Pipeline noise control device and method based on local resonance mechanism acoustic metamaterial

文档序号:1873237 发布日期:2021-11-23 浏览:9次 中文

阅读说明:本技术 基于局域共振机理声学超材料的管道噪声控制装置及方法 (Pipeline noise control device and method based on local resonance mechanism acoustic metamaterial ) 是由 沈承 李金泽 杨莎莎 周小玲 施飞舟 张崇峰 于 2021-09-22 设计创作,主要内容包括:本发明公开了基于局域共振机理声学超材料的管道噪声控制装置,包括管道,管道的侧壁嵌装有具有预紧力的柔性薄膜,柔性薄膜上设有若干个连接点,连接点上安装有弹簧振子,弹簧振子和柔性薄膜能产生叠加振动,当入射声激励达到特定的频率时,弹簧振子和柔性薄膜振动产生的辐射声波与入射声波相消。本发明采用了全新的设计方法、尤其对历来难以解决的低频噪声有较好的控制效果,可在超低频段实现高隔声。本发明采用组件数量少、结构简单,因此建造周期短、设计效果显著,具有一定实际工程应用价值。(The invention discloses a pipeline noise control device based on an acoustic metamaterial based on a local resonance mechanism, which comprises a pipeline, wherein a flexible film with pretightening force is embedded on the side wall of the pipeline, a plurality of connection points are arranged on the flexible film, spring vibrators are arranged on the connection points, the spring vibrators and the flexible film can generate superposed vibration, and when incident sound excitation reaches a specific frequency, radiation sound waves generated by the vibration of the spring vibrators and the flexible film are cancelled with the incident sound waves. The invention adopts a brand new design method, has better control effect on low-frequency noise which is difficult to solve ever before, and can realize high sound insulation in an ultra-low frequency band. The invention adopts a small number of components and a simple structure, thereby having short construction period, remarkable design effect and certain practical engineering application value.)

1. Pipeline noise control device based on local resonance mechanism acoustics metamaterial includes pipeline (1), characterized by: the side wall of the pipeline (1) is embedded with a flexible film (2) with pretightening force, the flexible film (2) is provided with a plurality of connection points (3), spring vibrators (4) are mounted on the connection points (3), the spring vibrators (4) and the flexible film (2) can generate superposed vibration, and when incident sound excitation reaches specific frequency, radiation sound waves generated by vibration of the spring vibrators (4) and the flexible film (2) are cancelled with the incident sound waves.

2. The pipeline noise control device based on the local resonance mechanism acoustic metamaterial according to claim 1, wherein: the pipeline (1) is made of rigid materials.

3. The pipeline noise control device based on the local resonance mechanism acoustic metamaterial according to claim 2, wherein: the film (2) is a rectangular elastic film.

4. The local resonance mechanism acoustic metamaterial-based pipeline noise control device as claimed in claim 3, wherein: the film (2) is a silicon rubber film or a polyetherimide film.

5. The local resonance mechanism acoustic metamaterial-based pipeline noise control device as claimed in claim 4, wherein: the spring vibrator (4) is a beam-shaped vibrator.

6. The local resonance mechanism acoustic metamaterial-based pipeline noise control device as claimed in claim 4, wherein: the spring vibrator (4) is made of porous elastic material.

7. The pipeline noise control device based on the local resonance mechanism acoustic metamaterial according to claim 5 or 6, wherein: the mass of the spring vibrator (4) is far less than the mass of the film (2).

8. The method for controlling the pipeline noise control device based on the local resonance mechanism acoustic metamaterial as claimed in claim 1, wherein: the method comprises the following steps:

s1, determining the frequency band and range of the needed isolated noise by measuring the sound pressure level or sound intensity level of the noise source on the spot, measuring the geometric parameter of the pipeline, and obtaining the physical parameter of the transmission medium in the pipeline;

s2, designing and determining the thickness of the flexible film (2), the materials adopted by the flexible film (2) and the spring vibrator (4) and the corresponding mass according to the measured noise parameters and pipeline parameters;

s3, designing a corresponding high sound insulation peak in a specific frequency band by using the combination of the flexible films (2) with different lengths and the plurality of spring vibrators (4) according to the required elimination frequency band;

and S4, determining the installation position and the installation mode of the flexible film (2) and the spring vibrator (4) in each length according to the requirement of the pipeline flow field, and installing.

Technical Field

The invention relates to an acoustic metamaterial applying a local resonance mechanism, which consists of a spring vibrator and a tensioning embedded type film. The structural design is applied to the aspects of sound insulation and noise reduction of the pipeline, and belongs to the field of noise control.

Background

Pipeline structures are common in aerospace, industrial production, vehicles, and other everyday life. The sound wave in the pipe has the characteristics of long propagation distance, small attenuation, large control difficulty and the like, and has important practical application significance in the research of noise reduction of the pipeline. The existing noise elimination design adopts a variable cross-section type automobile tail gas pipe which reflects sound waves by utilizing an acoustic impedance mismatching mechanism; a duct liner for dissipating acoustic energy using damping. But the variable cross-section design is often heavy, and a pass band exists, so that the flow of fluid in the pipe is influenced; the sound damping capacity at low frequencies drops dramatically with the acoustic liner of the sound absorbing material. Membrane Acoustic Metamaterials (MAMs) have attracted a great deal of scholars' attention since their inception, and possess magical properties of light weight, low frequency noise reduction, negative mass density or modulus, and the like. With the development of membrane type acoustic metamaterials, the membrane type acoustic metamaterials are applied to the field of pipeline noise reduction to become new possibilities.

The invention patent application with the application number of 'CN 201610253954.2', entitled 'pipeline noise control method and device based on multi-model adaptive switching' discloses a device for actively controlling pipeline noise; a sound velocity sensor, a reference noise sensor, an error noise sensor and a noise suppression loudspeaker are respectively arranged at different positions in the pipeline. The sound velocity of the noise to be controlled is measured by using a sound velocity sensor, a reference signal of the noise to be controlled is measured by using a reference noise sensor, a residual signal after the active suppression of the noise to be controlled is measured by using an error noise sensor, convolution operation is carried out by using the reference signal and the residual signal, and a domain noise suppression loudspeaker is used, so that the real-time suppression of the pipeline noise is realized. Although the patent has an inhibiting effect on random pipeline noise, the structure is very complex, a large amount of external facilities need to be applied to the outside of the pipeline, and the implementation is difficult under the conditions of strict requirement on the weight of the pipeline and severe working environment.

The invention patent application with the application number of 'CN 201810239630.2' and the name of 'a pipeline noise active control device and method' also discloses a device for actively controlling the pipeline noise; comprises a pipeline and a noise control device arranged on the pipeline. The noise control device comprises a signal conversion unit, a signal acquisition unit, a control unit and an execution unit which are respectively used for executing noise signal conversion, acquisition, receiving control and secondary sound output. The structure is simplified along with the former structure, still has too many additional equipment, changes the drawback of intraductal original flow field, only aims at first-order noise mode simultaneously, can't control follow-up mode.

Disclosure of Invention

The invention aims to solve the problems mentioned in the background technology and provides a pipeline noise control device and method based on an acoustic metamaterial based on a local resonance mechanism.

In order to achieve the technical purpose, the technical scheme adopted by the invention is as follows:

the pipeline noise control device based on the local resonance mechanism acoustic metamaterial comprises a pipeline, wherein a flexible film with pretightening force is embedded on the side wall of the pipeline, a plurality of connection points are arranged on the flexible film, spring vibrators are mounted on the connection points, the spring vibrators and the flexible film can generate superposed vibration, and when incident sound excitation reaches specific frequency, radiation sound waves generated by the spring vibrators and the flexible film are cancelled with the incident sound waves.

In order to optimize the technical scheme, the specific measures adopted further comprise:

the pipeline is made of rigid materials.

The film is a rectangular elastic film.

The film is a silicon rubber film or a polyetherimide film.

The spring vibrator is a beam-shaped vibrator.

The spring oscillator is made of porous elastic material.

The mass of the spring oscillator is far smaller than that of the film.

The pipeline noise control method based on the local resonance mechanism acoustic metamaterial comprises the following steps:

s1, determining the frequency band and range of the needed isolated noise by measuring the sound pressure level or sound intensity level of the noise source on the spot, measuring the geometric parameter of the pipeline, and obtaining the physical parameter of the transmission medium in the pipeline;

s2, designing and determining the thickness of the flexible film, the materials adopted by the flexible film and the spring vibrator and the corresponding mass according to the measured noise parameters and pipeline parameters;

s3, designing a corresponding high sound insulation peak by using the combination of flexible films and a plurality of spring vibrators with different lengths in a specific frequency band according to a required elimination frequency band;

and S4, determining the installation position and the installation mode of the flexible film and the spring vibrator in each length according to the requirement of the pipeline flow field, and installing.

The invention has the following advantages:

(1) the invention adopts a brand-new design method, has better control effect on low-frequency noise which is difficult to solve ever before, and can realize high sound insulation (more than 20 dB) in an ultra-low frequency band (near 100 Hz).

(2) The invention is essentially an acoustic metamaterial design method, and has the characteristic of negative mass density in a specified working frequency band, so that the acoustic metamaterial can be better made into a light structure, and is different from the traditional pipeline noise control method, and has fewer additional devices and less influence on the pipeline.

(3) The sound insulation design method provided by the invention has the corresponding theory and simulation result as supports, so that the sound insulation design method is strong in expansibility and wide in design space in the future.

(4) The invention has the advantages of short construction period, obvious design effect and certain practical engineering application value because of adopting a small number of components and simple structure.

Drawings

FIG. 1 is a two-dimensional schematic diagram of a pipeline noise control structure based on a local resonance mechanism;

FIG. 2 is a simplified schematic diagram of a two-degree-of-freedom system of a film-singlet at localized resonance;

fig. 3 shows a practical application of the vibrator of the present invention: a "beam-like" vibrator;

fig. 4 shows a practical application of the vibrator of the present invention: a porous elastomeric material;

fig. 5 is a sound insulation curve TL (theoretical and simulation results) for a single vibrator;

FIG. 6 is a graph of velocity mode comparison with and without vibrators;

fig. 7 is a sound insulation curve TL (theoretical and simulation results) for a multi-vibrator.

The label names in the figure: the flexible pipe comprises a pipeline 1, a flexible film 2, a connecting point 3 and a spring vibrator 4.

Detailed Description

Embodiments of the present invention are described in further detail below with reference to the accompanying drawings.

Referring to fig. 1, 2 and 3, the pipeline noise silencer based on the local resonance principle is mainly technically characterized in that a flexible film 2 is embedded in the side wall of a pipeline 1, a plurality of small spring vibrators 4 are applied to the flexible film 2, structural parameters are changed according to the required noise reduction frequency, and the noise at the frequency is eliminated by using a local resonance mechanism. Specific embodiments are as follows:

the thin film acoustic metamaterial silencer structure comprises a pipeline 1; the pipeline assumes a square pipe, the side of the pipeline replaces the original rigid wall with a flexible film 2, a spring vibrator 4 is attached to the flexible film 2, and if noise is not expected to radiate from the film to the outside, a rigid cavity can be arranged on the outer side of the film. The membrane vibration displacement is the same as the spring vibrator displacement at the connection point 3. The film is an elastic film material, such as a silicon rubber film or a polyetherimide film, and needs to be tensioned according to a preset value in advance in the installation process, and certain transverse rigidity is provided through pretightening force. The spring element 4 may be a "beam-like element" or a porous wire elastic material in actual installation, and its own natural frequency needs to be determined by a two-degree-of-freedom simplified model (fig. 2).

The pipe 1 is connected to a noise source, and the noise sound wave is represented as a 0 th plane wave in the pipe when the noise frequency is lower than the cutoff frequency of the pipe. The film and the vibrator form a local resonance unit, when the noise frequency reaches the resonance frequency of the simplified system of the unit, the vibrator resonates, the radiated sound wave and the incident sound wave are cancelled, the STL curve at the moment has a peak value, namely the sound insulation effect reaches the best, and the noise cannot be transmitted continuously, so that the noise reduction and elimination effect is achieved.

The embodiments and the sound insulation mechanism of the invention are further described in detail below with reference to the accompanying drawings and examples:

the duct 1 has a structure as shown in fig. 1, and is shaped as a square pipe, which is a rigid material, and it is assumed that it has a hard sound field boundary condition and the frequency of the sound source is lower than the cutoff frequency of the duct. The side of pipeline is inlayed and is equipped with flexible film 2, can regard the boundary condition of junction as simply to support, is provided with a plurality of spring oscillator tie points 3 on flexible film 2, and specific tie point figure is decided according to the demand of silencer, including the frequency of making an uproar, frequency width and the volume of making an uproar isoparametric of making an uproar. The spring vibrator 4 is attached to the connection point 3, a porous material or a beam-shaped vibrator made of a rigid material can be considered when the vibrator is installed, the influence of strong nonlinearity caused by large mass of the vibrator on the transverse rigidity of the film is avoided, the thickness of the film is far smaller than the height of a pipeline, and the only mechanical restoring force is tension.

As a supplement, the rigid material of the pipe 1 may be common 45 steel, or may be directly selected according to the application scenario, so long as the medium characteristic impedance is far greater than that of the film.

In addition, the flexible film 2 is a rectangular elastic film, and a common silicone rubber film or polyetherimide film or other elastic materials with high flexibility are generally adopted.

In addition to the above, the thickness of the flexible membrane 2 should be much smaller than the height of the pipe, ensuring that the only mechanical restoring force in the model is the correctness of the tension.

In addition, the spring vibrator 4 (in fig. 1) can be designed into a beam-shaped vibrator (as shown in fig. 3 a) in practical application, or a vibrator-like form (as shown in fig. 3 b) composed of soft-hard material blocks or other structural forms with the same principle, and can also be replaced by porous elastic material (as shown in fig. 4), which is convenient for engineering practical application.

In addition to the above, the mass of the spring vibrator should be much smaller than the mass of the film itself to conform to a linear approximation to the micro-vibrations.

The following parameters are used in the case to illustrate the mechanism of sound insulation: the height of the pipeline is 10cm, the length of the film is 10cm, only one side is embedded, the rigidity of the vibrator is 1000N/m, the mass is 0.001kg, and the medium in the pipe is air, so the sound velocity is 340 m/s. And calculating by using an MATLAB accurate solution, and simultaneously performing simulation calculation on the structure by using COMSOL, so that the situation of incident noise at infinity is simulated by using a perfect matching layer.

When sound waves enter the pipeline, the film and the vibrator are subjected to sound excitation, the first-order natural vibration mode of the original system is changed by the addition of the vibrator, the frequency of first-order resonance is reduced, and therefore a first sound insulation peak appears at 134Hz (as shown in figure 5). The 134Hz is not the natural frequency of the oscillator itself, but the local resonance frequency of a two-degree-of-freedom model (as shown in fig. 2) obtained by simplifying the film and the oscillator at the time of resonance. Similar to the first peak sound insulation, the subsequent peaks also correspond to the local resonance frequencies of the system. The addition of the vibrator changes other vibration modes at the same time, and essentially changes the vibration speed field of the film, thereby improving the sound insulation performance. As shown in fig. 6, the first order velocity mode is greatly improved by adding the oscillator, and the even order velocity mode is not changed by the central oscillator because the oscillator is just at the vibration node, and the eccentric oscillator has influence on each order velocity mode.

When the number of vibrators is increased, the sound insulation peak value (figure 7) of specific frequency can be increased, at the moment, the model can be simplified into a corresponding multi-degree-of-freedom model, and the structure can be directionally designed according to the target noise reduction amount and the target noise reduction frequency band. The analysis is designed aiming at the single-side embedded film, and if the films are arranged on the opposite sides, the noise reduction bandwidth can be further widened, and the noise reduction effect is improved.

The above is only a preferred embodiment of the present invention, and the protection scope of the present invention is not limited to the above-mentioned embodiments, and all technical solutions belonging to the idea of the present invention belong to the protection scope of the present invention. It should be noted that modifications and embellishments within the scope of the invention may be made by those skilled in the art without departing from the principle of the invention.

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