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CN103411904A - Opto-acoustic gas sensing device based on polyvinylidene fluoride piezoelectric film - Google Patents

Opto-acoustic gas sensing device based on polyvinylidene fluoride piezoelectric film Download PDF

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CN103411904A
CN103411904A CN2013103236026A CN201310323602A CN103411904A CN 103411904 A CN103411904 A CN 103411904A CN 2013103236026 A CN2013103236026 A CN 2013103236026A CN 201310323602 A CN201310323602 A CN 201310323602A CN 103411904 A CN103411904 A CN 103411904A
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polyvinylidene fluoride
piezoelectric film
device based
fluoride piezoelectric
sensing device
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CN103411904B (en
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刘锟
高晓明
汪磊
谈图
张为俊
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Hefei Institutes of Physical Science of CAS
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Abstract

本发明公开了一种基于聚偏氟乙烯压电薄膜的光声气体传感装置。它由光源(1)和其光路(2)上的管状声学谐振腔(6),以及置于管状声学谐振腔(6)侧开口处的光声气体传感器,与光声气体传感器配接的调制解调部件组成,特别是管状声学谐振腔(6)的管长为20~150mm、管内径为3~10mm,管状声学谐振腔(6)侧的开口为与其相连通的小孔(4),其孔深为1.5~2.5mm、孔直径为1.5~2.5mm,光声气体传感器为聚偏氟乙烯压电薄膜(5),其膜平面与小孔(4)端平面的间距为0.1~3mm、输出端经前置放大器(7)与调制解调部件的锁相放大器(8)的输入端电连接。它具有结构简单、较宽的响应带宽和工作稳定的特点,可广泛地用于探测和确定气体浓度或化学成分。

The invention discloses a photoacoustic gas sensing device based on polyvinylidene fluoride piezoelectric film. It consists of a light source (1) and a tubular acoustic resonant cavity (6) on its optical path (2), and a photoacoustic gas sensor placed at the side opening of the tubular acoustic resonant cavity (6). Demodulation components, especially the pipe length of the tubular acoustic resonant cavity (6) is 20-150 mm, the inner diameter of the tube is 3-10 mm, the opening on the side of the tubular acoustic resonant cavity (6) is a small hole (4) connected to it, The hole depth is 1.5-2.5mm, and the hole diameter is 1.5-2.5mm. The photoacoustic gas sensor is a polyvinylidene fluoride piezoelectric film (5), and the distance between the film plane and the end plane of the small hole (4) is 0.1-3mm , the output terminal is electrically connected to the input terminal of the lock-in amplifier (8) of the modulation and demodulation part through the preamplifier (7). It has the characteristics of simple structure, wide response bandwidth and stable operation, and can be widely used to detect and determine gas concentration or chemical composition.

Description

基于聚偏氟乙烯压电薄膜的光声气体传感装置Photoacoustic gas sensing device based on polyvinylidene fluoride piezoelectric film

技术领域 technical field

本发明涉及一种光声气体传感装置,尤其是一种基于聚偏氟乙烯压电薄膜的光声气体传感装置。  The invention relates to a photoacoustic gas sensing device, in particular to a photoacoustic gas sensing device based on polyvinylidene fluoride piezoelectric film. the

背景技术 Background technique

探测和确定气体浓度或化学成分在环境监测、气候、农业、安全、医学诊断以及工业等领域有着广泛的应用需求。随着激光技术、弱信号检测技术的发展,光声光谱技术也得到了快速的发展,而且光声光谱技术被认为是一种零背景、高灵敏度、高选择性的光谱技术。  Detecting and determining the concentration or chemical composition of gases has a wide range of applications in environmental monitoring, climate, agriculture, security, medical diagnostics, and industry. With the development of laser technology and weak signal detection technology, photoacoustic spectroscopy technology has also been developed rapidly, and photoacoustic spectroscopy technology is considered to be a spectral technology with zero background, high sensitivity and high selectivity. the

光声光谱是与基于比尔-朗伯(Beer-Lambert)吸收定律的传统吸收光谱不同的独特光谱技术,是基于光声效应的一种光谱技术,探测的是被样品吸收的光能量而不是透射光强。当处于分子吸收波段的光源照射到样品上时,样品分子吸收光能量而跃迁到激发态,处于激发态的分子通过碰撞弛豫回到基态,同时吸收的光能量转化为分子的内能,并导致分子的局部温度升高。所以当照射到样品分子上的光受到调制时,分子的局部温度就产生周期性的变化,从而产生周期性的压力变化,即声波。当人们用麦克风等声传感器记录声信号随光源波长的关系,就得到了光声光谱信号。与一般的基于比尔-朗伯(Beer-Lambert)吸收定律的传统吸收光谱技术相比,光声光谱具有以下特点:一是光声光谱测量的是被分子吸收的光能量,因此光声光谱信号只与被分子吸收的光能量(而非透射光强或反射光强)相关,故无吸收就无信号,是一种零背景光谱技术;二是光声光谱信号用声传感器探测,因此探测器没有波长依赖特性;三是光声光谱具有线性度好、响应范围宽的特点,理论上一个校准点就足以体现传感器响应特性;四是光声光谱具有灵敏度高,系统体积小,便于发展成便携式气体传感器的特点。鉴于光声光谱的这些特点,除了基于麦克风的传统光声光谱外,新的光声光谱技术不断出现。如于2012年4月25日公告的中国发明专利说明书CN101813621B中记载的一种“基于声谐振腔的石英音叉增强型光声光谱气体传感装置”。该气体传感装置由激 光光路上的聚焦透镜、腔轴线与光路同轴的管状声谐振腔和置于声谐振腔侧开口狭缝处的石英音叉,以及与激光源、石英音叉配接的电路组成。这种使用石英音叉的气体传感装置虽有着抗干扰能力强的特点,却因石英音叉的响应带宽一般小于5Hz,而对激光源的调制频率的精度要求很高,偏差应小于0.1Hz,当探测的环境条件——温度、载气成分等发生改变时,需要对激光源的调制频率进行及时的校正,才能保证准确的信号输出之不足。  Photoacoustic spectroscopy is a unique spectroscopic technique that is different from traditional absorption spectroscopy based on the Beer-Lambert absorption law. It is a spectroscopic technique based on the photoacoustic effect. light intensity. When a light source in the molecular absorption band irradiates the sample, the sample molecules absorb light energy and transition to an excited state, and the molecules in the excited state return to the ground state through collision relaxation, and the absorbed light energy is converted into the internal energy of the molecule, and This results in an increase in the local temperature of the molecule. So when the light irradiated on the sample molecules is modulated, the local temperature of the molecules changes periodically, thus generating periodic pressure changes, namely sound waves. When people use an acoustic sensor such as a microphone to record the relationship between the acoustic signal and the wavelength of the light source, the photoacoustic spectral signal is obtained. Compared with the general traditional absorption spectroscopy technology based on the Beer-Lambert (Beer-Lambert) absorption law, photoacoustic spectroscopy has the following characteristics: First, photoacoustic spectroscopy measures the light energy absorbed by molecules, so photoacoustic spectroscopy signals It is only related to the light energy absorbed by the molecule (rather than the transmitted light intensity or reflected light intensity), so there is no signal without absorption. There is no wavelength-dependent characteristic; third, photoacoustic spectroscopy has the characteristics of good linearity and wide response range, and theoretically one calibration point is enough to reflect the sensor response characteristics; fourth, photoacoustic spectroscopy has high sensitivity and small system size, which is easy to develop into a portable Features of gas sensors. In view of these characteristics of photoacoustic spectroscopy, in addition to traditional microphone-based photoacoustic spectroscopy, new photoacoustic spectroscopy techniques continue to emerge. For example, a "quartz tuning fork enhanced photoacoustic spectroscopy gas sensing device based on an acoustic resonant cavity" is described in the Chinese invention patent specification CN101813621B published on April 25, 2012. The gas sensing device consists of a focusing lens on the laser optical path, a tubular acoustic resonant cavity whose cavity axis is coaxial with the optical path, a quartz tuning fork placed at the side opening slit of the acoustic resonant cavity, and a laser source and a quartz tuning fork. Circuit composition. Although this gas sensing device using a quartz tuning fork has the characteristics of strong anti-interference ability, because the response bandwidth of the quartz tuning fork is generally less than 5Hz, and the accuracy of the modulation frequency of the laser source is very high, the deviation should be less than 0.1Hz. When the environmental conditions of the detection - temperature, carrier gas composition, etc. change, the modulation frequency of the laser source needs to be corrected in time to ensure accurate signal output. the

发明内容 Contents of the invention

本发明要解决的技术问题为克服现有技术中的不足之处,提供一种结构简单,具有较宽响应带宽的基于聚偏氟乙烯压电薄膜的光声气体传感装置。  The technical problem to be solved by the present invention is to overcome the deficiencies in the prior art and provide a photoacoustic gas sensing device based on polyvinylidene fluoride piezoelectric film with simple structure and wide response bandwidth. the

为解决本发明的技术问题,所采用的技术方案为:基于聚偏氟乙烯压电薄膜的光声气体传感装置由光源和其光路上的管状声学谐振腔,以及置于管状声学谐振腔侧开口处的光声气体传感器,与光声气体传感器配接的调制解调部件组成,特别是,  In order to solve the technical problem of the present invention, the adopted technical scheme is: the photoacoustic gas sensing device based on the polyvinylidene fluoride piezoelectric film consists of a light source and a tubular acoustic resonant cavity on its optical path, and a tube-shaped acoustic resonant cavity placed on the side of the tubular acoustic resonant cavity. The photoacoustic gas sensor at the opening is composed of modulation and demodulation components matched with the photoacoustic gas sensor, especially,

所述管状声学谐振腔的管长为20~150mm、管内径为3~10mm;  The tube length of the tubular acoustic resonant cavity is 20-150 mm, and the inner diameter of the tube is 3-10 mm;

所述管状声学谐振腔侧的开口为与其相连通的小孔,其孔深为1.5~2.5mm、孔直径为1.5~2.5mm;  The opening on the side of the tubular acoustic resonator is a small hole communicating with it, the hole depth is 1.5-2.5mm, and the hole diameter is 1.5-2.5mm;

所述光声气体传感器为聚偏氟乙烯压电薄膜,所述聚偏氟乙烯压电薄膜的膜平面与小孔端平面的间距为0.1~3mm,其输出端经前置放大器与所述调制解调部件的锁相放大器的输入端电连接。  The photoacoustic gas sensor is a polyvinylidene fluoride piezoelectric film, the distance between the film plane of the polyvinylidene fluoride piezoelectric film and the hole end plane is 0.1-3 mm, and its output terminal is connected to the modulated The input terminal of the lock-in amplifier of the demodulation part is electrically connected. the

作为基于聚偏氟乙烯压电薄膜的光声气体传感装置的进一步改进:  As a further improvement of the photoacoustic gas sensing device based on polyvinylidene fluoride piezoelectric film:

所述的光源与管状声学谐振腔之间的光路上置有其焦点位于管状声学谐振腔中点的聚焦透镜。  A focusing lens whose focal point is located at the midpoint of the tubular acoustic resonant cavity is placed on the optical path between the light source and the tubular acoustic resonant cavity. the

所述的光源为激光器,其输出的波长为待测气体的光吸收波长。  The light source is a laser, and its output wavelength is the light absorption wavelength of the gas to be measured. the

所述的管状声学谐振腔的管轴线与光路的光轴同轴。  The tube axis of the tubular acoustic resonant cavity is coaxial with the optical axis of the optical path. the

所述的小孔位于管状声学谐振腔的中点,且与其相垂直连接。  The small hole is located at the midpoint of the tubular acoustic resonant cavity and is vertically connected to it. the

所述的聚偏氟乙烯压电薄膜的膜长为20~30mm、膜宽为9~19mm、膜厚为0.1~0.3mm。  The film length of the polyvinylidene fluoride piezoelectric film is 20-30 mm, the film width is 9-19 mm, and the film thickness is 0.1-0.3 mm. the

所述的调制解调部件由电连接的锁相放大器和函数发生器组成,其中,函数发生器的输出端分别与光源的电源控制端、锁相放大器的输入端电连接。  The modulation and demodulation part is composed of an electrically connected lock-in amplifier and a function generator, wherein the output end of the function generator is respectively electrically connected to the power control end of the light source and the input end of the lock-in amplifier. the

所述的调制解调部件由电连接的锁相放大器和斩波器组成,其中,斩波器的光阑位于光源与管状声学谐振腔之间的光路上,其控制单元的输出端分别与光阑驱动电机、锁相放大器的输入端电连接。  The modulation and demodulation part is composed of an electrically connected lock-in amplifier and a chopper, wherein the aperture of the chopper is located on the optical path between the light source and the tubular acoustic resonant cavity, and the output ends of the control unit are respectively connected to the optical The input terminals of the drive motor and the lock-in amplifier are electrically connected. the

相对于现有技术的有益效果是:  The beneficial effect relative to prior art is:

其一,管状声学谐振腔的构造,即其管长、管内径和小孔的孔深、孔径的确定,使其于常压大气环境下具备了极佳的谐振效果,既为实现高探测灵敏度奠定了基础,也使其结构简单、工作稳定,易于调制解调部件调制信号频率的确定。  First, the structure of the tubular acoustic resonant cavity, that is, the length of the tube, the inner diameter of the tube and the depth and diameter of the small hole, make it have an excellent resonance effect in the normal pressure atmospheric environment, which is not only to achieve high detection sensitivity The foundation is laid, the structure is simple, the work is stable, and the modulation and demodulation components are easy to determine the modulation signal frequency. the

其二,采用聚偏氟乙烯压电薄膜作为声传感器来探测光声吸收,因其具有很宽的频率响应特性,能在0.01Hz~100MHz的频率范围内线性输出,故不仅使本发明适用的范围相当的宽泛,还对光源调制频率的精度无任何要求,大大地拓展了应用的场合和完全能满足特定场合的应用需求,更有着调制解调部件调制信号频率的调整和使用均十分方便的特点,使其可广泛地用于探测气体的成分或含量。加之聚偏氟乙烯压电薄膜还有着柔韧性好、耐摔性强、防水性佳和化学稳定性高的优点,且价格低廉,大大地降低了本发明的制造、使用和维护的成本。  Second, polyvinylidene fluoride piezoelectric film is used as an acoustic sensor to detect photoacoustic absorption, because it has a wide frequency response characteristic and can be linearly output in the frequency range of 0.01Hz to 100MHz, so it not only makes the present invention applicable The range is quite wide, and there is no requirement for the accuracy of the light source modulation frequency, which greatly expands the application occasions and can fully meet the application requirements of specific occasions. It is also very convenient to adjust and use the modulation signal frequency of the modulation and demodulation components. Features, so that it can be widely used to detect the composition or content of gas. In addition, the polyvinylidene fluoride piezoelectric film has the advantages of good flexibility, strong drop resistance, good water resistance and high chemical stability, and the price is low, which greatly reduces the cost of manufacture, use and maintenance of the present invention. the

作为有益效果的进一步体现:  As a further manifestation of beneficial effects:

一是聚焦透镜的设置,利于探测灵敏度的进一步提高。  One is the setting of the focusing lens, which is conducive to the further improvement of the detection sensitivity. the

二是优选其输出波长为待测气体的光吸收波长的激光器作为光源,易于提升探测的灵敏度。  The second is to choose a laser whose output wavelength is the light absorption wavelength of the gas to be measured as the light source, which is easy to improve the detection sensitivity. the

三是选择聚偏氟乙烯压电薄膜的膜长为20~30mm、膜宽为9~19mm、膜厚为0.1~0.3mm,便于其与小孔的优化匹配。  The third is to choose the polyvinylidene fluoride piezoelectric film with a film length of 20-30 mm, a film width of 9-19 mm, and a film thickness of 0.1-0.3 mm, so as to facilitate its optimal matching with the small hole. the

附图说明 Description of drawings

下面结合附图对本发明的优选方式作进一步详细的描述。  The preferred modes of the present invention will be further described in detail below in conjunction with the accompanying drawings. the

图1是本发明的一种基本结构示意图。  Fig. 1 is a kind of basic structure schematic diagram of the present invention. the

图2是本发明中的调制器选用斩波器时的一种基本结构示意图。  Fig. 2 is a schematic diagram of a basic structure when a chopper is selected as the modulator in the present invention. the

图3是本发明中使用的聚偏氟乙烯压电薄膜的一种基本形貌图。  Fig. 3 is a basic topographic view of the polyvinylidene fluoride piezoelectric film used in the present invention. the

图4是使用本发明测量大气中的水汽时,得到的信号谱图。  Fig. 4 is a signal spectrogram obtained when the present invention is used to measure water vapor in the atmosphere. the

具体实施方式 Detailed ways

参见图1、图3和图4,基于聚偏氟乙烯压电薄膜的光声气体传感装置的构成如下:  Referring to Figure 1, Figure 3 and Figure 4, the composition of the photoacoustic gas sensing device based on polyvinylidene fluoride piezoelectric film is as follows:

光源1的光路2上依次置有聚焦透镜3、管状声学谐振腔6;其中,  The optical path 2 of the light source 1 is provided with a focusing lens 3 and a tubular acoustic resonant cavity 6 in sequence; wherein,

光源1优选为激光器,其输出的波长为待测气体的光吸收波长。  The light source 1 is preferably a laser, and its output wavelength is the light absorption wavelength of the gas to be measured. the

聚焦透镜3的焦点位于管状声学谐振腔6的中点。  The focal point of the focusing lens 3 is located at the midpoint of the tubular acoustic resonant cavity 6 . the

管状声学谐振腔6的管长优选为30(可为20~150)mm、管内径优选为5(可为3~10)mm,且其管轴线与光路2的光轴同轴。其在常压大气环境下的工作频率约为5800Hz。  The tube length of the tubular acoustic resonator 6 is preferably 30 (can be 20-150) mm, the inner diameter of the tube is preferably 5 (can be 3-10) mm, and the tube axis is coaxial with the optical axis of the optical path 2 . Its working frequency is about 5800Hz under normal pressure atmospheric environment. the

管状声学谐振腔6的中点置有与其相垂直连接的小孔4,小孔4的孔深优选为2(可为1.5~2.5mm)、孔直径优选为2(可为1.5~2.5)mm。  The midpoint of the tubular acoustic resonant cavity 6 is provided with a small hole 4 vertically connected to it. The hole depth of the small hole 4 is preferably 2 (can be 1.5-2.5 mm), and the hole diameter is preferably 2 (can be 1.5-2.5) mm. . the

小孔4上附有聚偏氟乙烯压电薄膜5,其优选为美国Measurement Specialties公司生产的型号为LDT0、膜长为25(可为20~30)mm、膜宽为14(可为9~19mm)、膜厚为0.2(可为0.1~0.3)mm的成品。该聚偏氟乙烯压电薄膜5的膜平面与小孔4端平面的间距优选为1(可为0.1~3)mm,其输出端经前置放大器7与调制解调部件的锁相放大器8的输入端电连接。  A polyvinylidene fluoride piezoelectric film 5 is attached to the small hole 4, which is preferably the model LDT0 produced by the American Measurement Specialties company, the film length is 25 (can be 20-30) mm, and the film width is 14 (can be 9-30) mm. 19mm), film thickness of 0.2 (can be 0.1 ~ 0.3) mm finished product. The distance between the film plane of the polyvinylidene fluoride piezoelectric film 5 and the end plane of the small hole 4 is preferably 1 (may be 0.1 to 3) mm, and its output terminal passes through the preamplifier 7 and the lock-in amplifier 8 of the modulation and demodulation component. The input terminals are electrically connected. the

调制解调部件由电连接的锁相放大器8和函数发生器9组成,其中,函数发生器9的输出端分别与光源1的电源控制端、锁相放大器8的输入端电连接。  The modulation and demodulation part is composed of an electrically connected lock-in amplifier 8 and a function generator 9, wherein the output terminal of the function generator 9 is electrically connected to the power control terminal of the light source 1 and the input terminal of the lock-in amplifier 8 respectively. the

调制解调部件也可选用如图2所示的结构。此时,调制解调部件由电连接的锁相放大器8和斩波器10组成,其中,斩波器10的光阑位于光源1与管状声学谐振腔6之间的光路2上,其控制单元的输出端分别与光阑驱动电机、锁相放大器8的输入端电连接。  Modulation and demodulation components can also choose the structure shown in Figure 2. At this time, the modulation and demodulation components are composed of an electrically connected lock-in amplifier 8 and a chopper 10, wherein the diaphragm of the chopper 10 is located on the optical path 2 between the light source 1 and the tubular acoustic resonant cavity 6, and its control unit The output ends of the aperture drive motor and the input end of the lock-in amplifier 8 are electrically connected respectively. the

使用木发明测量大气中的水汽时,当已被调制的激光波大气中的水收后,将产生光声信号并激发聚偏氟乙烯压电薄膜5振动,从而使其产电电流信号并被送往锁相放大器8,由锁相放大器8解调后得到水汽的吸收信号,即获得了如图4所示的大气中的水汽的信号谱图。  When using the invention to measure water vapor in the atmosphere, when the modulated laser wave absorbs the water in the atmosphere, a photoacoustic signal will be generated and the PVDF piezoelectric film 5 will be excited to vibrate, so that it will generate an electric current signal and be detected Sent to the lock-in amplifier 8, after being demodulated by the lock-in amplifier 8, the absorption signal of the water vapor is obtained, that is, the signal spectrum of the water vapor in the atmosphere as shown in FIG. 4 is obtained. the

显然,本领域的技术人员可以对本发明的基于聚偏氟乙烯压电薄膜的光声气体传感装置进行各种改动和变型而不脱离本发明的精神和范围。这样,倘若对本发明的这些修改和变型属于本发明权利要求及其等同技术的范围之 内,则本发明也意图包含这些改动和变型在内。  Obviously, those skilled in the art can make various changes and modifications to the photoacoustic gas sensing device based on the polyvinylidene fluoride piezoelectric film of the present invention without departing from the spirit and scope of the present invention. In this way, if these modifications and variations to the present invention belong to the scope of the claims of the present invention and equivalent technologies thereof, the present invention is also intended to include these modifications and variations. the

Claims (8)

1. The utility model provides a photoacoustic gas sensing device based on polyvinylidene fluoride piezoelectric film, by tubular acoustic resonant cavity (6) on light source (1) and its light path (2) to and arrange the photoacoustic gas sensor of tubular acoustic resonant cavity (6) side opening part in, the modem part that connects with photoacoustic gas sensor constitutes its characterized in that:
the pipe length of the tubular acoustic resonant cavity (6) is 20-150 mm, and the inner diameter of the pipe is 3-10 mm;
the opening at the side of the tubular acoustic resonant cavity (6) is a small hole (4) communicated with the tubular acoustic resonant cavity, the hole depth is 1.5-2.5 mm, and the hole diameter is 1.5-2.5 mm;
the photoacoustic gas sensor is a polyvinylidene fluoride piezoelectric film (5), the distance between the film plane of the polyvinylidene fluoride piezoelectric film (5) and the end plane of the small hole (4) is 0.1-3 mm, and the output end of the photoacoustic gas sensor is electrically connected with the input end of a phase-locked amplifier (8) of the modulation and demodulation component through a preamplifier (7).
2. A photo-acoustic gas sensing device based on polyvinylidene fluoride piezoelectric film according to claim 1, wherein a focusing lens (3) with its focus at the midpoint of the tubular acoustic resonator (6) is disposed on the optical path (2) between the light source (1) and the tubular acoustic resonator (6).
3. A photo acoustic gas sensor device based on polyvinylidene fluoride piezoelectric film according to claim 2, characterized in that the light source (1) is a laser outputting a wavelength of light absorption of the gas to be measured.
4. A photo-acoustic gas sensing device based on polyvinylidene fluoride piezoelectric film according to claim 3, characterized in that the tube axis of the tubular acoustic resonator (6) is coaxial with the optical axis of the optical path (2).
5. A photo-acoustic gas sensing device based on polyvinylidene fluoride piezoelectric film according to claim 4, characterized in that the small hole (4) is located at the midpoint of the tubular acoustic resonator (6) and is connected to it perpendicularly.
6. A photoacoustic gas sensing device based on polyvinylidene fluoride piezoelectric film as set forth in claim 1, wherein the polyvinylidene fluoride piezoelectric film (5) has a film length of 20 to 30mm, a film width of 9 to 19mm and a film thickness of 0.1 to 0.3 mm.
7. A photo-acoustic gas sensing device based on polyvinylidene fluoride piezoelectric film according to claim 1, wherein the modem part is composed of a phase-locked amplifier (8) and a function generator (9) which are electrically connected, wherein the output end of the function generator (9) is electrically connected with the power control end of the light source (1) and the input end of the phase-locked amplifier (8) respectively.
8. A photoacoustic gas sensing device based on polyvinylidene fluoride piezoelectric film as in claim 1, wherein the modem means consists of electrically connected lock-in amplifier (8) and chopper (10), wherein the diaphragm of chopper (10) is located on the optical path (2) between the light source (1) and the tubular acoustic resonator (6), and the output of its control unit is electrically connected to the input of the diaphragm driving motor and lock-in amplifier (8), respectively.
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