |
| dc.language.iso | zh-TW | |
| dc.subject | 吸音率 | zh_TW |
| dc.subject | 阻抗管 | zh_TW |
| dc.subject | 傳輸矩陣 | zh_TW |
| dc.subject | 微穿孔板 | zh_TW |
| dc.subject | impenance tubes | en |
| dc.subject | transfer matrix | en |
| dc.subject | mirco-perforated panels | en |
| dc.subject | sound absorption coefficients | en |
| dc.title | 傳輸矩陣法在微穿孔板以及穿孔板背貼多孔性吸音材之吸音特性應用 | zh_TW |
| dc.title | The Application of Transfer-Matrix Method on The Absorption of Micro-Perforated Panels and Perforated Panels Backing with Porous Materials | en |
| dc.type | Thesis | |
| dc.date.schoolyear | 94-2 | |
| dc.description.degree | 碩士 | |
| dc.contributor.oralexamcommittee | 陳永祥(Yung - Hsiang Chen),劉雲輝 | |
| dc.subject.keyword | 微穿孔板,傳輸矩陣,吸音率,阻抗管, | zh_TW |
| dc.subject.keyword | mirco-perforated panels,transfer matrix,sound absorption coefficients,impenance tubes, | en |
| dc.relation.page | 81 | |
| dc.rights.note | 有償授權 | |
| dc.date.accepted | 2006-07-05 | |
| dc.contributor.author-college | 工學院 | zh_TW |
| dc.contributor.author-dept | 工程科學及海洋工程學研究所 | zh_TW |
| 顯示於系所單位: | 工程科學及海洋工程學系 | |
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