CN109148123B - Acoustic metamaterial barrier system for transformer noise spatial distribution characteristics - Google Patents
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Abstract
一种针对变压器噪声空间分布特性的可调声学超材料屏障系统,由声学超材料屏障(3)和噪声测量分析系统(2)组成。声学超材料屏障(3)由超材料支撑支架(7)和分形结构声学超材料模块(8)组成。超材料支撑支架(7)与变压器声源面(1)平行。分形结构声学超材料模块(8)嵌入超材料支撑支架(4)内。噪声测量分析系统(2)测量声学超材料屏障(3)范围内的噪声,分析得到噪声空间分布特性。根据噪声空间分布特性,选取不同参数的分形结构声学超材料模块(8)。当声波传输至声学超材料屏障(3)时,由于声学超材料模块(8)参数是根据对应位置噪声分布特性选取的,可使目标降噪区域的噪声幅值大大降低。
An adjustable acoustic metamaterial barrier system aiming at the spatial distribution characteristics of transformer noise is composed of an acoustic metamaterial barrier (3) and a noise measurement and analysis system (2). The acoustic metamaterial barrier (3) is composed of a metamaterial support bracket (7) and a fractal structure acoustic metamaterial module (8). The metamaterial support bracket (7) is parallel to the sound source surface (1) of the transformer. The fractal structure acoustic metamaterial module (8) is embedded in the metamaterial support bracket (4). The noise measurement and analysis system (2) measures the noise within the range of the acoustic metamaterial barrier (3), and analyzes the noise spatial distribution characteristics. According to the spatial distribution characteristics of noise, a fractal structure acoustic metamaterial module (8) with different parameters is selected. When the sound wave is transmitted to the acoustic metamaterial barrier (3), since the parameters of the acoustic metamaterial module (8) are selected according to the noise distribution characteristics of the corresponding position, the noise amplitude of the target noise reduction area can be greatly reduced.
Description
技术领域technical field
本发明涉及一种声学超材料屏障。The present invention relates to an acoustic metamaterial barrier.
背景技术Background technique
变压器本体噪声主要来源于铁心、绕组的振动,噪声集中在100Hz的倍频,以低频噪声为主。变压器风扇噪声则为500-2000Hz之间的宽频噪声。随着城市的建设,大量的110kV、220kV变电站越来越接近中心城区。噪声传播环境复杂,声波的干涉、衍射等作用导致变压器噪声问题日益突出,不可避免的对站内工作人员和附近居民产生影响。因此,如何在传播途径控制变压器噪声,已经成为环保部门和电力部门亟待解决的重要问题。The noise of the transformer body mainly comes from the vibration of the iron core and the winding, and the noise is concentrated in the frequency multiplication of 100Hz, mainly low-frequency noise. Transformer fan noise is broadband noise between 500-2000Hz. With the construction of the city, a large number of 110kV and 220kV substations are getting closer and closer to the central city. The noise propagation environment is complex, and the interference and diffraction of sound waves lead to increasingly prominent transformer noise problems, which inevitably affect the station staff and nearby residents. Therefore, how to control the transformer noise in the transmission route has become an important problem to be solved urgently by the environmental protection department and the electric power department.
目前针对变压器噪声的降噪方法主要有:有源降噪及材料降噪。有源降噪即主动降噪,如中国专利CN106251855A《一种用于变压器降噪的非集中式虚拟声屏障》公开的有源声屏障安装在房间的开口面附近,由控制声源、误差传声器、参考传感器、多个单通道有源控制器和外围电路组成,可控制房间内声源通过开口向外辐射的噪声。有源声屏障的优点是控制灵活,缺点是当阵列数量增多时,控制难度很大。At present, the noise reduction methods for transformer noise mainly include active noise reduction and material noise reduction. Active noise reduction means active noise reduction. For example, Chinese patent CN106251855A "A Decentralized Virtual Sound Barrier for Transformer Noise Reduction" discloses that the active sound barrier is installed near the opening surface of the room, controlled by the sound source and error microphone. , reference sensor, multiple single-channel active controllers and peripheral circuits, which can control the noise radiated from the sound source in the room through the opening. The advantage of active sound barriers is flexible control, but the disadvantage is that when the number of arrays increases, the control is very difficult.
变压器本体噪声以低频噪声为主,传统隔声材料制作的声屏障对低频噪声的降噪效果很差。声学超材料具有负折射、强反射、负质量密度、负体积模量等超常物理特性,相比传统材料具有隔声量大、厚度小等优点,可以实现较小尺寸的材料控制低频噪声,有效弥补传统材料屏障难以阻隔低频噪声的不足,在变压器降噪领域有良好的发展前景。中国专利CN106192785A《一种用于变电站的全频段降噪声屏障及屏蔽装置》公布的声屏障包括超材料低频降噪层和高频降噪层,置于变压器附近,在变压器噪声传播路径上降低全频段噪声。专利公布的声学超材料屏障未考虑噪声空间分布的差异性,声屏障一旦建立,不能根据空间声场的分布的变化进行灵活调整,导致降噪效果不佳。The noise of the transformer itself is mainly low-frequency noise, and the sound barrier made of traditional sound insulation materials has poor noise reduction effect on low-frequency noise. Acoustic metamaterials have extraordinary physical properties such as negative refraction, strong reflection, negative mass density, and negative bulk modulus. Compared with traditional materials, they have the advantages of large sound insulation and small thickness, and can achieve smaller-sized materials to control low-frequency noise and effectively compensate for The traditional material barrier is difficult to block low-frequency noise, and it has a good development prospect in the field of transformer noise reduction. Chinese patent CN106192785A "A full-band noise reduction barrier and shielding device for substations", the sound barrier includes a metamaterial low-frequency noise reduction layer and a high-frequency noise reduction layer, which are placed near the transformer and reduce the noise transmission path of the transformer. full-band noise. The acoustic metamaterial barrier disclosed in the patent does not consider the difference in the spatial distribution of noise. Once the sound barrier is established, it cannot be flexibly adjusted according to the distribution of the spatial sound field, resulting in poor noise reduction effect.
发明内容SUMMARY OF THE INVENTION
本发明的目的是克服现有技术的缺点,提出一种针对变压器噪声空间分布特性的声学超材料屏障系统。The purpose of the present invention is to overcome the shortcomings of the prior art and propose an acoustic metamaterial barrier system aiming at the spatial distribution characteristics of transformer noise.
本发明声学超材料屏障系统包括声学超材料屏障和噪声测量分析系统,置于室内变压器通风口外侧或室外变压器四周。The acoustic metamaterial barrier system of the present invention includes an acoustic metamaterial barrier and a noise measurement and analysis system, which are placed outside the ventilation opening of the indoor transformer or around the outdoor transformer.
所述声学超材料屏障由超材料支撑支架和分形结构声学超材料模块组成,分形结构声学超材料模块嵌入超材料支撑支架内。The acoustic metamaterial barrier is composed of a metamaterial support bracket and a fractal structure acoustic metamaterial module, and the fractal structure acoustic metamaterial module is embedded in the metamaterial support bracket.
建立声学超材料屏障时,噪声测量分析系统测量声学超材料屏障位置的噪声特性,根据噪声空间分布,选择声学超材料屏障的每个分形结构声学超材料模块的分形阶数和声波波导宽度参数。当声源发生变化时,空间声场发生变化,再次通过噪声测量分析系统测量噪声,根据变化后的声场分布,调整声学超材料屏障的每个分形结构声学超材料模块的分形阶数和声波波导宽度参数,用调整参数后的声学超材料屏障的分形结构声学超材料模块替换之前的分形结构声学超材料模块。When building an acoustic metamaterial barrier, the noise measurement and analysis system measures the noise characteristics at the location of the acoustic metamaterial barrier, and selects the fractal order and acoustic waveguide width parameters of each fractal structure acoustic metamaterial module of the acoustic metamaterial barrier according to the spatial distribution of the noise. When the sound source changes, the spatial sound field changes, and the noise is measured again through the noise measurement and analysis system. According to the changed sound field distribution, the fractal order and acoustic waveguide width of each fractal structure acoustic metamaterial module of the acoustic metamaterial barrier are adjusted. parameters, replace the previous fractal structure acoustic metamaterial module with the fractal structure acoustic metamaterial module of the acoustic metamaterial barrier after adjusting the parameters.
所述超材料支撑支架为长方体。除去顶面和底面,变压器有四个方向的外轮廓面。定义任何一个方向的外轮廓面为变压器声源面。变压器声源面与所述超材料支撑支架平行,二者之间有一定距离。所述超材料支撑支架与变压器声源面正对的一面开有m×n个矩形通孔,m、n为正整数。矩形通孔尺寸相同,等距排布,形成阵列。The metamaterial support bracket is a rectangular parallelepiped. Except for the top and bottom surfaces, the transformer has four-directional outer contour surfaces. Define the outer contour surface in any direction as the sound source surface of the transformer. The sound source surface of the transformer is parallel to the metamaterial support bracket, and there is a certain distance between them. The side of the metamaterial support bracket facing the sound source side of the transformer is provided with m×n rectangular through holes, where m and n are positive integers. The rectangular vias have the same size and are equally spaced to form an array.
所述分形结构声学超材料模块嵌于超材料支撑支架矩形通孔中,且每个矩形通孔中的分形结构声学超材料模块均可拆卸。所述分形结构声学超材料模块与变压器声源面平行,距离变压器声源面近的面为声波入口面,距离变压器声源面远的面为声波出口面。与声波入口面和声波出口面垂直的面为分形结构声学超材料模块的横截面。The fractal structure acoustic metamaterial module is embedded in a rectangular through hole of the metamaterial support bracket, and the fractal structure acoustic metamaterial module in each rectangular through hole can be disassembled. The fractal structure acoustic metamaterial module is parallel to the sound source surface of the transformer, the surface close to the sound source surface of the transformer is the sound wave inlet surface, and the surface far from the sound source surface of the transformer is the sound wave exit surface. The plane perpendicular to the acoustic wave inlet surface and the acoustic wave exit surface is the cross section of the fractal structure acoustic metamaterial module.
所述分形结构声学超材料模块为由分形结构声学超材料单元组成的阵列。所述声学超材料单元的横截面为具有一定宽度Hilbert曲线型通道的矩形面。一定宽度的Hilbert曲线型通道称为声波波导。The fractal structure acoustic metamaterial module is an array composed of fractal structure acoustic metamaterial units. The cross section of the acoustic metamaterial unit is a rectangular surface with a certain width of the Hilbert curve channel. A Hilbert curved channel of a certain width is called an acoustic waveguide.
所述分形结构声学超材料单元的隔声频率与分形阶数和声波波导的宽度密切相关。The sound insulation frequency of the fractal structure acoustic metamaterial unit is closely related to the fractal order and the width of the acoustic waveguide.
建立分形结构声学超材料单元模型,给定声学超材料单元的分形阶数和波导宽度的参数范围,进行给定分形阶数下的波导宽度参数扫描,通过声场计算,得到给定阶数和波导宽度的声学超材料单元在不同频率的隔声量。Establish a fractal structure acoustic metamaterial element model, given the fractal order of the acoustic metamaterial element and the parameter range of the waveguide width, scan the waveguide width parameters under the given fractal order, and obtain the given order and waveguide through the sound field calculation. The amount of sound insulation of a wide acoustic metamaterial unit at different frequencies.
依据结构场和声场耦合方程(1)及声压波动方程(2)计算测量点的声压。The sound pressure at the measurement point is calculated according to the coupling equation (1) of the structure field and the sound field and the sound pressure wave equation (2).
其中,ρ0为质量密度,v为振动速度,p为声压,c为声速,▽为哈密顿算子。Among them, ρ 0 is the mass density, v is the vibration velocity, p is the sound pressure, c is the sound velocity, and ▽ is the Hamiltonian.
其中,ρ0为质量密度,p为声压,c为声速,▽为哈密顿算子,t为声波传播时间。Among them, ρ 0 is the mass density, p is the sound pressure, c is the sound speed, ▽ is the Hamiltonian operator, and t is the sound wave propagation time.
根据声压可以得到声压级:The sound pressure level can be obtained from the sound pressure:
其中,p为声压,pref为参考声压,国际取为2×10-5Pa,SPL为声压级,根据声压级得到隔声量:Among them, p is the sound pressure, pre is the reference sound pressure, the international value is 2×10 -5 Pa, SPL is the sound pressure level, and the sound insulation is obtained according to the sound pressure level:
TL=SPL2-SPL1 (4)TL=SPL 2 -SPL 1 (4)
其中,SPL2为为加入超材料单元时测量点位置的声压级,SPL1为加入超材料单元后测量点位置的声压级,TL为隔声量。Among them, SPL 2 is the sound pressure level at the measurement point when the metamaterial unit is added, SPL 1 is the sound pressure level at the measurement point after adding the metamaterial unit, and TL is the sound insulation.
隔声量高的频率范围为给定参数的声学超材料单元的最优隔声频率范围。根据最优隔声频率范围选择与该隔声频率范围对应的给定分形结构声学超材料单元的分形阶数和声波波导宽度。The frequency range with high sound insulation is the optimal sound insulation frequency range of the acoustic metamaterial unit with given parameters. According to the optimal sound insulation frequency range, the fractal order and acoustic waveguide width of a given fractal structure acoustic metamaterial unit corresponding to the sound insulation frequency range are selected.
空气在分形结构声学超材料单元中沿声波波导流通。Air circulates along acoustic waveguides in fractal-structured acoustic metamaterial cells.
所述噪声测量分析系统由传感器支撑支架、声压传感器和声压信号处理模块组成。声压传感器置于传感器支撑支架上,声压信号处理模块与声压传感器连接。The noise measurement and analysis system is composed of a sensor support bracket, a sound pressure sensor and a sound pressure signal processing module. The sound pressure sensor is placed on the sensor support bracket, and the sound pressure signal processing module is connected with the sound pressure sensor.
所述传感器支撑支架与超材料支撑支架平行,布置在超材料支撑支架的近处,且与超材料支撑支架同位于变压器的同一侧。所述传感器支撑支架为长方体结构,高度和超材料屏障支撑支架的高度相等,宽度小于超材料屏障支撑支架的宽度。所述传感器支撑支架包括多个横梁和竖梁,横梁和竖梁交叉形成多个矩形通孔,每个矩形通孔的尺寸相同,且矩形通孔的长度小于或等于超材料支撑支架矩形通孔长度的1/2,宽度小于或等于超材料支撑支架矩形通孔宽度的1/2。所述传感器支撑支架能够沿着与声学超材料屏障平行的方向移动。The sensor support bracket is parallel to the metamaterial support bracket, is arranged near the metamaterial support bracket, and is located on the same side of the transformer as the metamaterial support bracket. The sensor support bracket is a cuboid structure, the height is equal to the height of the metamaterial barrier support bracket, and the width is smaller than the width of the metamaterial barrier support bracket. The sensor support bracket includes a plurality of beams and vertical beams, the beams and the vertical beams intersect to form a plurality of rectangular through holes, the size of each rectangular through hole is the same, and the length of the rectangular through hole is less than or equal to the rectangular through hole of the metamaterial support bracket. 1/2 the length, and the width is less than or equal to 1/2 the width of the rectangular through hole of the metamaterial support bracket. The sensor support bracket can move in a direction parallel to the acoustic metamaterial barrier.
所述声压传感器置于传感器支撑支架横梁和竖梁的交点位置,形成声压传感器阵列。The sound pressure sensor is placed at the intersection of the transverse beam and the vertical beam of the sensor support bracket to form a sound pressure sensor array.
所述声压信号处理模块包括前置放大器、滤波器、A/D转换器和DSP处理器。所述前置放大器的输入端与声压传感器连接,放大声压传感器采集的噪声信号;所述滤波器的输入端与所述前置放大器的输出端连接,滤除声压传感器采集的噪声信号中的高频分量,将采集到的声压模拟信号由滤波器的输出端送至A/D转换器;信号经A/D转换器采样后送至DSP处理器的输入端;DSP处理器将噪声信号进行插值计算和频谱分析,得到传感器支撑支架范围内的噪声分布特性和频谱特性。The sound pressure signal processing module includes a preamplifier, a filter, an A/D converter and a DSP processor. The input end of the preamplifier is connected to the sound pressure sensor to amplify the noise signal collected by the sound pressure sensor; the input end of the filter is connected to the output end of the preamplifier to filter out the noise signal collected by the sound pressure sensor The high-frequency components in the medium, the collected sound pressure analog signal is sent to the A/D converter from the output end of the filter; the signal is sampled by the A/D converter and then sent to the input end of the DSP processor; the DSP processor will The noise signal is subjected to interpolation calculation and spectrum analysis to obtain the noise distribution characteristics and spectrum characteristics within the range of the sensor support bracket.
本发明工作过程为:传感器支撑支架与超材料支撑支架间隔距离很小且平行放置,传感器支撑支架与超材料支撑支架的外侧竖梁对齐。噪声测量分析系统测量并记录噪声,测量完成后,保持传感器支撑支架与超材料支撑支架距离不变,移动噪声测量分析系统测量下一个区域的噪声分布,直到测量范围覆盖整个声学超材料屏障为止。分析获得声学超材料屏障范围内的噪声空间分布特性。噪声测量分析系统对时间域的噪声进行频谱分析,得到噪声的频率域特性,从而得到超材料支撑支架每个矩形通孔位置的隔声频率范围。根据最优隔声频率范围和超材料支撑支架矩形通孔位置的隔声频率范围相同的原则,选取分形结构声学超材料模块嵌入超材料支撑支架矩形通孔内。所述分形结构声学超材料模块的声学超材料单元,其分形阶数和声波波导宽度为与最优隔声频率范围相同的隔声频率范围对应的分形结构声学超材料单元的分形阶数和声波波导宽度。当声源发生变化时,噪声空间分布发生变化,再次通过噪声测量分析系统测量噪声,根据变化后的声场分布,拆卸对应声场发生变化位置处的分形结构声学超材料模块,将其替换为针对声场变化后声场特性设计的分形结构声学超材料模块,针对声场变化后声场特性设计的分形结构声学超材料模块的分形结构声学超材料单元的分形阶数和声波波导宽度为声场变化后的隔声频率范围对应的分形结构声学超材料单元的分形阶数和声波波导宽度。The working process of the present invention is as follows: the sensor support bracket and the metamaterial support bracket have a small distance and are placed in parallel, and the sensor support bracket is aligned with the outer vertical beam of the metamaterial support bracket. The noise measurement and analysis system measures and records the noise. After the measurement is completed, keep the distance between the sensor support bracket and the metamaterial support bracket unchanged, and move the noise measurement and analysis system to measure the noise distribution in the next area until the measurement range covers the entire acoustic metamaterial barrier. The spatial distribution characteristics of noise within the acoustic metamaterial barrier are obtained by analysis. The noise measurement and analysis system performs spectrum analysis on the noise in the time domain to obtain the frequency domain characteristics of the noise, thereby obtaining the sound insulation frequency range of each rectangular through-hole position of the metamaterial support bracket. According to the principle that the optimal sound insulation frequency range is the same as the sound insulation frequency range of the rectangular through hole of the metamaterial support bracket, the acoustic metamaterial module with fractal structure is selected to be embedded in the rectangular through hole of the metamaterial support bracket. In the acoustic metamaterial unit of the fractal structure acoustic metamaterial module, the fractal order and the width of the acoustic wave guide are the fractal order and sound waves of the fractal structure acoustic metamaterial unit corresponding to the same sound insulation frequency range as the optimal sound insulation frequency range. Waveguide width. When the sound source changes, the spatial distribution of the noise changes, and the noise is measured again through the noise measurement and analysis system. According to the changed sound field distribution, the fractal structure acoustic metamaterial module at the position where the sound field changes is disassembled and replaced with one for the sound field. The fractal structure acoustic metamaterial module designed for the sound field characteristics after the change, the fractal structure acoustic metamaterial module designed for the sound field characteristics after the sound field change The fractal order of the fractal structure acoustic metamaterial unit and the width of the acoustic waveguide are the sound insulation frequencies after the sound field changes The range corresponds to the fractal order and acoustic waveguide width of the fractal-structured acoustic metamaterial unit.
当声波传输至声学超材料屏障时,由于分形结构声学超材料模块参数是根据对应位置噪声分布特性选取的,可使目标降噪区域的声波幅值大大降低。When the sound wave is transmitted to the acoustic metamaterial barrier, since the parameters of the fractal structure acoustic metamaterial module are selected according to the noise distribution characteristics of the corresponding position, the amplitude of the sound wave in the target noise reduction area can be greatly reduced.
本发明针对变压器噪声空间分布特性建立可调声学超材料屏障,能够有效地在传播路径上阻隔变压器噪声,降低环境噪声污染。相比于传统的声屏障,在屏障建立时,本发明可调声学超材料屏障系统根据实测声场分布选择分型结构声学超材料模块参数,可提高降噪效果;同时,当噪声空间分布变化时,可根据实测噪声分布调整声学超材料模块,提高声屏障的灵活性。The invention establishes an adjustable acoustic metamaterial barrier according to the spatial distribution characteristics of transformer noise, which can effectively block transformer noise on the propagation path and reduce environmental noise pollution. Compared with the traditional sound barrier, when the barrier is established, the adjustable acoustic metamaterial barrier system of the present invention selects the parameters of the acoustic metamaterial module of the typed structure according to the measured sound field distribution, which can improve the noise reduction effect; at the same time, when the spatial distribution of noise changes , the acoustic metamaterial module can be adjusted according to the measured noise distribution to improve the flexibility of the sound barrier.
附图说明Description of drawings
图1本发明可调声学超材料屏障系统示意图;1 is a schematic diagram of the tunable acoustic metamaterial barrier system of the present invention;
图2本发明可调声学超材料屏障系统侧视图;2 is a side view of the tunable acoustic metamaterial barrier system of the present invention;
图3本发明噪声测量分析系统正视图;3 is a front view of the noise measurement and analysis system of the present invention;
图4本发明声学超材料屏障正视图;4 is a front view of the acoustic metamaterial barrier of the present invention;
图5本发明声压信号处理模块结构图;5 is a structural diagram of a sound pressure signal processing module of the present invention;
图6本发明声学超材料单元横截面图。Figure 6 is a cross-sectional view of the acoustic metamaterial unit of the present invention.
图中:1变压器声源面,2噪声测量分析系统,3声学超材料屏障,4传感器支撑支架,5声压传感器,6声压信号处理模块,7超材料支撑支架,8分形结构声学超材料模块,9前置放大器,10滤波器,11A/D转换器,12DSP处理器,13一阶分形结构声学超材料单元横截面,14二阶分形结构声学超材料单元横截面,15三阶分形结构声学超材料单元横截面,16四阶分形结构声学超材料单元横截面。In the picture: 1 transformer sound source surface, 2 noise measurement and analysis system, 3 acoustic metamaterial barrier, 4 sensor support bracket, 5 sound pressure sensor, 6 sound pressure signal processing module, 7 metamaterial support bracket, 8 fractal structure acoustic metamaterial Modules, 9 preamplifiers, 10 filters, 11 A/D converters, 12 DSP processors, 13 first-order fractal structure acoustic metamaterial unit cross-sections, 14 second-order fractal structures acoustic metamaterial unit cross-sections, 15 third-order fractal structures Acoustic metamaterial unit cross section, 16 fourth order fractal structure acoustic metamaterial unit cross section.
具体实施方式Detailed ways
以下结合附图和具体实施方式进一步说明本发明。The present invention is further described below with reference to the accompanying drawings and specific embodiments.
如图1和图2所示,本发明针对变压器噪声空间分布特性的可调声学超材料屏障系统,置于室内变压器通风口外侧或室外变压器四周,包括声学超材料屏障3和噪声测量分析系统2。As shown in FIGS. 1 and 2 , the adjustable acoustic metamaterial barrier system of the present invention for the spatial distribution characteristics of transformer noise is placed outside the indoor transformer vent or around the outdoor transformer, including an acoustic metamaterial barrier 3 and a noise measurement and
如图4所示,所述声学超材料屏障3由超材料支撑支架7和分形结构声学超材料模块8组成,所述分形结构声学超材料模块8嵌于超材料支撑支架7内。As shown in FIG. 4 , the acoustic metamaterial barrier 3 is composed of a
所述超材料支撑支架7为长方体。除去顶面和底面,变压器有四个方向的外轮廓面。定义任何一个方向的外轮廓面为变压器声源面。变压器声源面1与所述超材料支撑支架7平行,二者之间有一定距离。所述超材料支撑支架7与变压器声源面1正对的一面开有m×n个矩形通孔,m、n为正整数。矩形通孔尺寸相同,等距排布,形成阵列。The
所述分形结构声学超材料模块8嵌于超材料支撑支架7的矩形通孔中,且每个矩形通孔中的分形结构声学超材料模块8均可拆卸,被替换。所述分形结构声学超材料模块8与变压器声源面1平行且距离变压器声源面近的面为声波入口面,距离变压器声源面1远的面为声波出口面。与声波入口面和声波出口面垂直的面为分形结构声学超材料模块8的横截面。The fractal structure
所述分形结构声学超材料模块8为由分形结构声学超材料单元组成的阵列。所述分形结构声学超材料单元的横截面为具有一定宽度Hilbert曲线型通道的矩形面,如图6所示。所述分形结构声学超材料单元截面形式可以为一阶13、二阶14、三阶15或四阶16。所述分形结构声学超材料单元的阶数和声波波导的宽度与隔声频率密切相关。The fractal structure
建立分形结构声学超材料单元模型,给定声学超材料单元的分形阶数和波导宽度的参数范围,进行给定分形阶数下的波导宽度参数扫描,通过声场计算,得到给定阶数和波导宽度的声学超材料单元在不同频率的隔声量。Establish a fractal structure acoustic metamaterial element model, given the fractal order of the acoustic metamaterial element and the parameter range of the waveguide width, scan the waveguide width parameters under the given fractal order, and obtain the given order and waveguide through the sound field calculation. The amount of sound insulation of a wide acoustic metamaterial unit at different frequencies.
依据结构场和声场耦合方程(1)及声压波动方程(2)计算测量点的声压。The sound pressure at the measurement point is calculated according to the coupling equation (1) of the structure field and the sound field and the sound pressure wave equation (2).
其中,ρ0为质量密度,v为振动速度,p为声压,c为声速,▽为哈密顿算子。Among them, ρ 0 is the mass density, v is the vibration velocity, p is the sound pressure, c is the sound velocity, and ▽ is the Hamiltonian.
其中,ρ0为质量密度,p为声压,c为声速,▽为哈密顿算子,t为声波传播时间。Among them, ρ 0 is the mass density, p is the sound pressure, c is the sound speed, ▽ is the Hamiltonian operator, and t is the sound wave propagation time.
根据声压可以得到声压级:The sound pressure level can be obtained from the sound pressure:
其中,p为声压,pref为参考声压,国际取为2×10-5Pa,SPL为声压级,根据声压级得到隔声量:Among them, p is the sound pressure, pre is the reference sound pressure, the international value is 2×10 -5 Pa, SPL is the sound pressure level, and the sound insulation is obtained according to the sound pressure level:
TL=SPL2-SPL1 (4)TL=SPL 2 -SPL 1 (4)
其中,SPL2为为加入超材料单元时测量点位置的声压级,SPL1为加入超材料单元后测量点位置的声压级,TL为隔声量。Among them, SPL 2 is the sound pressure level at the measurement point when the metamaterial unit is added, SPL 1 is the sound pressure level at the measurement point after adding the metamaterial unit, and TL is the sound insulation.
隔声量高的频率范围为给定参数的声学超材料单元的最优隔声频率范围。根据最优隔声频率范围选择与其相同的隔声频率范围对应的给定分形结构声学超材料单元的分形阶数和声波波导宽度。The frequency range with high sound insulation is the optimal sound insulation frequency range of the acoustic metamaterial unit with given parameters. According to the optimal sound insulation frequency range, the fractal order and acoustic waveguide width of the given fractal structure acoustic metamaterial unit corresponding to the same sound insulation frequency range are selected.
所述噪声测量分析系统2由传感器支撑支架4、声压传感器5和声压信号处理模块6组成。声压传感器5置于传感器支撑支架4上,声压信号处理模块6与声压传感器5连接。所述传感器支撑支架4和声压传感器5的正视图如图3所示。The noise measurement and
所述传感器支撑支架4与超材料支撑支架7平行,布置在超材料支撑支架7的近处,且与超材料支撑支架7同位于变压器的同一侧。所述传感器支撑支架4为长方体,其高度和超材料支撑支架7的高度相等,宽度小于超材料支撑支架7的宽度。所述传感器支撑支架4包括多个横梁和竖梁,横梁和竖梁交叉形成多个矩形通孔,每个矩形通孔的尺寸相同,且矩形通孔的长度小于或等于超材料支撑支架矩形通孔长度的1/2,矩形通孔的宽度小于或等于超材料支撑支架矩形通孔宽度的1/2。所述传感器支撑支架4可以沿着与超材料支撑支架7平行的方向移动。The
所述声压传感器5置于传感器支撑支架4横梁和竖梁的交点位置,形成声压传感器阵列。The
所述声压信号处理模块6包括前置放大器9、滤波器10、A/D转换器11和DSP处理器12。所述前置放大器9的输入端与声压传感器5连接,放大声压传感器5采集的噪声信号;所述滤波器10的输入端与所述前置放大器9的输出端连接,滤除声压传感器5采集的噪声信号中的高频分量,将采集到的声压模拟信号由滤波器10的输出端送至A/D转换器11;信号经A/D采样后送至DSP处理器12的输入端,DSP处理器12将噪声信号进行频谱分析和插值计算,得到声学超材料屏障3范围内的噪声分布和频谱特性。The sound pressure
本发明工作过程为:传感器支撑支架4与超材料支撑支架7间隔距离很小且平行放置,两个支架的外侧竖梁对齐。噪声测量分析系统2测量并记录噪声,测量完成后,保持传感器支撑支架4与超材料支撑支架7距离不变,移动噪声测量分析系统测量下一个区域的噪声分布,直到测量范围覆盖整个声学超材料屏障3为止。分析获得声学超材料屏障范围内的噪声空间分布特性。噪声测量分析系统对时间域的噪声进行频谱分析,得到噪声的频率域特性,从而得到超材料支撑支架7每个矩形通孔位置噪声的隔声频率范围。根据最优隔声频率范围和超材料支撑支架矩形通孔位置的隔声频率范围相同的原则,选取分形结构声学超材料模块8嵌入超材料支撑支架7的矩形通孔内,所述分形结构声学超材料模块的声学超材料单元,其分形阶数和声波波导宽度为与最优隔声频率范围相同的所需隔声频率范围对应的分形结构声学超材料单元的分形阶数和声波波导宽度。当声源发生变化时,空间声场发生变化,再次通过噪声测量分析系统2测量噪声,根据变化后的声场分布,拆卸对应声场发生变化位置处的分形结构声学超材料模块8,将其替换为针对变化后声场特性设计的分形结构声学超材料模块8,针对声场变化后声场特性设计的分形结构声学超材料模块的分形结构声学超材料单元的分形阶数和声波波导宽度为声场变化后的所需隔声频率范围对应的分形结构声学超材料单元的分形阶数和声波波导宽度。当声波传输至声学超材料屏障3时,由于分形结构声学超材料模块8的参数是根据对应位置噪声分布特性选取的,可使目标降噪区域的声波幅值大大降低。The working process of the present invention is as follows: the
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