南京大学学报(自然科学版) ›› 2023, Vol. 59 ›› Issue (5): 731–741.doi: 10.13232/j.cnki.jnju.2023.05.001

• •    下一篇

分流扬声器用于封闭空间降噪的布放研究

徐陈淳, 王有藩, 陶建成()   

  1. 教育部近代声学重点实验室,南京大学声学研究所,南京,210093
  • 收稿日期:2023-06-03 出版日期:2023-09-30 发布日期:2023-10-13
  • 通讯作者: 陶建成 E-mail:jctao@nju.edu.cn
  • 基金资助:
    国家自然科学基金(11874218)

A study of the placement of shunt loudspeakers for noise reduction in enclosed spaces

Chenchun Xu, Youfan Wang, Jiancheng Tao()   

  1. Institute of Acoustics of Nanjing University,Key Laboratory of Modern Acoustics,Ministry of Education,Nanjing,210093,China
  • Received:2023-06-03 Online:2023-09-30 Published:2023-10-13
  • Contact: Jiancheng Tao E-mail:jctao@nju.edu.cn

摘要:

分流扬声器将入射声能转化成电能进行储存和耗散,可作为一种共振吸声体.对界面刚性的长方体封闭空间建立解析模型,分析在顶面布放分流扬声器时布放方式对空间内低频噪声的控制效果.数值仿真表明:在封闭空间本征频率附近,布放分流扬声器可有效降低空间内的平均声压级;当分流扬声器数目有限时,布放在初始声压级大的区域能产生更好的降噪效果;长方体顶角是所有模态响应较大的位置,因此是宽带降噪时布放分流扬声器的较优选择.地面铺设吸声材料后,封闭空间内平均声压级整体降低,但上述分流扬声器布放方式的影响规律依然存在.最后,实验验证了数值仿真结果.

关键词: 分流扬声器, 封闭空间噪声控制, 低频, 布放优化

Abstract:

The shunt loudspeaker can be used as a resonant sound absorber,as it can convert incident sound energy into electrical energy for storage and dissipation. In this paper,an analytical model is established for a rectangular rigid enclosure with shunt loudspeakers on the ceiling to analyze the noise reduction performance at low frequencies. Numerical simulations show that the sound pressure level inside the enclosure can be significantly reduced at its characteristic frequencies by using shunt loudspeakers. Better noise reduction is achieved when the shunt loudspeakers with limited numbers are placed at the locations with high initial noise level. Therefore,the top corners of the rectangle enclosure are optimal locations when employing shunt loudspeakers for broadband noise reduction,because large responses occur there for all the enclosure modes. If the ground is covered with sound absorption materials,the placement effects of the shunt loudspeakers on the noise reduction still remain although the overall sound pressure level in the enclosure decreases. Finally,experiments are conducted to verify the numerical simulation results.

Key words: shunt loudspeaker, noise control in enclosure, low frequency, placement optimization

中图分类号: 

  • O429

图1

(a)长方体封闭空间模型;(b)分流扬声器示意图"

图2

分流扬声器振膜表面的(a)正入射吸声系数和(b)法向声阻抗率"

图3

分流扬声器的布放方式(a) without SL,(b) 42 SLs covering the ceiling,(c) 12 SLs at the ceiling center,(d) 12 SLs along the 2 short sides of the ceiling,(e) 12 SLs along the 2 long sides of the ceiling,(f) 12 SLs at the 4 ceiling corners"

图4

刚性界面的封闭空间中不同分流扬声器布放下的平均声压级频谱(a) without SL,at the center,along the long sides and (b) covering the ceiling,along the short sides,at the corners"

表1

144 Hz时分流扬声器在不同布放方式下的平均声压级和降噪量 (dB)"

扬声器的布放方式

方式

(a)

方式

(b)

方式

(c)

方式

(d)

方式

(e)

方式

(f)

SPLs72.366.575.171.874.3
SPLr72.354.768.258.662.759.5
ΔSPLr17.64.113.79.612.8

表2

168 Hz时分流扬声器在不同布放方式下的平均声压级和降噪量 (dB)"

扬声器的布放方式

方式

(a)

方式

(b)

方式

(c)

方式

(d)

方式

(e)

方式

(f)

SPLs70.967.870.373.472.6
SPLr70.956.865.663.559.961.5
ΔSPLr14.15.37.411.09.4

图5

刚性界面下未放置分流扬声器的声压级分布(a) 144 Hz,at z=lz plane,(b) 144 Hz,at y=0 plane, (c) 168 Hz,at z=lz plane and (d) 168 Hz,at x=0 plane"

图6

多孔吸声材料的(a)正入射吸声系数和(b)法向声阻抗率"

图7

(a)地面铺设多孔吸声材料前后封闭空间内平均声压级频谱;(b)地面吸声时封闭空间内不同分流扬声器布放下的平均声压级频谱"

图8

地面吸声时顶面声压级分布:(a) 145 Hz;(b) 168 Hz"

表3

地面吸声时前二阶本征频率处分流扬声器典型布放下的平均声压级和降噪量 (dB)"

频率145 Hz168 Hz

分流扬声器

布放方式

不布放

方式(a)

最优布放

方式(d)

顶角布放

方式(f)

不布放

方式(a)

最优布放

方式(e)

顶角布放

方式(f)

SPLs65.064.565.364.7
SPLr62.356.156.662.756.757.3
ΔSPLr6.25.76.05.4

图9

实验装置"

图10

封闭空间中不同分流扬声器布放下的平均声压级频谱(a) with rigid boundaries,(b) with sound absorption material laying on the bottom surface"

表4

刚性边界时本征频率处分流扬声器不同布放下实测平均声压级和降噪量 (dB)"

分流扬声器布放方式方式(a)方式(b)方式(c)方式(d)方式(e)方式(f)
147 HzSPLs87.783.789.987.589.6
SPLr87.474.484.177.080.777.7
ΔSPLr13.13.310.56.79.7
171 HzSPLs86.282.685.988.287.9
SPLr85.874.781.780.577.678.7
ΔSPLr11.24.15.38.27.2

表5

地面吸声时本征频率处分流扬声器不同布放下实测平均声压级和降噪量 (dB)"

分流扬声器布放方式方式(a)方式(b)方式(c)方式(d)方式(e)方式(f)
147 HzSPLs82.778.384.982.684.6
SPLr82.873.681.075.878.676.4
ΔSPLr9.31.97.04.36.4
169 HzSPLs82.478.982.684.584.0
SPLr82.573.979.778.676.177.1
ΔSPLr8.62.83.96.45.3
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