王昭男臺灣大學：工程科學及海洋工程學研究所陳詩凱Chen, Shih-KaiShih-KaiChen2007-11-262018-06-282007-11-262018-06-282005http://ntur.lib.ntu.edu.tw//handle/246246/51042本文探討吸音材料在受到壓縮作用後其吸音能力的改變情形，利用Biot彈性多孔材理論與彈性固體理論分別推導出在空氣中與水中其材料之波動方程，探討當材料受壓縮作用後其各參數之變化情形，考慮材料兩端速度與應力的連續條件，可建立聲波之轉換矩陣，進而求得材料吸音率與回聲衰減量。本文分別就空氣中與水中兩部份探討材料之吸音效能的變化情形。 空氣中的部份探討了多孔材受壓與否之吸音效能比較，亦嘗試以不同角度入射時其吸音能力的變化情形；而當吸音材料受壓縮作用後，整體之吸音曲線會往高頻處平移，其吸音效能比不受壓時略為降低。但若比較相同厚度的多孔材，材料受到壓縮作用會比材料無受壓之情形其吸音效果要佳。水下的部份則模擬材料承受水壓後，吸音效能因材料厚度、聲能損耗性質改變所造成的影響，導致於整體之吸音效能變差。This work studies that the sound is muffled by the acoustic material which is compressed. For yielding the sound wave equation of the material in water or air, Biot theory and the sound propagation of the solid are used. Furthermore, the variation in the acoustic parameters is presented and discussed. By considering the boundary conditions, the continuous velocity and pressure on the both sides of the material, the sound transfer matrix can be build. Than the absorption coefficient and the echo reduction can be calculated. The two parts, the sound absorptions of the material in air and water are researched separately. In the one part, the abilities of sound absorption of the compressed material in air are investigated. The influence of the different incident angles of sound wave are also discussed in the article. As the acoustical material is compressed, the characteristics (peak or tip) of curve of absorption coefficient shift to high frequency. The value of absorption coefficient becomes low. On the other side, as the both thicknesses of the compressed and the un-compressed porous materials are the same, the ability of absorption of compressed material is better than another un-compressed material. In the other part, the work focuses on the acoustic studies in water. As the thickness of the material varies from the pressure of water, the influences on the abilities of sound absorption of the material are simulated. In water, the ability of absorption of material is bad because the pressure of water lead the property of the material to change.第一章　序論 …………………………………... 1 1.1 前言 ……………………………………. 1 1.2 文獻回顧 ………………………………. 2 1.3 研究方法 ………………………………. 4 第二章 理論分析 ……………………………... 6 2.1多孔材吸音原理 ..................... 6 2.2剛性結構與彈性結構 ................. 7 2.3彈性固體之波傳理論 ................. 8 2.3.1 應力與應變之關係 ............ 8 2.3.2 彈性固體之運動方程式 ........ 9 2.3.3 彈性固體之波動方程式 ........ 11 2.4 彈性多孔材之應力應變 .............. 12 2.4.1 彈性多孔材應力應變關係 ...... 12 2.4.2 彈性係數P,Q,R,N ............ 13 2.4.3 流體為空氣時之簡化 .. . . 14 2.5 彈性多孔材料慣性偶合效應 ........... 15 2.5.1 Biot慣性理論 ................ 15 2.5.2慣性耦合項 ................... 17 2.6彈性多孔材料的波傳理論 .................. 18 2.6.1 多孔材料的波動方程式 ........ 18 2.6.2 壓縮波與剪力波 .............. 19 2.7 壓縮多孔材造成各參數之改變 ........ 22 第三章 轉換矩陣與材料之吸音 ................ 27 3.1 各種材料之轉換矩陣 ................ 27 3.1.1 多孔材之轉換矩陣 ............ 27 3.1.2 彈性固體之轉換矩陣 ...... ..........32 3.1.3 流體之轉換矩陣 ............. 35 3.2 交界面之轉換矩陣 .................. 36 3.2.1流體-流體間之轉換矩陣 ........ 36 3.2.2彈性固體-彈性固體間之轉換矩陣 . 37 3.2.3多孔材-多孔材間之轉換矩陣 .... 37 3.2.4流體-彈性固體間之轉換矩陣 .... 39 3.2.5流體-多孔材間之轉換矩陣 ...... 39 3.2.6彈性固體-多孔材間之轉換矩陣 .. 40 3.3轉換矩陣求解及材料之吸音率 ......... 41 第四章 空氣中壓縮作用對吸音率之影響 ........ 44 4.1 理論驗證 .................... 44 4.1.1表面阻抗比較 ................. 44 4.1.2 吸音率比較 .................. 48 4.1.3 壓縮後其吸音率之比較 ........ 51 4.2 材料參數之選取 ................ 55 4.3各材料不受壓之吸音特性 ............ 56 4.3.1 各材料在正向入射時不同厚度之情況 . 56 4.3.2 各材料斜向入射之情況 ........ 61 4.4各材料受壓縮作用後之吸音特性 ....... 63 4.4.1 各材料在正向入射時之情況 .... 63 4.4.2 各材料在斜向入射時之情況 .... 69 第五章 水下吸音效能探討 ............ 74 5.1 水下吸音材料之選取 ................ 74 5.1.1 一般橡膠 ................. 74 5.1.2 Rho-C 橡膠 ................. 76 5.2吸音材料之參數探討 ................. 78 5.2.1 吸音材料之參數探討 .......... 78 5.2.2 實驗驗證 ............... 83 5.3 模擬潛艦之吸音效能分析 ............ 84 5.3.1 不考慮水壓影響下之吸音效能探討 . 84 5.3.2 在水壓影響下其吸音效能探討 .. 89 第六章 結論與展望 ................. 95 6.1 結論 ....................... 95 6.2 未來展望 .......................... 97 參考文獻 ................................... 981202070 bytesapplication/pdfen-US吸音材壓縮acoustic materialcompressionthesishttp://ntur.lib.ntu.edu.tw/bitstream/246246/51042/1/ntu-94-R92525034-1.pdf