CN115575491A - Self powered gas sensing device, system and method - Google Patents
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Abstract
公开了一种自供能气体传感系统、装置和方法,用于识别待测气体环境中的气体的属性。自供能气体传感系统包括:自供能气体传感装置,包括:能量收集器,被配置为获取机械能,并将所述机械能转换为电能;击穿放电器,被设置在所述待测气体环境中,所述击穿放电器被配置为获取所述电能,其中所述电能使得所述击穿放电器在待测气体环境中进行击穿放电,击穿放电所产生的电流导致电磁波信号的发射,并且其中,所述电磁波信号携带与所述待测气体环境中的气体的属性相关联的信息;以及气体属性识别装置,被配置为从所述自供能气体传感装置接收所述电磁波信号,并基于所述电磁波信号识别所述待测气体环境中的气体的属性。
A self-powered gas sensing system, apparatus and method for identifying properties of gases in a gaseous environment to be measured are disclosed. The self-powered gas sensing system includes: a self-powered gas sensing device, including: an energy harvester configured to obtain mechanical energy and convert the mechanical energy into electrical energy; a breakdown arrestor arranged in the gas environment to be measured In the above, the breakdown arrester is configured to obtain the electric energy, wherein the electric energy causes the breakdown arrester to perform breakdown discharge in the gas environment to be tested, and the current generated by the breakdown discharge leads to the emission of electromagnetic wave signals , and wherein the electromagnetic wave signal carries information associated with a property of the gas in the gas environment to be measured; and a gas property identification device configured to receive the electromagnetic wave signal from the self-powered gas sensing device, And identifying the property of the gas in the gas environment to be measured based on the electromagnetic wave signal.
Description
技术领域technical field
本公开涉及传感技术领域,并且更具体地,涉及一种自供能气体传感装 置、系统和方法。The present disclosure relates to the field of sensing technology, and more particularly, to a self-powered gas sensing device, system and method.
背景技术Background technique
气体传感器在工业排气、室内环境检测等领域中扮演重要的角色,具有 广阔的应用背景。传统的气体传感器通常依赖于外部电源提供能量,例如, 催化燃烧式气体传感器、半导体式气体传感器、热导式气体传感器、红外气 体传感器等等。需要依靠外部电源供电大大地限制了气体传感器的应用范围。 即使现在已经出现了无线传能,但是这种供电方式受限于有限的传输距离, 并且仍然存在需要外部电源给能量发射部分供电的需求。Gas sensors play an important role in industrial exhaust, indoor environment detection and other fields, and have a broad application background. Traditional gas sensors usually rely on external power sources to provide energy, such as catalytic combustion gas sensors, semiconductor gas sensors, thermal conductivity gas sensors, infrared gas sensors, and so on. The need to rely on an external power supply greatly limits the application range of the gas sensor. Even though wireless energy transmission has appeared now, this power supply method is limited by a limited transmission distance, and there is still a demand for an external power supply to power the energy transmitting part.
自供能技术是一种无需外加电源,收集周围环境中其他形式能量(如太 阳能、风能、机械能、热能等)并将其转换成电能,为电子设备提供安全、 稳定、高效的电能供给技术。但是,这种基于自供能技术的供电方式由于能 量收集器具有的不同阻抗和输出特性,通常需要引入能量管理电路,这样又 引入额外的能量需求,并增大了整个系统的体积。Self-powered technology is a technology that collects other forms of energy (such as solar energy, wind energy, mechanical energy, heat energy, etc.) However, due to the different impedance and output characteristics of energy harvesters, this power supply method based on self-energy technology usually requires the introduction of energy management circuits, which introduces additional energy requirements and increases the size of the entire system.
同时,现有的气体传感器还往往具有检测范围的局限性并具有其他缺陷, 例如催化燃烧式气体传感器仅限于测试可燃气体并且有引燃爆炸的危险,半 导体式气体传感器受背景气体干扰较大、易受温度影响,热导式气体传感器 受温度影响明显,检测精度差,灵敏度低,以及红外气体传感器成本高、系 统复杂、仅限于测试吸收红外线辐射的气体等等。此外,许多气体传感器不 能与后续的传感器数据分析装置相隔太远(例如,不能超过1m),因为例如 如果需要导线等传输介质来传输传感信号,过长的导线会存在过大阻抗因此 影响传感信号的有效性,且增大系统体积,但是某些应用场景由于例如空间 限制或者数据分析装置不宜移动而无法将气体传感器和传感器数据分析装置 足够近地设置。At the same time, existing gas sensors often have limitations in detection range and other defects. For example, catalytic combustion gas sensors are limited to testing combustible gases and have the risk of ignition and explosion. Semiconductor gas sensors are greatly interfered by background gas, Susceptible to temperature, thermal conductivity gas sensors are significantly affected by temperature, poor detection accuracy, low sensitivity, and infrared gas sensors have high cost, complex systems, and are limited to testing gases that absorb infrared radiation, etc. In addition, many gas sensors cannot be separated from the subsequent sensor data analysis device too far (for example, not more than 1m), because for example, if a transmission medium such as a wire is required to transmit the sensing signal, a too long wire will have too much impedance and thus affect the transmission. The effectiveness of the sensing signal and increase the volume of the system, but in some application scenarios, the gas sensor and the sensor data analysis device cannot be placed close enough due to space constraints or the data analysis device is not suitable for movement.
为此,亟需一种能够集能量收集转换功能和检测气体功能于一体、体积 小、能够适用于安全地感测各种类型的气体、感测精度高、且传感信号具有 较远传输距离的自供能气体传感器。For this reason, there is an urgent need for a sensor that can integrate energy harvesting and conversion functions and gas detection functions, is small in size, can be used to safely sense various types of gases, has high sensing accuracy, and has a long transmission distance for sensing signals. self-powered gas sensor.
发明内容Contents of the invention
根据本公开的一方面,提供了一种自供能气体传感系统,用于识别待测 气体环境中的气体的属性,包括:自供能气体传感装置,包括:能量收集器, 被配置为获取机械能,并将所述机械能转换为电能;击穿放电器,被设置在 所述待测气体环境中,所述击穿放电器被配置为获取所述电能,其中所述电 能使得所述击穿放电器在待测气体环境中进行击穿放电,击穿放电所产生的 电流导致电磁波信号的发射,并且其中,所述电磁波信号携带与所述待测气 体环境中的气体的属性相关联的信息;以及气体属性识别装置,被配置为从所述自供能气体传感装置接收所述电磁波信号,并基于所述电磁波信号识别 所述待测气体环境中的气体的属性。According to an aspect of the present disclosure, there is provided a self-powered gas sensing system for identifying properties of a gas in a gas environment to be measured, comprising: a self-powered gas sensing device including: an energy harvester configured to acquire mechanical energy, and convert the mechanical energy into electrical energy; a breakdown arrester is arranged in the gas environment to be measured, and the breakdown arrester is configured to obtain the electrical energy, wherein the electrical energy causes the breakdown The discharger performs a breakdown discharge in the gas environment to be tested, and the current generated by the breakdown discharge causes the emission of an electromagnetic wave signal, and wherein the electromagnetic wave signal carries information associated with the properties of the gas in the gas environment to be tested and a gas attribute identification device configured to receive the electromagnetic wave signal from the self-powered gas sensing device, and identify an attribute of the gas in the gas environment to be measured based on the electromagnetic wave signal.
根据本公开的实施例,其中,所述击穿放电器包括经由所述待测气体环 境中的气体绝缘隔离的第一电极和第二电极,并且其中,所述第一电极和第 二电极具有相对的放电尖端,所述相对的放电尖端之间具有放电间隙,所述 电能在所述第一电极和第二电极的尖端之间形成电场,并且所述电场使得在 第一电极和第二电极的放电尖端的放电间隙之间击穿所述待测气体环境中的 气体,以进行击穿放电。According to an embodiment of the present disclosure, wherein the breakdown arrestor includes a first electrode and a second electrode separated by gas insulation in the gas environment to be measured, and wherein the first electrode and the second electrode have Opposite discharge tips, there is a discharge gap between the opposite discharge tips, the electric energy forms an electric field between the tips of the first electrode and the second electrode, and the electric field makes the electric field between the first electrode and the second electrode The gas in the gas environment to be measured is broken down between the discharge gaps of the discharge tips to perform a breakdown discharge.
根据本公开的实施例,其中所述气体的属性包括以下至少之一:气体成 分、气体浓度、气体气压。According to an embodiment of the present disclosure, the properties of the gas include at least one of the following: gas composition, gas concentration, and gas pressure.
根据本公开的实施例,其中,所述气体属性识别装置包括:信号接收单 元,被配置为从所述自供能气体传感装置接收所述电磁波信号,并将所述电 磁波信号转换为预定电参数的时序信号;以及识别单元,被配置为基于所述 预定电参数的时序信号识别所述待测气体环境中的气体的属性。According to an embodiment of the present disclosure, wherein the gas property identification device includes: a signal receiving unit configured to receive the electromagnetic wave signal from the self-powered gas sensing device, and convert the electromagnetic wave signal into a predetermined electrical parameter and an identification unit configured to identify the property of the gas in the gas environment to be measured based on the time series signal of the predetermined electrical parameter.
根据本公开的实施例,其中,所述气体属性识别装置还包括:信号处理 单元,被配置为对所述预定电参数的时序信号进行信号处理,得到经处理信 号,其中,所述识别单元基于所述经处理信号识别所述待测气体环境中的气 体的属性;其中,所述信号处理包括以下操作中的至少一项:去除噪声信号 或截取有效信号;以及提取频谱信号。According to an embodiment of the present disclosure, wherein the gas property identification device further includes: a signal processing unit configured to perform signal processing on the time series signal of the predetermined electrical parameter to obtain a processed signal, wherein the identification unit is based on The processed signal identifies the properties of the gas in the gas environment to be measured; wherein the signal processing includes at least one of the following operations: removing noise signals or intercepting effective signals; and extracting spectrum signals.
根据本公开的实施例,其中,所述识别单元包括机器学习模型,所述机 器学习模型经训练能够针对经处理信号而生成指示所述待测气体环境中的气 体的属性的识别结果,其中,所述机器学习模型在训练集上训练得到经训练 机器学习模型,并且所述训练集包括多个经处理信号以及所述多个经处理信 号各自对应的气体属性的真实标签。According to an embodiment of the present disclosure, wherein the identification unit includes a machine learning model, the machine learning model is trained to generate an identification result indicating the property of the gas in the gas environment to be measured for the processed signal, wherein, The machine learning model is trained on a training set to obtain a trained machine learning model, and the training set includes a plurality of processed signals and real labels of gas properties corresponding to each of the plurality of processed signals.
根据本公开的实施例,其中,所述训练集通过以下方式得到:选择具有 不同的气体属性的第一数量的参考气体环境;针对每种参考气体环境得到第 二数量的经处理信号;针对每种参考气体环境,将所述第二数量的经处理信 号和各自对应的气体属性的真实标签作为训练子集;以及将针对所有参考气 体环境的训练子集共同作为训练集。According to an embodiment of the present disclosure, wherein the training set is obtained by: selecting a first number of reference gas environments with different gas properties; obtaining a second number of processed signals for each reference gas environment; a reference gas environment, using the second number of processed signals and the true labels of their corresponding gas properties as a training subset; and using the training subsets for all reference gas environments together as a training set.
根据本公开的实施例,其中,针对每种参考气体环境的第二数量的经处 理信号通过以下方式得到:针对所述参考气体环境,由放置在充满所述参考 气体环境中的气体的密闭气室中的所述击穿放电器,基于从所述能量收集器 获取的电能而在所述参考气体环境中进行击穿放电,其中所述击穿放电所产 生的电流导致电磁波信号的发射;获取所述电磁波信号,并将所述电磁波信 号转换为预定电参数的第二数量的时序信号;以及对预定电参数的每个时序 信号进行处理,得到所述第二数量的经处理信号。According to an embodiment of the present disclosure, wherein the second quantity of processed signals for each reference gas environment is obtained by: for the reference gas environment, an airtight gas placed in the gas filled in the reference gas environment The breakdown arrester in the chamber, based on the electrical energy obtained from the energy harvester, performs a breakdown discharge in the reference gas environment, wherein the current generated by the breakdown discharge causes the emission of an electromagnetic wave signal; obtaining The electromagnetic wave signal, and converting the electromagnetic wave signal into a second number of time-series signals of predetermined electrical parameters; and processing each time-series signal of predetermined electrical parameters to obtain the second number of processed signals.
根据本公开的实施例,其中,所述训练集包括的经处理信号中的每一者 为时域信号,所述机器学习模型为双向长短时记忆循环神经网络(bi-LSTM) 模型,其中,所述机器学习模型通过以下方式训练:将所述训练集包括的每 个时域信号分别正向输入以及反向输入到所述bi-LSTM模型,以得到每个所 述时域信号对应的预测标签,并且基于每个预测标签和对应的时域信号的真 实标签的差异,通过误差反向传播法和梯度下降法来更新所述bi-LSTM模型 的模型参数,直至所述模型参数相对于所述训练集而收敛。According to an embodiment of the present disclosure, wherein each of the processed signals included in the training set is a time-domain signal, the machine learning model is a bidirectional long-short-term memory recurrent neural network (bi-LSTM) model, wherein, The machine learning model is trained in the following manner: each time domain signal included in the training set is input forward and reversely to the bi-LSTM model to obtain a prediction corresponding to each time domain signal label, and based on the difference between each predicted label and the real label of the corresponding time-domain signal, the model parameters of the bi-LSTM model are updated by the error backpropagation method and the gradient descent method until the model parameters are relative to the set Converge on the training set.
根据本公开的实施例,其中,所述训练集包括的经处理信号中的每一者 为频谱图像信号,所述机器学习模型为卷积神经网络(CNN)模型,其中, 所述机器学习模型通过以下方式训练:将所述训练集包括的每个频谱图像信 号输入到所述CNN模型,以得到每个所述频谱图像信号对应的预测标签,并 且基于每个预测标签和对应的频谱图像信号的真实标签的差异,通过误差反 向传播法和梯度下降法来更新所述CNN模型的模型参数,直至所述模型参数 相对于所述训练集而收敛。According to an embodiment of the present disclosure, wherein each of the processed signals included in the training set is a spectral image signal, the machine learning model is a convolutional neural network (CNN) model, wherein the machine learning model Training in the following manner: each spectral image signal included in the training set is input to the CNN model to obtain a prediction label corresponding to each spectral image signal, and based on each prediction label and the corresponding spectral image signal The difference of the true label, update the model parameters of the CNN model through the error backpropagation method and the gradient descent method, until the model parameters converge with respect to the training set.
根据本公开的另一方面,提供了自供能气体传感装置,包括:能量收集 器,被配置为获取机械能,并将所述机械能转换为电能;击穿放电器,被设 置在所述待测气体环境中,所述击穿放电器被配置为获取所述电能,其中所 述电能使得所述击穿放电器在待测气体环境中进行击穿放电,并且击穿放电 所产生的电流导致电磁波信号的发射,其中,所述电磁波信号携带与所述待 测气体环境中的气体的属性相关联的信息。According to another aspect of the present disclosure, a self-powered gas sensing device is provided, including: an energy harvester configured to harvest mechanical energy and convert the mechanical energy into electrical energy; In a gas environment, the breakdown arrester is configured to obtain the electrical energy, wherein the electrical energy causes the breakdown arrester to perform a breakdown discharge in the gas environment to be tested, and the current generated by the breakdown discharge causes an electromagnetic wave The emission of a signal, wherein the electromagnetic wave signal carries information associated with the property of the gas in the gas environment to be measured.
根据本公开的实施例,其中,所述击穿放电器包括经由所述待测气体环 境中的气体绝缘隔离的第一电极和第二电极,并且其中,所述第一电极和第 二电极具有相对的放电尖端,放电尖端之间具有放电间隙,所述电能在所述 第一电极和第二电极的尖端之间形成电场,并且所述电场在第一电极和第二 电极的放电尖端的放电间隙之间击穿所述待测气体环境中的气体,以进行击 穿放电。According to an embodiment of the present disclosure, wherein the breakdown arrestor includes a first electrode and a second electrode separated by gas insulation in the gas environment to be measured, and wherein the first electrode and the second electrode have Opposite discharge tips, there is a discharge gap between the discharge tips, the electric energy forms an electric field between the tips of the first electrode and the second electrode, and the discharge of the electric field at the discharge tips of the first electrode and the second electrode The gas in the gas environment to be measured is broken down between the gaps to perform breakdown discharge.
根据本公开的又一方面,提供了一种自供能气体传感方法,用于识别待 测气体环境中的气体的属性,包括:将击穿放电器放置在所述待测气体环境 中;利用能量收集器获取机械能,并将所述机械能转换为电能;利用所述击 穿放电器获取所述电能,其中所述电能使得所述击穿放电器在待测气体环境 中进行击穿放电,并且击穿放电所产生的电流导致电磁波信号的发射,并且 其中,所述电磁波信号携带与所述待测气体环境中的气体的属性相关联的信 息;以及利用气体属性识别装置基于所述电磁波信号,识别所述待测气体环境中的气体的属性。According to yet another aspect of the present disclosure, there is provided a self-powered gas sensing method for identifying properties of a gas in a gas environment to be tested, comprising: placing a breakdown arrestor in the gas environment to be tested; utilizing The energy harvester obtains mechanical energy and converts the mechanical energy into electrical energy; the electrical energy is obtained by using the breakdown arrester, wherein the electrical energy causes the breakdown arrester to perform breakdown discharge in the gas environment to be measured, and The current generated by the breakdown discharge causes the emission of an electromagnetic wave signal, and wherein the electromagnetic wave signal carries information associated with the properties of the gas in the gas environment to be measured; and using the gas property identification device based on the electromagnetic wave signal, Identifying properties of gases in the gas environment to be measured.
根据本公开的实施例,其中,利用气体属性识别装置基于所述电磁波信 号,识别所述待测气体环境中的气体的属性,包括:接收所述电磁波信号, 并将所述电磁波信号转换为预定电参数的时序信号;对所述预定电参数的时 序信号进行信号处理,得到经处理信号;以及基于所述经处理信号,识别所 述待测气体环境中的气体的属性。According to an embodiment of the present disclosure, wherein, using the gas attribute identification device to identify the attribute of the gas in the gas environment to be measured based on the electromagnetic wave signal includes: receiving the electromagnetic wave signal, and converting the electromagnetic wave signal into a predetermined A time-series signal of an electrical parameter; performing signal processing on the time-series signal of the predetermined electrical parameter to obtain a processed signal; and identifying the property of the gas in the gas environment to be measured based on the processed signal.
根据本公开的实施例,其中,所述气体属性识别装置包括机器学习模型, 所述自供能气体传感方法还包括:获取多个经处理信号以及所述多个经处理 信号各自对应的气体属性的真实标签,作为训练集;以及利用所述训练集训 练所述机器学习模型,使得经训练机器学习模型能够针对经处理信号而生成 指示所述待测气体环境中的气体的属性的识别结果。According to an embodiment of the present disclosure, wherein the gas property identification device includes a machine learning model, the self-powered gas sensing method further includes: acquiring a plurality of processed signals and gas properties corresponding to each of the plurality of processed signals as a training set; and using the training set to train the machine learning model, so that the trained machine learning model can generate a recognition result indicating the property of the gas in the gas environment under test for the processed signal.
根据本公开实施例的自供能气体传感装置、系统和方法,可以实现对自 供能气体传感装置所在气体环境的气体的属性,如气体成分、浓度及气压等 信息的识别,相比于目前的气体传感技术,可以实现对大多数气体的感测, 无需外部电源供能,产生的传感信号本身为无线信号从而不受信号传输线的 约束,更不需要附加的能量管理模块以及无线信号发射模块,体积小,并且 气体属性的识别准确性高,使得自供能气体传感系统具有更大的应用范围。According to the self-powered gas sensing device, system, and method of the embodiments of the present disclosure, the properties of the gas in the gas environment where the self-powered gas sensing device is located, such as gas composition, concentration, and air pressure, can be identified. The advanced gas sensing technology can realize the sensing of most gases without external power supply, and the generated sensing signal itself is a wireless signal so that it is not constrained by the signal transmission line, and does not require additional energy management modules and wireless signals The transmitter module has a small volume and high recognition accuracy of gas properties, so that the self-powered gas sensing system has a wider range of applications.
附图说明Description of drawings
为了更清楚地说明本公开实施例的技术方案,下面将对实施例的描述中 所需要使用的附图作简单的介绍。显而易见地,下面描述中的附图仅仅是本 公开的一些示例性实施例,对于本领域普通技术人员来说,在不付出创造性 劳动的前提下,还可以根据这些附图获得其它的附图。In order to more clearly illustrate the technical solutions of the embodiments of the present disclosure, the drawings that need to be used in the description of the embodiments will be briefly introduced below. Apparently, the drawings in the following description are only some exemplary embodiments of the present disclosure, and those skilled in the art can obtain other drawings according to these drawings without creative efforts.
图1示出了根据本公开实施例的自供能气体传感系统的示意结构框图。Fig. 1 shows a schematic structural block diagram of a self-powered gas sensing system according to an embodiment of the present disclosure.
图2示出了根据本公开实施例的自供能气体传感装置的示意结构框图。Fig. 2 shows a schematic structural block diagram of a self-powered gas sensing device according to an embodiment of the present disclosure.
图3A-3B示出了摩擦纳米发电机的示例结构。Figures 3A-3B illustrate example structures of triboelectric nanogenerators.
图4示出了图2所述的自供能气体传感装置的等效电路模型。FIG. 4 shows an equivalent circuit model of the self-powered gas sensing device described in FIG. 2 .
图5A示出了根据本公开实施例的气体属性识别装置的示意结构框图。Fig. 5A shows a schematic structural block diagram of a gas property identification device according to an embodiment of the present disclosure.
图5B示出了基于自供能气体传感装置得到第二数量的经处理信号的结 构示意图。Fig. 5B shows a schematic diagram of a structure for obtaining a second quantity of processed signals based on a self-powered gas sensing device.
图5C示出了针对10种参考气体环境得到的电压-时间的时间序列的示意 图。Figure 5C shows a schematic diagram of the voltage-time time series obtained for 10 reference gas environments.
图5D示出了针对每种参考气体环境得到多个经处理信号的流程图。Figure 5D shows a flow diagram for obtaining multiple processed signals for each reference gas environment.
图6示出了基于混淆矩阵示出自供能气体传感系统的有效性的示意图。Fig. 6 shows a schematic diagram illustrating the effectiveness of a self-powered gas sensing system based on a confusion matrix.
图7示出了根据本公开实施例的自供能气体传感方法的示意流程图。FIG. 7 shows a schematic flowchart of a self-powered gas sensing method according to an embodiment of the present disclosure.
图8示出了根据本公开实施例的可用于实现识别单元的计算设备的示意 结构框图。Fig. 8 shows a schematic structural block diagram of a computing device that can be used to implement an identification unit according to an embodiment of the present disclosure.
具体实施方式detailed description
以下对本发明的实施方式作详细说明。应该强调的是,下述说明仅仅是 示例性的,而不是为了限制本发明的范围及其应用。Embodiments of the present invention will be described in detail below. It should be emphasized that the following description is only exemplary and not intended to limit the scope of the invention and its application.
为了使得本公开的目的、技术方案和优点更为明显,下面将参照附图详 细描述根据本公开的示例实施例。显然,所描述的实施例仅仅是本公开的一 部分实施例,而不是本公开的全部实施例,应理解,本公开不受这里描述的 示例实施例的限制。In order to make the objects, technical solutions, and advantages of the present disclosure more apparent, exemplary embodiments according to the present disclosure will be described in detail below with reference to the accompanying drawings. Apparently, the described embodiments are only some of the embodiments of the present disclosure, rather than all the embodiments of the present disclosure, and it should be understood that the present disclosure is not limited by the exemplary embodiments described here.
在本说明书和附图中,具有基本上相同或相似步骤和元素用相同或相似 的附图标记来表示,且对这些步骤和元素的重复描述将被省略。术语“第一”、 “第二”仅用于描述目的,而不能理解为指示或暗示相对重要性或者隐含指 明所指示的技术特征的数量。由此,限定有“第一”、“第二”的特征可以明 示或者隐含地包括一个或发明实施例的描述中,“多个”的含义是两个或两个 以上,除非另有明确具体的限定。In the present specification and drawings, substantially the same or similar steps and elements are denoted by the same or similar reference numerals, and repeated descriptions of these steps and elements will be omitted. The terms "first" and "second" are used for descriptive purposes only, and should not be understood as indicating or implying relative importance or implicitly indicating the quantity of the indicated technical features. Therefore, the features defined as "first" and "second" may explicitly or implicitly include one or in the description of the embodiment of the invention, "plurality" means two or more, unless otherwise specified Specific limits.
图1示出了根据本公开实施例的一种自供能气体传感系统100的示意框 图。Fig. 1 shows a schematic block diagram of a self-powered
如图1所示,自供能气体传感系统100可以包括自供能气体传感装置110 和气体属性识别装置120两部分。As shown in FIG. 1 , the self-powered
自供能气体传感装置110可以用于获取机械能,并且通过将该机械能转 换为电能从而实现自供能。此外,该自供能气体传感装置110还能够对待测 气体环境中的气体的属性进行传感,并生成电磁波信号,该电磁波信号携带 与待测气体环境中的气体的属性相关的信息。The self-powered
例如,气体的属性可以包括以下至少之一:气体成分、气体浓度、气体 气压。气体成分可以是针对纯气体环境也可以针对混合气体环境来说的。在 混合气体环境下,气体成分不仅指代包括气体成分的类型,同时还指代它们 各自的气体浓度。For example, the properties of the gas may include at least one of the following: gas composition, gas concentration, and gas pressure. Gas composition can be for pure gas environment or for mixed gas environment. In the case of a mixed gas environment, gas composition refers not only to the type of gas composition included, but also to their respective gas concentrations.
例如,机械能可以来自人为施加的力、风力、波浪施加的力、交通工具 运动施加的力、雨滴、液体流动等等。For example, mechanical energy can come from human-applied forces, wind, waves, vehicle motion, raindrops, liquid flow, and so on.
气体属性识别装置120可以用于从自供能气体传感装置110接收电磁波 信号,并基于该电磁波信号识别所述待测气体环境中的气体的属性。The gas attribute identification device 120 can be used to receive the electromagnetic wave signal from the self-powered
由于自供能气体传感装置110和气体属性识别装置120之间是电磁波信 号传递,因此两者可以相隔较远的距离并且无需导线连接,例如可以相隔30m, 气体属性识别装置120也可以接收到电磁波信号并进行气体属性的识别。因 此,在例如受限于空间或不宜搬动气体属性识别装置的具体场景中可以有较 好的应用。Due to the electromagnetic wave signal transmission between the self-powered
自供能气体传感装置110与气体属性识别装置120的更多细节将在后文 详细描述。More details of the self-powered
根据上述自供能气体传感系统,可以实现对自供能气体传感装置所在气 体环境的气体的属性,并且可以实现对大多数气体的感测,无需外部电源供 能,产生的传感信号本身为无线信号从而不受信号传输线的约束,更不需要 附加的能量管理模块以及无线信号发射模块,因此结构简单且体积小,并且 气体属性的识别准确性高,使得自供能气体传感系统具有更大的应用范围。According to the above self-powered gas sensing system, the properties of the gas in the gas environment where the self-powered gas sensing device is located can be realized, and the sensing of most gases can be realized without external power supply, and the generated sensing signal itself is The wireless signal is not constrained by the signal transmission line, and does not require additional energy management modules and wireless signal transmission modules, so the structure is simple and small, and the identification accuracy of gas properties is high, making the self-powered gas sensing system more powerful. scope of application.
以下结合图2-4对图1所描述的自供能气体传感系统100中的自供能气 体传感装置进行详细描述。The self-powered gas sensing device in the self-powered
图2示出了根据本公开实施例的自供能气体传感装置的结构框图。FIG. 2 shows a block diagram of a self-powered gas sensing device according to an embodiment of the present disclosure.
如图2所示,自供能气体传感装置110包括能量收集器110-1和击穿放 电器110-2。As shown in Figure 2, the self-powered
能量收集器110-1被配置为获取机械能,并将机械能转换为电能。The energy harvester 110-1 is configured to harvest mechanical energy and convert the mechanical energy into electrical energy.
能量收集器110-1可以被放置在待测气体环境中,也可以放置在待测气 体环境之外。无论放置在何处,能量收集器110-1需要获取机械能,并将机 械能转换为电能,以实现自供能气体传感装置110的自供能。The energy harvester 110-1 can be placed in the gas environment to be tested, and can also be placed outside the gas environment to be tested. No matter where it is placed, the energy harvester 110-1 needs to capture mechanical energy and convert the mechanical energy into electrical energy to realize the self-powering of the self-powered
作为示例而非限制,如本公开的上下文所描述的,能量收集器110-1可 以为摩擦纳米发电机。By way of example and not limitation, energy harvester 110-1 may be a triboelectric nanogenerator as described in the context of this disclosure.
以下对摩擦纳米发电机的工作原理进行介绍。应理解,以下将描述的工 作原理是示例性地,仅仅是为了帮助更好地理解本公开的实施例,不同的摩 擦纳米发电机具有不同的工作原理。The working principle of the triboelectric nanogenerator is introduced as follows. It should be understood that the working principle described below is exemplary only to help better understand the embodiments of the present disclosure, and different triboelectric nanogenerators have different working principles.
摩擦纳米发电机110-1可以包括摩擦发电层、第一输出电极和第二输出 电极(未示出),其中,摩擦发电层用于基于所获取的机械能而在所述第一输 出电极和所述第二输出电极上形成极性相反的电荷,从而在如后文描述的与 第一输出电极和第二输出电极连接的、击穿放电器的第一电极和第二电极之 间形成电场(向击穿放电器提供电能)。当然,如果是其他类型的能量收集器, 也存在第一输出电极和第二输出电极,以在击穿放电器的第一电极和第二电 极之间形成电场。The triboelectric nanogenerator 110-1 may include a triboelectric generation layer, a first output electrode, and a second output electrode (not shown), wherein the triboelectric generation layer is used to generate electricity between the first output electrode and the second output electrode based on the obtained mechanical energy. Charges of opposite polarity are formed on the second output electrode, thereby forming an electric field between the first electrode and the second electrode of the breakdown discharger connected to the first output electrode and the second output electrode as described later ( supply power to the breakdown arrester). Of course, if it is another type of energy harvester, there are also a first output electrode and a second output electrode to form an electric field between the first electrode and the second electrode of the breakdown discharger.
摩擦纳米发电机110-1的示例结构可以如图3A-3B所示,包括滑动式摩 擦纳米发电机(FS-TENG)(图3A)、和接触分离式摩擦纳米发电机(CS-TENG) (图3B),具体工作过程将参考图3A-3B进行描述。当然,以下示例结构仅 仅是为了帮助更好地理解本公开,而不是用于限制。可以采用其他任何合适 的摩擦纳米发电机的结构。An exemplary structure of the triboelectric nanogenerator 110-1 can be shown in FIGS. 3A-3B , including a sliding type triboelectric nanogenerator (FS-TENG) ( FIG. 3A ), and a contact separation type triboelectric nanogenerator (CS-TENG) ( Fig. 3B), the specific working process will be described with reference to Fig. 3A-3B. Of course, the following exemplary structures are only for helping to better understand the present disclosure, not for limitation. Any other suitable triboelectric nanogenerator structure can be used.
摩擦纳米发电机可以为滑动式摩擦发电机,如图3A所示。滑动摩擦式 发电机由两种不同背面镀有金属电极材料的薄膜聚合物或者薄膜聚合物和电 极构成,从上往下依次包括顶部电极、摩擦极性相反的第一类型材料薄膜层 和第二类型材料薄膜层、以及底部电极。滑动摩擦式发电机接收外力(机械 能),使得第一类型材料薄膜层、第二类型材料薄膜层发生相对运动,并且由 于摩擦起电效应会有电荷转移发生,以在顶部电极和底部电极之间形成电势 差(电压差),从而可以在与顶部电极和底部电极连接的、击穿放电器的第一电极和第二电极之间形成电场(向击穿放电器提供电能)。The friction nanogenerator can be a sliding friction generator, as shown in Fig. 3A. The sliding friction generator is composed of two different thin-film polymers or thin-film polymers and electrodes coated with metal electrode materials on the back. Type material film layer, and bottom electrode. The sliding friction generator receives external force (mechanical energy), so that the first type material film layer and the second type material film layer move relative to each other, and charge transfer occurs due to the triboelectric effect, so that the top electrode and the bottom electrode A potential difference (voltage difference) is formed so that an electric field can be formed between the first electrode and the second electrode of the breakdown arrester connected to the top electrode and the bottom electrode (powering the breakdown arrestor).
示例性的,图3A显示了聚四氟乙烯是氟碳固体(PTFE)和耐纶(nylon) 两种摩擦极性相反材料构成的发电机以及其工作机理。当PTFE和nylon接触 时,因为PTFE得电子比nylon强,在PTFE表面会产生负电荷而nylon表面 有正电荷。当PTFE和nylon完全重时,nylon上的电极与PTFE下的电极并 没有电势差产生,当两者在外力(机械能)的作用下有错位运动时,在错位 面积上摩擦电荷不能完全抵消掉,此时在两个电极之间会有电势差产生。当 PTFE和nylon再次重合时,错位面积将消失,由摩擦电荷产生的电势差也会 消失,自由电子又会从nylon上的电极流向PTFE上的电极。从两个电极之间 可以输出由机械能转换得到的电能。Exemplarily, FIG. 3A shows a generator made of polytetrafluoroethylene (PTFE) and nylon (nylon) two materials with opposite frictional polarities and its working mechanism. When PTFE and nylon are in contact, because PTFE has stronger electrons than nylon, negative charges will be generated on the surface of PTFE while positive charges will be generated on the surface of nylon. When PTFE and nylon are completely heavy, there is no potential difference between the electrode on the nylon and the electrode under the PTFE. When the two have dislocation movement under the action of external force (mechanical energy), the frictional charge on the dislocation area cannot be completely offset. There is a potential difference between the two electrodes. When PTFE and nylon overlap again, the dislocation area will disappear, and the potential difference generated by the triboelectric charge will also disappear, and free electrons will flow from the electrode on the nylon to the electrode on the PTFE. The electrical energy converted from mechanical energy can be output from between the two electrodes.
另一种示例的摩擦纳米发电机可以为接触分离式摩擦纳米发电机 (CS-TENG)。如图3B所示,所述摩擦纳米发电机从上往下依次包括第一电 极层、第一摩擦材料层、与第一摩擦材料层具有不同电负性材料的第二摩擦 材料层和第二电极层,第一摩擦材料层和第二摩擦材料层中的至少一者的材 料为绝缘材料(用于长时间地保持摩擦电荷),例如,第一摩擦材料层的材料 可以是聚酰亚胺(PI)薄膜(Kapton),第二摩擦材料层的材料可以是聚甲基 丙烯酸甲酯(PMMA)。Another exemplary triboelectric nanogenerator may be a contact-separation triboelectric nanogenerator (CS-TENG). As shown in Fig. 3B, the triboelectric nanogenerator includes a first electrode layer, a first friction material layer, a second friction material layer having a different electronegativity material from the first friction material layer, and a second friction nanogenerator from top to bottom. The material of at least one of the electrode layer, the first friction material layer and the second friction material layer is an insulating material (for maintaining triboelectric charge for a long time), for example, the material of the first friction material layer can be polyimide (PI) film (Kapton), the material of the second friction material layer may be polymethyl methacrylate (PMMA).
在对第一电极层施加压力(机械能)的情况下,第一摩擦材料层和第二 摩擦材料层相互接触,由于摩擦电效应,在第一摩擦材料层和第二摩擦材料 层彼此接触的表面会带上不同极性的电荷,但是该电荷仅形成在接触表面且 正负电荷可以抵消,因此此时不会在第一电极层和第二电极层之间形成电势 差。When pressure (mechanical energy) is applied to the first electrode layer, the first friction material layer and the second friction material layer are in contact with each other. Charges of different polarities are charged, but the charges are only formed on the contact surface and the positive and negative charges can be offset, so no potential difference is formed between the first electrode layer and the second electrode layer at this time.
一旦第一摩擦材料层和第二摩擦材料层彼此接触的表面被释放而产生分 离,那么在第一摩擦材料层和第二摩擦材料层的上下两个表面上的电极就会 有电势差的产生,在该释放过程中该电势差可以在与第一电极层和第二电极 层连接的、击穿放电器的第一电极和第二电极之间形成电场(向击穿放电器 提供电能)。Once the contact surfaces of the first friction material layer and the second friction material layer are released to separate, the electrodes on the upper and lower surfaces of the first friction material layer and the second friction material layer will have a potential difference. This potential difference can form an electric field during the release process between the first electrode and the second electrode of the breakdown arrester connected to the first electrode layer and the second electrode layer (supplying the breakdown arrester with electrical energy).
也就是说,在没有压力信号输入时,摩擦纳米发电机的两个电极层上不 会产生感应电荷,从而两者之间不存在电势差,因此不能向击穿放电器提供 电能。当存在压力信号输入时,第一摩擦材料层与第二摩擦材料层产生感应 电荷,从而当在压力信号停止输入时(如前面所述的释放过程中)会在所述 第一电极层和所述第二电极层上产生感应电荷从而在两个电极层之间形成电 势差,进一步,产生的电能会提供给击穿放电器。That is to say, when there is no pressure signal input, no induced charge will be generated on the two electrode layers of the triboelectric nanogenerator, so there is no potential difference between the two, so it cannot provide electric energy to the breakdown discharger. When there is a pressure signal input, the first friction material layer and the second friction material layer generate induced charges, so that when the pressure signal stops inputting (during the release process as described above), the first electrode layer and the second friction material layer will Inductive charges are generated on the second electrode layer to form a potential difference between the two electrode layers, and further, the generated electric energy is provided to the breakdown discharger.
以下对击穿放电器110-2的工作原理进行介绍。应理解,以下将描述的 工作原理是示例性地,仅仅是为了帮助更好地理解本公开的实施例。The working principle of the breakdown arrestor 110-2 will be introduced below. It should be understood that the working principles to be described below are exemplary only to help better understand the embodiments of the present disclosure.
击穿放电器110-2被设置在待测气体环境中,击穿放电器被配置为获取 摩擦纳米发电机110-1对获取的机械能进行转换得到的电能,其中所述电能 使得所述击穿放电器在待测气体环境中进行击穿放电,击穿放电所产生的电 流导致电磁波信号的发射。The breakdown arrester 110-2 is set in the gas environment to be tested, and the breakdown arrester is configured to obtain the electrical energy obtained by converting the acquired mechanical energy by the triboelectric nanogenerator 110-1, wherein the electrical energy makes the breakdown The discharger performs breakdown discharge in the gas environment to be tested, and the current generated by the breakdown discharge leads to the emission of electromagnetic wave signals.
由于针对不同的待测气体环境(具有不同的气体属性),所生成的电磁波 信号的特性,例如,波形、幅值、频谱特征等等是不同的,因此,电磁波信 号能够携带与待测气体环境中的气体的属性相关联的信息。基于对该电磁波 信号进行分析,就可以识别出待测气体环境中的气体的属性。Due to different gas environments to be measured (with different gas properties), the characteristics of the generated electromagnetic wave signals, such as waveforms, amplitudes, spectral features, etc. are different, therefore, the electromagnetic wave signals can carry The information associated with the properties of the gases in . Based on the analysis of the electromagnetic wave signal, the properties of the gas in the gas environment to be measured can be identified.
击穿放电器110-2可以包括经由所述待测气体环境中的气体绝缘隔离的 第一电极和第二电极,并且其中,所述第一电极和第二电极具有相对的放电 尖端,所述相对的放电尖端之间具有放电间隙,所述电能在所述第一电极和 第二电极的放电尖端之间形成电场,并且所述电场使得在第一电极和第二电 极的放电尖端的放电间隙之间击穿所述待测气体环境中的气体,以进行击穿 放电。The breakdown arrester 110-2 may include a first electrode and a second electrode separated by gas insulation in the gas environment to be measured, and wherein the first electrode and the second electrode have opposite discharge tips, the There is a discharge gap between the opposite discharge tips, the electric energy forms an electric field between the discharge tips of the first electrode and the second electrode, and the electric field makes the discharge gap between the discharge tips of the first electrode and the second electrode The gas in the gas environment to be measured is broken down to perform a breakdown discharge.
例如,放电尖端可以为金属结构,并可以由电子束蒸镀工艺制造形成。 两个金属结构间最小的间距被控制在5-500微米,这一间距可以被显微镜观 测到。当从摩擦纳米发电机110-1获取到电能时,在击穿放电器的第一电极 和第二电极之间将形成电场,电场强度在放电尖端处将达到最大,当放电尖 端处的电场强度足够大时,在第一电极和第二电极的放电尖端的放电间隙之 间击穿所述待测气体环境中的气体,以进行击穿放电。For example, the discharge tip can be a metal structure and can be formed by electron beam evaporation process. The minimum distance between two metal structures is controlled at 5-500 microns, which can be observed by microscope. When the electrical energy is obtained from the triboelectric nanogenerator 110-1, an electric field will be formed between the first electrode and the second electrode of the breakdown discharger, and the electric field intensity will reach the maximum at the discharge tip, when the electric field intensity at the discharge tip When it is large enough, the gas in the gas environment to be measured is broken down between the discharge gaps of the discharge tips of the first electrode and the second electrode, so as to perform a breakdown discharge.
击穿放电将在放电尖端之间形成电流,而该电流会导致电磁波信号的发 射。The breakdown discharge will form a current between the discharge tips, and this current will cause the emission of electromagnetic wave signals.
具体地,击穿放电器的第一电极和第二电极的相对的放电尖端间产生了 一个强电场,使得电子从阴极向阳极运动。在运动过程中,电子与空气分子 发生高速碰撞,导致新的电子、正离子及负离子产生,引起电子崩并进一步 产生等离子体。该等离子体可被视为带电粒子簇的集体振荡,产生了一片零 阻抗区域,以充当电子的导体。因此,一个脉冲电流在发射系统中产生,其 幅值及脉冲上升时时间与电压、间隙宽度及气体属性(气体成分、气压、浓 度等)等有关。最终,随着电场的减弱,变弱的电子崩无法继续支持通路, 使得电路继续回到开路状态。Specifically, a strong electric field is generated between the opposing discharge tips of the first and second electrodes of the breakdown discharger, causing electrons to move from the cathode to the anode. During the movement, electrons collide with air molecules at high speed, resulting in the generation of new electrons, positive ions and negative ions, causing electron avalanche and further generating plasma. The plasma can be viewed as a collective oscillation of clusters of charged particles, creating a region of zero impedance that acts as a conductor for electrons. Therefore, a pulse current is generated in the emission system, and its amplitude and pulse rise time are related to voltage, gap width and gas properties (gas composition, pressure, concentration, etc.). Eventually, as the electric field weakens, the weakened electron avalanche cannot continue to support the path, causing the circuit to continue returning to the open circuit state.
将结合图4详细描述电磁波信号的产生过程。The process of generating the electromagnetic wave signal will be described in detail with reference to FIG. 4 .
图4示出了图2-3B所述的自供能气体传感装置(包括能量收集器和击穿 放电器)的等效电路模型。Figure 4 shows an equivalent circuit model of the self-powered gas sensing device (including the energy harvester and the breakdown arrestor) described in Figures 2-3B.
如图4所示,电压源Vi和等效电容Ci对应于能量收集器(例如摩擦纳 米发电机)的等效电路模型;C、R和L为能量收集器与击穿放电器的电容、 电感及电阻,可来源于寄生电容、寄生自感、寄生电阻等,也就是说,当击 穿放电时,能量收集器(例如摩擦纳米发电机)的电极(如前面描述的第一 输出电极和第二输出电极)和击穿放电器的第一电极和第二电极将形成一个 导通回路。一旦在击穿放电时的脉冲电流出现,它将会在摩擦纳米发电机和击穿放电器件组成的发射系统中产生一个欠阻尼振荡的电流信号。该振荡可 以在周围产生变化的磁场及变化的电场,以产生全向传播的电磁波信号,最 终传递到气体属性识别装置接收。可选地,气体属性识别装置中可以通过接 收线圈或接收电容来进行电磁波信号的接收。As shown in Figure 4, the voltage source Vi and the equivalent capacitance Ci correspond to the equivalent circuit model of the energy harvester (such as a triboelectric nanogenerator); C, R and L are the capacitance and inductance of the energy harvester and the breakdown discharger and resistance, which can be derived from parasitic capacitance, parasitic self-inductance, parasitic resistance, etc. two output electrodes) and the first electrode and the second electrode of the breakdown discharger will form a conduction loop. Once the pulse current in the breakdown discharge occurs, it will generate an underdamped oscillation current signal in the emission system composed of the triboelectric nanogenerator and the breakdown discharge device. The oscillation can generate a changing magnetic field and a changing electric field in the surroundings to generate an omnidirectionally propagating electromagnetic wave signal, which is finally transmitted to the gas attribute identification device for reception. Optionally, the electromagnetic wave signal can be received by a receiving coil or a receiving capacitor in the gas property identification device.
可以进行用于评价由击穿所引起的电磁波信号的输出表现及影响因素关 系的研究。主要影响因素根据经验可以确定为包括击穿放电器电压(U)、击 穿放电器电极间间隙距离(d)、摩擦纳米发电机运动方向(-)、能量收集器 (例如摩擦纳米发电机)与击穿放电器间连接导线长度(l)、空间导体分布 (a)、击穿放电器及接收器间距离(D)、气体成分(N)、气体气压(P)、气 体浓度(C)、温度(T)、湿度(H)。Research can be conducted to evaluate the output performance of the electromagnetic wave signal caused by the breakdown and the relationship between the influencing factors. The main influencing factors can be determined empirically, including the breakdown arrester voltage (U), the gap distance between electrodes of the breakdown arrester (d), the movement direction of the triboelectric nanogenerator (-), the energy harvester (such as triboelectric nanogenerator) The length of the connecting wire with the breakdown arrester (l), the space conductor distribution (a), the distance between the breakdown arrester and the receiver (D), the gas composition (N), the gas pressure (P), and the gas concentration (C) , temperature (T), humidity (H).
通过依次改变一个影响因素的参数值,而保持其他影响因素的参数值不 变,可以得到以下结论:大部分上述影响因素的改变会改变电磁波信号的幅 值,但是不会影响波形和频谱,但是能量收集器(例如摩擦纳米发电机)与 击穿放电器间连接导线长度(l)以及气体成分(N)、气体气压(P)、气体浓 度(C)的改变会导致电磁波信号的波形和频谱改变。这也说明了在同一个自 供能气体传感系统的结构不改变的情况下,即能量收集器(例如摩擦纳米发 电机)与击穿放电器间连接导线长度(l)固定的情况下,可以通过电磁波信 号而识别出该自供能气体传感系统所在的待测气体环境中的气体的属性。By sequentially changing the parameter value of one influencing factor, while keeping the parameter values of other influencing factors unchanged, the following conclusions can be drawn: the change of most of the above influencing factors will change the amplitude of the electromagnetic wave signal, but will not affect the waveform and spectrum, but Changes in the length of the connecting wire (l) between the energy harvester (such as a triboelectric nanogenerator) and the breakdown discharger, as well as changes in gas composition (N), gas pressure (P), and gas concentration (C) will cause the waveform and spectrum of the electromagnetic wave signal Change. This also shows that under the condition that the structure of the same self-powered gas sensing system does not change, that is, when the length (l) of the connecting wire between the energy harvester (such as a triboelectric nanogenerator) and the breakdown discharger is fixed, the The property of the gas in the gas environment to be measured where the self-powered gas sensing system is located is identified through the electromagnetic wave signal.
通过如参考图2-4描述的自供能气体传感装置,可以实现对自供能气体 传感装置所位于的气体环境中的气体的属性的感测,可以实现对大多数气体 的感测,无需外部电源供能,产生的电磁波信号本身为无线信号从而不受信 号传输线的约束并且能够携带气体属性的信息,从而通过对该电磁波信号进 行分析就能确定气体的属性。By means of the self-powered gas sensing device as described with reference to FIGS. Powered by an external power supply, the generated electromagnetic wave signal itself is a wireless signal, so it is not restricted by the signal transmission line and can carry information about the properties of the gas, so that the properties of the gas can be determined by analyzing the electromagnetic wave signal.
以下结合图5A-5D对图1所描述的自供能气体传感系统中的气体属性识 别装置的构成和工作过程进行详细描述。The composition and working process of the gas property identification device in the self-powered gas sensing system described in Fig. 1 will be described in detail below in conjunction with Figs. 5A-5D.
图5A示出了根据本公开实施例的气体属性识别装置的示意结构框图。Fig. 5A shows a schematic structural block diagram of a gas property identification device according to an embodiment of the present disclosure.
如图5A所示,气体属性识别装置120可以包括:信号接收单元120-1以 及识别单元120-2。As shown in Fig. 5A, the gas attribute identification device 120 may include: a signal receiving unit 120-1 and an identification unit 120-2.
信号接收单元120-1被配置为从所述自供能气体传感装置110接收所述 电磁波信号,并将所述电磁波信号转换为电参数的时序信号,即电参数随着时 间变化的时序信号。The signal receiving unit 120-1 is configured to receive the electromagnetic wave signal from the self-powered
例如,信号接收单元120-1可以包括电磁波接收电路以及采样电路。电 磁波接收电路可以将电磁波信号转换为预定电参数信号(例如,预定电参数 可以为电压或电流),并且采样电路可以按照预定采样频率对该预定电参数信 号进行采样,从而得到预定电参数的时序信号。电磁波接收电路的示例可以 为接收线圈和接收天线中的至少一个。For example, the signal receiving unit 120-1 may include an electromagnetic wave receiving circuit and a sampling circuit. The electromagnetic wave receiving circuit can convert the electromagnetic wave signal into a predetermined electrical parameter signal (for example, the predetermined electrical parameter can be voltage or current), and the sampling circuit can sample the predetermined electrical parameter signal according to a predetermined sampling frequency, thereby obtaining the timing of the predetermined electrical parameter Signal. An example of the electromagnetic wave receiving circuit may be at least one of a receiving coil and a receiving antenna.
识别单元120-2被配置为基于所述预定电参数的时序信号识别所述待测 气体环境中的气体的属性。The identification unit 120-2 is configured to identify the property of the gas in the gas environment to be measured based on the time series signal of the predetermined electrical parameter.
如前面所述,如果气体的属性不同,那么电磁波信号的波形和频谱特征 也会相应地不同,因此通过对电磁波信号接收和采样后得到的预定电参数的 时序信号进行分析,即能得到该电磁波信号就可以得到待测气体环境中的气 体的属性。As mentioned earlier, if the properties of the gas are different, the waveform and spectrum characteristics of the electromagnetic wave signal will be different accordingly. Therefore, the electromagnetic wave signal can be obtained by analyzing the time series signal of predetermined electrical parameters obtained after the electromagnetic wave signal is received and sampled. The properties of the gas in the gas environment to be measured can be obtained from the signal.
由于通过对电磁波信号接收和采样后得到的预定电参数的时序信号中可 能包括一些冗余信号以及噪声信号。此外,考虑多个影响因素都会影响电磁 波信号的特性(波形、幅值或频谱),例如即使针对相同的气体环境,机械能 的大小的不同也会导致电磁波信号的幅值不同,但是这不会影响波形和频谱 特征,因此还可以在信号处理过程中提取频谱信号,并可选地如后文所述的 需要基于频谱信号来进行识别,因此在一些情况下,气体属性识别装置还可 以包括信号处理单元120-3,用于对预定电参数的时序信号进行预处理得到经 处理信号,然后识别单元120-2将基于该经处理信号进行识别。当然,也可 以将该信号处理单元120-3包括在识别单元120-2中。Because the timing signal of predetermined electrical parameters obtained by receiving and sampling the electromagnetic wave signal may include some redundant signals and noise signals. In addition, considering multiple influencing factors will affect the characteristics (waveform, amplitude or spectrum) of the electromagnetic wave signal. For example, even for the same gas environment, the difference in the magnitude of the mechanical energy will cause the amplitude of the electromagnetic wave signal to be different, but this will not affect Waveform and spectrum features, so the spectrum signal can also be extracted in the signal processing process, and can optionally be identified based on the spectrum signal as described later, so in some cases, the gas attribute identification device can also include signal processing The unit 120-3 is configured to preprocess the timing signal of predetermined electrical parameters to obtain a processed signal, and then the identification unit 120-2 will perform identification based on the processed signal. Of course, the signal processing unit 120-3 may also be included in the identification unit 120-2.
例如,信号处理单元120-3可以针对电磁波接收电路输出的所述预定电 参数的时序信号去除噪声信号和/或截取有效信号,而得到经处理信号。即, 为了提高传感的准确性和/或便于识别,在将预定电参数的时序信号输入到识 别单元120-2进行识别前,先对预定电参数的时序信号进行信号处理(例如, 去除噪声信号、截取有效信号,以及提取频谱信号等等),然后基于经处理信 号来得到待测气体环境中的气体的属性。For example, the signal processing unit 120-3 may remove noise signals and/or intercept effective signals from the time series signals of the predetermined electrical parameters output by the electromagnetic wave receiving circuit to obtain processed signals. That is, in order to improve the accuracy of sensing and/or facilitate identification, before inputting the time-series signals of predetermined electrical parameters into the identification unit 120-2 for identification, the time-series signals of predetermined electrical parameters are signal-processed (for example, noise removal signal, intercept effective signal, and extract spectrum signal, etc.), and then obtain the properties of the gas in the gas environment to be measured based on the processed signal.
可选地,关于识别单元120-2识别气体属性的方式,一种方式可以包括: 识别单元120-2可以基于对获取的预定电参数的时序信号中的预定电参数的 值随时间的变化趋势(该变化趋势能反映波形)进行分析,而根据该变化趋 势而可以确定待测气体环境对应于或最接近哪种气体环境(参考气体环境之 一,根据应用场景(例如,工业、汽车尾气、室内环境等等)而预先确定可 能的气体环境作为参考气体环境)。Optionally, regarding the manner in which the identification unit 120-2 identifies the properties of the gas, one manner may include: The identification unit 120-2 may be based on the time-varying trend of the value of the predetermined electrical parameter in the time series signal of the acquired predetermined electrical parameter (this trend of change can reflect the waveform) is analyzed, and according to this trend of change, it can be determined that the gas environment to be measured corresponds to or is the closest to which gas environment (one of the reference gas environments, according to application scenarios (for example, industry, automobile exhaust, Indoor environment, etc.) and predetermine possible gas environment as a reference gas environment).
此外,另一种方式可以包括:识别单元120-2也可以根据预定电参数的 时序信号得到频谱信号(例如频谱图像),而通过对频谱信号进行分析,而确 定待测气体环境对应于或最接近哪种气体环境。In addition, another method may include: the identification unit 120-2 may also obtain a spectrum signal (such as a spectrum image) according to the time series signal of a predetermined electrical parameter, and by analyzing the spectrum signal, determine that the gas environment to be tested corresponds to or is the most Which gas environment to approach.
可选地,识别单元120-2可以基于机器学习来基于预定电参数的时序信 号得到待测气体环境中的气体的属性。Optionally, the identification unit 120-2 can obtain the properties of the gas in the gas environment to be measured based on the time series signals of predetermined electrical parameters based on machine learning.
即,识别单元120-2可以包括机器学习模型,该机器学习模块经训练能 够针对预定电参数的时序信号(为了提高识别准确性,一般采用信号处理后 的经处理信号)而生成指示气体的属性的识别结果。That is, the identification unit 120-2 may include a machine learning model, and the machine learning module can be trained to generate a property indicating gas for a time-series signal of a predetermined electrical parameter (in order to improve the identification accuracy, the processed signal after signal processing is generally used). recognition results.
如上所述,对于第一种方式,经处理信号是时域信号,因此可以选择适 合训练时域信号的机器学习模型的类型。As mentioned above, for the first approach, the processed signal is a time-domain signal, so the type of machine learning model suitable for training time-domain signals can be selected.
对于第二种方式,经处理信号是频域信号(频谱图像),因此可以选择适 合图像分类的机器学习模型的类型。For the second way, the processed signal is a frequency domain signal (spectral image), so the type of machine learning model suitable for image classification can be selected.
当然,除了利用机器学习模型之外,识别单元120-2也可以通过其他方 式来识别所述待测气体环境中的气体的属性,本公开不限于此。例如,可以 根据应用场合,预先将针对常见的各种参考气体环境中的每种参考气体环境 的电磁波信号的特性(例如,前文所述的电参数的值相对于时间的变化趋势、 频谱特征)对应地进行存储,而将在待测气体环境下时的电磁波信号进行采 样、信号处理后的经处理信号的特性与存储的各个特性进行比对,确定该特 性所对应的或最接近的气体环境。Of course, in addition to using a machine learning model, the identification unit 120-2 may also identify the attributes of the gas in the gas environment to be measured in other ways, and the present disclosure is not limited thereto. For example, according to the application, the characteristics of the electromagnetic wave signal for each of the common reference gas environments (for example, the variation trend of the value of the electrical parameters mentioned above relative to time, the spectral characteristics) Store correspondingly, and compare the characteristics of the processed signal with the stored characteristics by sampling the electromagnetic wave signal in the gas environment to be tested and signal processing, and determine the corresponding or closest gas environment for the characteristic .
接下来主要针对识别单元120-2基于机器学习模型来识别所述待测气体 环境中的气体的属性进行详细描述。Next, the identification unit 120-2 is mainly described in detail for identifying the properties of the gas in the gas environment to be measured based on the machine learning model.
机器学习模型在训练集上训练得到经训练机器学习模型,并且所述训练 集包括多个经处理信号以及所述多个经处理信号各自对应的气体属性的真实 标签。The machine learning model is trained on the training set to obtain the trained machine learning model, and the training set includes a plurality of processed signals and true labels of gas properties corresponding to each of the plurality of processed signals.
例如,对于时域信号,机器学习模型可以为双向长短时记忆循环神经网 络(bi-LSTM)模型。For example, for time-domain signals, the machine learning model can be a bidirectional long-short-term memory recurrent neural network (bi-LSTM) model.
可以对该双向长短时记忆循环神经网络(bi-LSTM)模型进行如下训练: 将训练集包括的每个时域信号分别正向输入以及反向输入到所述bi-LSTM模 型,以得到每个所述时域信号对应的预测标签,并且基于每个预测标签和对 应的时域信号的真实标签的差异,通过误差反向传播法和梯度下降法来更新 所述bi-LSTM模型的模型参数,直至所述模型参数相对于所述训练集而收敛。 训练集的获取方式将在后文描述。This bidirectional long-short-term memory recurrent neural network (bi-LSTM) model can be trained as follows: Each time domain signal included in the training set is input into the bi-LSTM model forwardly and backwardly, to obtain each The predicted label corresponding to the time domain signal, and based on the difference between each predicted label and the real label of the corresponding time domain signal, the model parameters of the bi-LSTM model are updated by the error backpropagation method and the gradient descent method, until the model parameters converge with respect to the training set. The way to obtain the training set will be described later.
例如,关于该bi-LSTM模型,双向LSTM层每个方向设置有50个神经 元,一共存在100个神经元;然后,在该双向LSTM层之后的输出连接到全 连接层(包括32个神经元),经过批归一化(Batch Normalization,动量 momentum设置为0.8)之后通过激活函数(例如,ReLu)激活,然后连接至 模型输出结构中的全连接层,该全连接层根据分类的数量而设置神经元的数 量(例如,如果该模型经训练后用于识别十种气体环境中的气体,那么该神 经元的数量则设置为10),最后通过softmax函数激活,从而得到训练集中的 每个训练样本(经处理信号)的预测标签。预测标签和该训练样本的真实标 签可能存在差异,因此可以利用该差异来进行模型参数更新,即在模型参数 更新的过程中,可以采用误差反向传播法和梯度下降法来进行模型参数更新。For example, regarding the bi-LSTM model, the bidirectional LSTM layer has 50 neurons in each direction, and there are 100 neurons in total; then, the output after the bidirectional LSTM layer is connected to the fully connected layer (including 32 neurons ), after batch normalization (Batch Normalization, momentum momentum is set to 0.8), it is activated by an activation function (for example, ReLu), and then connected to the fully connected layer in the model output structure, which is set according to the number of categories The number of neurons (for example, if the model is trained to identify gases in ten gas environments, then the number of neurons is set to 10), and finally activated by the softmax function, so that each training set in the training set The predicted label for the sample (processed signal). There may be differences between the predicted label and the real label of the training sample, so the difference can be used to update the model parameters, that is, in the process of updating the model parameters, the error back propagation method and the gradient descent method can be used to update the model parameters.
例如,对于频谱信号,机器学习模型可以为例如卷积神经网络模型等等 可以用于图像分类的机器学习模型。For example, for spectral signals, the machine learning model can be, for example, a convolutional neural network model, etc., which can be used for image classification.
可以对该例如卷积神经网络模型等等可以用于图像分类的机器学习模型 进行如下训练:将所述训练集包括的每个频谱图像信号输入到所述CNN模型, 以得到每个所述频谱图像信号对应的预测标签,并且基于每个预测标签和对 应的频谱图像信号的真实标签的差异,通过误差反向传播法和梯度下降法来 更新所述CNN模型的模型参数,直至所述模型参数相对于所述训练集而收敛。 同样地,训练集的获取方式将在后文描述。The machine learning model that can be used for image classification, such as a convolutional neural network model, etc., can be trained as follows: each spectrum image signal included in the training set is input to the CNN model to obtain each spectrum. The predicted label corresponding to the image signal, and based on the difference between each predicted label and the corresponding real label of the spectral image signal, the model parameters of the CNN model are updated by the error backpropagation method and the gradient descent method until the model parameters Converged with respect to the training set. Likewise, the way to obtain the training set will be described later.
例如,卷积神经网络可以采用例如AlexNet、ResNet架构等通用架构, 并且同样地输出针对训练集中的每个训练样本(经处理信号)的预测标签。 预测标签和该训练样本的真实标签也可能存在差异,因此也可以利用该差异 来进行模型参数更新,即在模型参数更新的过程中,可以采用误差反向传播 法和梯度下降法来进行模型参数更新。For example, a convolutional neural network can adopt a general architecture such as AlexNet, ResNet architecture, etc., and likewise output a predicted label for each training sample (processed signal) in the training set. There may also be differences between the predicted label and the real label of the training sample, so this difference can also be used to update the model parameters, that is, in the process of updating the model parameters, the error back propagation method and the gradient descent method can be used to update the model parameters. renew.
通常,机器学习模型是在训练集上进行训练的,因此在训练机器学习模 型之前,需要获取训练集。Usually, the machine learning model is trained on the training set, so before training the machine learning model, it is necessary to obtain the training set.
由于参考前文所述,每个经处理信号是通过将接收到的电磁波信号进行 信号处理而得到的,并且不同气体环境下基于击穿放电过程生成的电磁波信 号的特性是不同的,因此基于不同气体环境下的电磁波信号可用于得到多个 经处理信号。因此,可以通过以下方式得到训练集。As mentioned above, each processed signal is obtained by signal processing the received electromagnetic wave signal, and the characteristics of the electromagnetic wave signal generated based on the breakdown discharge process in different gas environments are different, so based on different gas The electromagnetic wave signal in the environment can be used to obtain a plurality of processed signals. Therefore, the training set can be obtained in the following way.
首先,选择具有不同的气体属性的第一数量的参考气体环境。First, a first number of reference gas environments with different gas properties are selected.
作为示例而非限制,在本公开的实施例中使用10种参考气体环境(如表 1所示),根据具体的应用场景(例如,工业、汽车尾气、室内环境等等)需 要实际识别的气体环境,而可以选择不同的更多种参考气体环境来生成训练 集。其中,在本公开的如下内容中,10种参考气体环境的气压均为一个标准 大气压。当然,如果最终训练的机器学习模型需要识别待测气体环境的气体 气压,那么识别气体气压也应该作为一个训练目标,这时候可以将气体气压 也作为变量,例如可以将至少两个参考气体环境的气体气压设置为不同,但 是气体成分、气体浓度又相同。As an example and not a limitation, 10 kinds of reference gas environments (as shown in Table 1) are used in the embodiments of the present disclosure, according to specific application scenarios (for example, industry, automobile exhaust, indoor environment, etc.) need to actually identify the gas environment, but different and more reference gas environments can be selected to generate the training set. Wherein, in the following content of the present disclosure, the air pressure of 10 kinds of reference gas environments is a standard atmospheric pressure. Of course, if the final training machine learning model needs to identify the gas pressure of the gas environment to be tested, then identifying the gas pressure should also be used as a training goal. At this time, the gas pressure can also be used as a variable, for example, at least two reference gas environments can be The gas pressure is set to be different, but the gas composition and gas concentration are the same.
【表1】10种参考气体环境[Table 1] 10 reference gas environments
然后,针对每种参考气体环境得到第二数量的经处理信号。A second quantity of processed signals is then obtained for each reference gas environment.
图5B示出了基于自供能气体传感装置得到第二数量的经处理信号的结 构示意图。选择要用于识别待测气体环境的自供能气体传感装置的结构,即 选择能量收集器(例如摩擦纳米发电机)以及击穿放电器的结构和参数。如 前面参考图2-4描述的自供能气体传感装置的结构,能量收集器的第一输出 电极和第二输出电极分别与击穿放电器的第一电极和第二电极连接,以向击 穿放电器提供电能。也就是说,在确定了要用于识别待测气体环境中的气体 的属性的自供能气体传感装置的结构之后,如将在后文描述的基于参考气体 环境生成训练集所基于的自供能气体传感装置的结构也需要是相同的结构 (不同的结构(例如,能量收集器和击穿放大器的连接导线长度(l)可能存 在差异)会导致针对同一气体环境生成的电磁波信号的波形和频谱特征不同), 这样才能最准确地训练机器学习模型。Fig. 5B shows a schematic diagram of a structure for obtaining a second quantity of processed signals based on a self-powered gas sensing device. Select the structure of the self-powered gas sensing device to be used to identify the gas environment to be measured, i.e. select the structure and parameters of the energy harvester (e.g. triboelectric nanogenerator) and the breakdown arrestor. As in the structure of the self-powered gas sensing device described above with reference to FIGS. The discharger provides electrical energy. That is to say, after determining the structure of the self-powered gas sensing device to be used to identify the properties of the gas in the gas environment to be measured, as will be described later, the self-powered gas sensing device on which the training set is generated based on the reference gas environment is based. The structure of the gas sensing device also needs to be the same structure (different structures (for example, the connection wire length (l) of the energy harvester and the breakdown amplifier may be different) will cause the waveform and Spectral features are different), so that the machine learning model can be trained most accurately.
可选地,依次针对每种参考气体环境,执行以下操作i-iii,来获得第二数 量的经处理信号。Optionally, for each reference gas environment in turn, perform the following operations i-iii to obtain the second number of processed signals.
操作i,将击穿放电器放置在充满所述参考气体环境中的气体的密闭气室 中,例如可以先将密闭气室抽真空,然后注入该参考气体环境对应的气体。 在后续更换参考气体环境时,又可以重新将密闭气室抽真空,然后注入下一 个参考气体环境对应的气体。Operation i, the breakdown arrester is placed in the airtight chamber filled with the gas in the reference gas environment, for example, the airtight chamber can be evacuated first, and then the gas corresponding to the reference gas environment can be injected. When the reference gas environment is subsequently replaced, the airtight chamber can be evacuated again, and then the gas corresponding to the next reference gas environment can be injected.
操作ii,由能量收集器(例如,摩擦纳米发电机)获取机械能,以将所 述机械能转换为电能,其中所述击穿放电器基于从所述能量收集器获取的电 能而在所述参考气体环境中进行击穿放电,并且击穿放电所产生的电流导致 电磁波信号的发射。Operation ii, harvesting mechanical energy by an energy harvester (e.g., a triboelectric nanogenerator) to convert the mechanical energy into electrical energy, wherein the breakdown arrestor is activated in the reference gas based on the electrical energy harvested from the energy harvester The breakdown discharge is carried out in the environment, and the current generated by the breakdown discharge leads to the emission of electromagnetic wave signals.
操作iii,在该电磁波信号发射后,电磁波接收电路可以获取该电磁波信 号,并将所述电磁波信号转换为电参数的第二数量的时序信号(例如将相同 时间长度的第二数量的时间段各自的多个采样点以及对应的电参数值形成预 定电参数的第二数量的时序信号),例如,如图5C所示,作为示例,参考气 体环境的种类数量(第一数量)为10,针对每个参考气体环境得到的电压的 时序信号的数量为100,如后文所述,包括用于训练集的第二数量80加上用 于测试集的第三数量20。此后,对每个预定电参数的时序信号进行处理,得 到所述第二数量的经处理信号。Operation iii, after the electromagnetic wave signal is emitted, the electromagnetic wave receiving circuit can acquire the electromagnetic wave signal, and convert the electromagnetic wave signal into a second number of time series signals of electrical parameters (for example, the second number of time periods of the same time length are respectively A plurality of sampling points and corresponding electrical parameter values form a second number of time series signals of predetermined electrical parameters), for example, as shown in Figure 5C, as an example, the number of types (first number) of the reference gas environment is 10, for The number of time-series signals of the voltage obtained for each reference gas environment is 100, as described later, including the
为了更清楚的说明上述得到第二数量的经处理信号的过程,图5D还示 出了针对每种参考气体环境得到第二数量的经处理信号的流程图。In order to more clearly illustrate the above process of obtaining the second number of processed signals, Fig. 5D also shows a flowchart for obtaining the second number of processed signals for each reference gas environment.
如图5D所示,气室初始状为空气环境,首先对气室抽真空至0.001兆帕 (MPa),并且注入此次的参考气体环境对应的气体(目标气体)至0.1MPa (一个大气压),并重复该过程多次(这里举例为5),以保证目标气体充满 气室并且气室中不存在其他气体。然后,由能量收集器(例如,摩擦纳米发 电机)输出的电能使得所述击穿放电器进行击穿放电以实现电磁波信号的发 射,接着在接收电磁波信号时还将所述电磁波信号转换为预定电参数的时序 信号并进一步得到经处理信号,当预定电参数的时序信号的数量达到预设数 量100(如后文所述,用于训练集的第二数量80加上用于测试集的第三数量 20)时,停止针对当前参考气体环境的经处理信号的获取,重新将气室抽真 空至0.001MPa,并且注入下一个的参考气体环境对应的气体(图中示出为空 气环境)至0.1MPa(一个大气压),并重复该过程多次(这里举例为5),以 进行针对下一个参考气体环境得到第二数量的经处理信号。As shown in Figure 5D, the initial state of the gas chamber is an air environment. First, the gas chamber is evacuated to 0.001 MPa (MPa), and the gas (target gas) corresponding to the reference gas environment is injected to 0.1 MPa (one atmosphere) , and repeat this process several times (here, 5 for example) to ensure that the target gas fills the air chamber and there are no other gases in the air chamber. Then, the electrical energy output by the energy harvester (for example, a triboelectric nanogenerator) causes the breakdown discharger to perform breakdown discharge to realize the emission of electromagnetic wave signals, and then convert the electromagnetic wave signals into predetermined The time-series signals of electrical parameters and further obtain processed signals, when the number of time-series signals of predetermined electrical parameters reaches the preset number 100 (as described later, the
接着,针对每种参考气体环境,将所述第二数量的经处理信号和各自对 应的气体属性的真实标签作为该种参考气体环境的训练子集。Then, for each kind of reference gas environment, the processed signals of the second quantity and the true labels of the respective gas properties are used as the training subset of this kind of reference gas environment.
最后,将所述第一数量的参考气体环境各自的训练子集共同作为训练集。Finally, the respective training subsets of the first quantity of reference gas environments are collectively used as a training set.
例如,在第二数量为80的情况下,将针对每种参考气体环境获得的80 个经处理信号(当然,这里80仅仅是示例)以及这80个经处理信号各自对 应的气体属性的真实标签(例如,是空气、氮气、还是氦气等等,可以用表 格里的编号(1、2、3…10)来标注)共同作为训练集,在该示例中,该训 练集包括800组训练数据。For example, in the case where the second number is 80, the 80 processed signals obtained for each reference gas environment (of course, 80 is only an example here) and the real labels of the respective gas properties corresponding to the 80 processed signals (for example, air, nitrogen, or helium, etc., can be marked with the number (1, 2, 3...10) in the table) together as the training set, in this example, the training set includes 800 sets of training data .
可选地,这80个经处理信号(可能为时域信号也可能为频谱信号)可以 为图像形式。也就是说,在从预定电参数的每个时序信号得到时域信号或频 谱信号后,可以进一步生成时域图像或频谱图像,以便于机器学习模型的训 练。Optionally, the 80 processed signals (which may be time domain signals or frequency spectrum signals) may be in the form of images. That is to say, after obtaining a time-domain signal or a frequency spectrum signal from each time-series signal of predetermined electrical parameters, a time-domain image or frequency spectrum image can be further generated to facilitate the training of the machine learning model.
此外,一般在机器学习模型训练结束后,还会使用测试集来评估经训练 机器学习模型的性能,即利用该模型未见过的训练样本来测试经训练机器学 习模型的性能。In addition, generally after the machine learning model is trained, the test set is used to evaluate the performance of the trained machine learning model, that is, the performance of the trained machine learning model is tested by using training samples that the model has not seen.
在本公开的实施例中,可以通过以下方式来验证经训练机器学习模型的 性能,也即自供能气体传感系统的有效性。In an embodiment of the present disclosure, the performance of the trained machine learning model, i.e., the effectiveness of the self-powered gas sensing system, can be verified in the following manner.
首先,针对每种参考气体环境,在获取第二数量的经处理信号时还附加 地获取第三数量的经处理信号,并将该第三数量的经处理信号和各自对应的 气体属性的真实标签作为测试子集。First, for each reference gas environment, when acquiring the second number of processed signals, a third number of processed signals is additionally acquired, and the third number of processed signals and the real labels of the respective corresponding gas properties as a test subset.
然后,将所述第一数量的参考气体环境的测试子集共同作为测试集。Then, the test subsets of the first quantity of reference gas environments are collectively used as a test set.
例如,针对每种参考气体环境获取100个经处理信号,并将其划分为第 一部分和第二部分,其中,第一部分如上所述包括第二数量80个经处理信号 (和其标签作为80组训练数据),第二部分包括第三数量20个经处理信号(和 其标签作为20组测试数据)。例如,由于参考气体环境为10种,那么具有 10个测试子集共同构成该测试集,共有200组测试数据。For example, 100 processed signals are acquired for each reference gas environment and divided into a first part and a second part, wherein the first part includes a second number of 80 processed signals (and their labels as 80 groups) as described above. training data), the second part includes a third number of 20 processed signals (and their labels as 20 sets of test data). For example, since there are 10 reference gas environments, 10 test subsets together constitute the test set, and there are 200 sets of test data in total.
接着,将所述测试集中的所有经处理信号输入经训练机器学习模型,并 从所述经训练机器学习模型得到识别结果(预测标签)。Next, all the processed signals in the test set are input into the trained machine learning model, and the recognition results (predicted labels) are obtained from the trained machine learning model.
例如,可以将测试集中的测试数据按照真实标签类型顺序地或者随机地 输入经训练机器学习模型,并从所述经训练机器学习模型得到识别结果(预 测标签)。For example, the test data in the test set can be sequentially or randomly input into the trained machine learning model according to the true label type, and the recognition result (predicted label) is obtained from the trained machine learning model.
最后,基于从所述经训练机器学习模型得到的每个经处理信号的识别结 果(预测标签)和所述经处理信号对应的气体属性的真实标签,得到所述自 供能气体传感系统的有效性。Finally, based on the recognition result (predicted label) of each processed signal obtained from the trained machine learning model and the real label of the gas property corresponding to the processed signal, the effective value of the self-powered gas sensing system is obtained. sex.
例如,以测试集中的200组测试数据为例,如果197组测试数据(经处 理信号)各自的识别结果和标签一致,3组测试数据(经处理信号)各自的 识别结果和标签不一致,则可以确定该自供能气体传感系统的有效性为98.5%。For example, taking the 200 sets of test data in the test set as an example, if the recognition results of the 197 sets of test data (processed signals) are consistent with the labels, and the recognition results of the 3 sets of test data (processed signals) are inconsistent with the labels, then you can The effectiveness of the self-powered gas sensing system was determined to be 98.5%.
在机器学习中,还可以基于测试集通过混淆矩阵来自动地得到该有效性。In machine learning, this validity can also be obtained automatically through the confusion matrix based on the test set.
图6示出了基于混淆矩阵示出有效性的示意图。仍然以训练集和数据集 都针对上述10种参考气体环境而获得为例。Fig. 6 shows a schematic diagram showing effectiveness based on a confusion matrix. Still take the training set and data set obtained for the above-mentioned 10 kinds of reference gas environments as an example.
从图6示出的混淆矩阵可知,对于针对编号为1、2、4-8的参考气体环 境获得的7个测试子集中的所有测试数据,预测标签(经训练机器学习模型 的识别结果)与真实标签是一致的,例如,均是1,均是2,均是4-8之一等 等,也可以理解为,针对编号为1、2、4-8的参考气体环境中的每一者获得 的测试子集中的20个测试数据的识别结果均正确。另一方面,对于针对编号 为3、9-10的参考气体环境获得的3个测试子集中的部分测试数据,预测标 签(经训练机器学习模型的识别结果)与真实标签不一致。例如,针对编号 为3的参考气体环境获得的测试子集中,有一个测试数据的预测标签(识别 结果)为2,但是真实标签应该为3,因此针对编号为3的参考气体环境获得 的测试子集的识别结果的正确率为95%,错误率为5%。From the confusion matrix shown in Figure 6, it can be seen that for all the test data in the 7 test subsets obtained for the reference gas environments numbered 1, 2, 4-8, the predicted labels (recognition results of the trained machine learning model) and The real labels are consistent, for example, all are 1, all are 2, all are one of 4-8, etc., which can also be understood as, for each of the reference gas environments numbered 1, 2, 4-8 The recognition results of 20 test data in the obtained test subset are all correct. On the other hand, for some of the test data in the 3 test subsets obtained for the reference gas environments numbered 3, 9-10, the predicted labels (recognition results of the trained machine learning model) were inconsistent with the real labels. For example, in the test subset obtained for the reference gas environment numbered 3, there is a test data whose predicted label (recognition result) is 2, but the real label should be 3, so the test subset obtained for the reference gas environment numbered 3 The correct rate of the recognition results of the set is 95%, and the error rate is 5%.
综合针对编号为1-10的所有参考气体环境获得的所有测试数据的预测标 签与真实标签的比对结果,基于混淆矩阵可以确定该自供能气体传感系统的 有效性为98.5%,可以实现对输入信号的成功识别。Based on the comparison results of the predicted labels and the real labels of all test data obtained for all reference gas environments numbered 1-10, it can be determined that the effectiveness of the self-powered gas sensing system is 98.5% based on the confusion matrix. Successful recognition of the input signal.
通过上面参考图5A-6描述的气体属性识别装置,可以实现对自供能气体 传感装置(或者其包括的击穿放大器)所位于的气体环境中的气体的属性的 识别,通过对该电磁波信号进行分析就能确定气体的属性,并且可以实现对 大多数气体的感测。此外,气体属性的具体识别过程可以通过机器学习模型 来识别,并且机器学习模型的训练集可以通过针对不同的气体环境而生成的 电磁波信号来获得。此外,在获取训练集的同时还获取了测试集,可以用来 测试该自供能气体传感系统的有效性。Through the gas attribute identification device described above with reference to FIGS. Analysis allows the properties of the gas to be determined, and sensing of most gases is possible. In addition, the specific identification process of gas properties can be identified through a machine learning model, and the training set of the machine learning model can be obtained through electromagnetic wave signals generated for different gas environments. In addition, a test set was obtained along with the training set, which can be used to test the effectiveness of the self-powered gas sensing system.
根据本公开的又一方面,还提供了一种自供能气体传感方法,可以用于 识别待测气体环境中的气体的属性。According to yet another aspect of the present disclosure, there is also provided a self-powered gas sensing method that can be used to identify properties of gases in a gaseous environment to be measured.
图7示出了根据本公开的实施例的自供能气体传感方法的示意流程图, 该方法用于识别待测气体环境中的气体的属性。FIG. 7 shows a schematic flow diagram of a self-powered gas sensing method for identifying properties of a gas in a gas environment to be measured, according to an embodiment of the present disclosure.
如图7所示,在步骤S710中,将击穿放电器放置在待测气体环境中。As shown in FIG. 7, in step S710, the breakdown arrester is placed in the gas environment to be tested.
可选地,击穿放电器可以为如参考图2-4描述的自供能气体传感装置中 的击穿放电器。Alternatively, the breakdown arrestor may be a breakdown arrestor as in a self-powered gas sensing device as described with reference to Figures 2-4.
在步骤S720中,利用能量收集器获取机械能,并将所述机械能转换为电 能。In step S720, the energy harvester is used to obtain mechanical energy and convert the mechanical energy into electrical energy.
可选地,能量收集器可以为摩擦纳米发电机。该摩擦纳米发电机可以为 如参考图2-4描述的自供能气体传感装置中的摩擦纳米发电机。并且,步骤 S720的更多细节也已经在前文详细描述,因此这里不再重复。Alternatively, the energy harvester can be a triboelectric nanogenerator. The triboelectric nanogenerator may be a triboelectric nanogenerator in a self-powered gas sensing device as described with reference to Figures 2-4. Moreover, more details of step S720 have also been described in detail above, so it will not be repeated here.
可选地,摩擦纳米发电机可以与击穿放电器一起放在待测气体环境中, 但是有些时候,例如空间限制的情况下,摩擦纳米发电机也可以不放在待测 气体环境中(击穿放大器需要放在待测气体环境中)。Optionally, the triboelectric nanogenerator can be placed in the gas environment to be tested together with the breakdown arrester, but sometimes, for example, in the case of space constraints, the triboelectric nanogenerator can also not be placed in the gas environment to be measured (the breakdown arrester The wear amplifier needs to be placed in the gas environment to be tested).
在步骤S730中,利用所述击穿放电器获取所述电能,其中所述电能使得 所述击穿放电器在待测气体环境中进行击穿放电,并且击穿放电所产生的电 流导致电磁波信号的发射,并且其中,所述电磁波信号携带与所述待测气体 环境中的气体的属性相关联的信息。In step S730, the electrical energy is obtained by using the breakdown arrester, wherein the electrical energy causes the breakdown arrester to perform breakdown discharge in the gas environment to be tested, and the current generated by the breakdown discharge causes an electromagnetic wave signal and wherein the electromagnetic wave signal carries information associated with properties of the gas in the gas environment to be measured.
如前面所述,能量收集器(例如,摩擦纳米发电机)的第一输出电极和 第二输出电极与击穿放电器的第一电极和第二电极连接,以向击穿放电器提 供电能,以在该第一电极和第二电极之间形成电场,并且当电场的强度足够 大时,击穿放大器能够进行击穿放电,因此会形成一个电流回路,在该电流 回路中由于存在电感和电容,因此会发生振荡,该振荡可以在周围产生变化 的磁场及变化的电场,以产生全向传播的电磁波信号,最终传递到气体属性 识别装置接收。此外,针对不同气体环境,电磁波信号的幅值和频谱都会不 同,因此气体属性识别装置基于对所发射的电磁波信号的分析就可以得知此 时的气体环境中的气体的属性。As mentioned above, the first output electrode and the second output electrode of the energy harvester (for example, a triboelectric nanogenerator) are connected to the first electrode and the second electrode of the breakdown arrester to provide electrical energy to the breakdown arrester, To form an electric field between the first electrode and the second electrode, and when the strength of the electric field is large enough, the breakdown amplifier can perform breakdown discharge, so a current loop will be formed. In this current loop, due to the existence of inductance and capacitance , so there will be oscillation, which can generate a changing magnetic field and a changing electric field around, so as to generate an omnidirectionally propagating electromagnetic wave signal, which is finally transmitted to the gas attribute identification device for reception. In addition, for different gas environments, the amplitude and frequency spectrum of the electromagnetic wave signal will be different, so the gas property identification device can know the property of the gas in the gas environment at this time based on the analysis of the emitted electromagnetic wave signal.
在步骤S740中,利用气体属性识别装置基于所述电磁波信号,识别所述 待测气体环境中的气体的属性。In step S740, the property of the gas in the gas environment to be measured is identified based on the electromagnetic wave signal by using the gas property identification device.
可选地,步骤S740可以包括利用气体属性识别装置执行以下各个子步骤。Optionally, step S740 may include using the gas property identification device to perform the following sub-steps.
在子步骤S740-1中,接收所述电磁波信号,并将所述电磁波信号转换为 预定电参数的时序信号。In sub-step S740-1, the electromagnetic wave signal is received, and the electromagnetic wave signal is converted into a time series signal of predetermined electrical parameters.
例如,可以通过接收线圈接收电磁波信号并将其转换为预定电参数信号, 并通过采样电路而获得预定电参数的时序信号。For example, the electromagnetic wave signal can be received by the receiving coil and converted into a predetermined electrical parameter signal, and the time series signal of the predetermined electrical parameter can be obtained through the sampling circuit.
在子步骤S740-2中,对所述预定电参数的时序信号进行信号处理,得到 经处理信号。In sub-step S740-2, signal processing is performed on the time series signal of the predetermined electrical parameter to obtain a processed signal.
例如,信号处理可以包括以下至少一项操作:去除噪声信号;截取有效 信号;以及提取频谱信号。For example, signal processing may include at least one of the following operations: removing noise signals; intercepting effective signals; and extracting spectrum signals.
在子步骤S740-3中,基于所述经处理信号,识别所述待测气体环境中的 气体的属性。In sub-step S740-3, based on the processed signal, the properties of the gas in the gas environment to be measured are identified.
例如,可以利用经训练机器学习模型来基于所述经处理信号,识别所述 待测气体环境中的气体的属性。For example, a trained machine learning model may be utilized to identify properties of the gas in the gaseous environment under test based on the processed signal.
用于训练机器学习模型的训练集以及测试机器学习模型性能的测试集的 获取方式可以参考如图5B-5D进行的描述。The way to obtain the training set for training the machine learning model and the test set for testing the performance of the machine learning model can refer to the descriptions in Figures 5B-5D.
自供能气体传感方法的更多细节与前文对自供能气体传感装置和系统的 内容相同相似,因此这里不再重复描述。More details of the self-powered gas sensing method are the same as those for the self-powered gas sensing device and system above, so the description will not be repeated here.
同样的,通过上述自供能气体传感方法,可以实现对自供能气体传感装 置所位于的气体环境中的气体的属性的识别,并可以实现对大多数气体的感 测,无需外部电源供能,且产生的电磁波信号本身为无线信号从而不受信号 传输线的约束并且能够携带气体属性的信息,从而通过对该电磁波信号进行 分析就能确定气体的属性。此外,气体属性的具体识别过程可以通过机器学 习模型来识别,并且机器学习模型的训练集可以通过针对不同的气体环境而 生成的电磁波信号来获得。此外,在获取训练集的同时还获取了测试集,可 以用来测试该自供能气体传感系统的有效性。Similarly, through the above self-powered gas sensing method, the identification of the properties of the gas in the gas environment where the self-powered gas sensing device is located can be realized, and the sensing of most gases can be realized without external power supply , and the generated electromagnetic wave signal itself is a wireless signal, so it is not restricted by the signal transmission line and can carry the information of gas properties, so that the properties of the gas can be determined by analyzing the electromagnetic wave signal. In addition, the specific identification process of gas properties can be identified through a machine learning model, and the training set of the machine learning model can be obtained through electromagnetic wave signals generated for different gas environments. In addition, a test set was obtained along with the training set, which can be used to test the effectiveness of the self-powered gas sensing system.
根据本公开的又一方面,还提供了一种计算设备。该计算设备可以用于 实现如前文所述的气体属性识别装置中的识别单元或者执行该识别单元的各 个操作。此外,计算设备还可以实现气体属性识别装置中的信号处理单元的 至少一部分操作。According to yet another aspect of the present disclosure, a computing device is also provided. The computing device can be used to implement the recognition unit in the gas attribute recognition device as described above or perform various operations of the recognition unit. In addition, the computing device can also implement at least a part of the operations of the signal processing unit in the gas property identification device.
图8示出了根据本公开实施例的计算设备800的结构框图。FIG. 8 shows a structural block diagram of a computing device 800 according to an embodiment of the present disclosure.
该计算机设备包括:处理器;和存储器,其上存储有指令,所述指令在 由所述处理器执行时,使得所述处理器执行识别单元所执行的基于机器学习 来识别待测气体环境中的气体的属性的过程涉及的各个操作。The computer device includes: a processor; and a memory, on which instructions are stored, and the instructions, when executed by the processor, cause the processor to perform the machine learning-based identification of the gas environment to be tested performed by the identification unit. The individual operations involved in the process of the properties of the gas.
所述计算设备可以为计算机终端、移动终端或其它设备。The computing device may be a computer terminal, a mobile terminal or other devices.
处理器可以是一种集成电路芯片,具有信号的处理能力。上述处理器可 以是通用处理器、数字信号处理器(DSP)、专用集成电路(ASIC)、现成可 编程门阵列(FPGA)或者其他可编程逻辑器件、分立门或者晶体管逻辑器件、 分立硬件组件。可以实现或者执行本公开的实施例中的识别单元以及可选地 信号处理单元执行的操作的各步骤及逻辑框图。通用处理器可以是微处理器 或者该处理器也可以是任何常规的处理器等,可以是X84架构或ARM架构 的。The processor can be an integrated circuit chip with signal processing capability. The above-mentioned processor may be a general-purpose processor, a digital signal processor (DSP), an application-specific integrated circuit (ASIC), an off-the-shelf programmable gate array (FPGA) or other programmable logic devices, discrete gate or transistor logic devices, and discrete hardware components. The steps and logical block diagrams of the operations performed by the identification unit and optionally the signal processing unit in the embodiments of the present disclosure may be realized or executed. The general-purpose processor can be a microprocessor or the processor can also be any conventional processor, etc., and can be of X84 architecture or ARM architecture.
存储器可以是非易失性存储器,诸如只读存储器(ROM)、可编程只读 存储器(PROM)、可擦除可编程只读存储器(EPROM)、电可擦除可编程只 读存储器(EEPROM)或闪存。应注意,本公开描述的方法的存储器旨在包 括但不限于这些和任意其它适合类型的存储器。The memory can be a non-volatile memory such as read only memory (ROM), programmable read only memory (PROM), erasable programmable read only memory (EPROM), electrically erasable programmable read only memory (EEPROM) or flash. It should be noted that the memory of the methods described in this disclosure is intended to include, but not be limited to, these and any other suitable types of memory.
计算设备的显示屏可以是液晶显示屏或者电子墨水显示屏,计算机设备 的输入装置可以是显示屏上覆盖的触摸层,也可以是终端外壳上设置的按键、 轨迹球或触控板,还可以是外接的键盘、触控板或鼠标等。The display screen of the computing device may be a liquid crystal display screen or an electronic ink display screen, and the input device of the computer device may be a touch layer covered on the display screen, or a button, a trackball or a touch pad provided on the terminal shell, or It is an external keyboard, trackpad or mouse.
需要说明的是,附图中的流程图和框图,图示了按照本公开各种实施例 的系统、方法和计算机程序产品的可能实现的体系架构、功能和操作。在这 点上,流程图或框图中的每个方框可以代表一个模块、程序段、或代码的一 部分,模块、程序段、或代码的一部分包含至少一个用于实现规定的逻辑功 能的可执行指令。也应当注意,在有些作为替换的实现中,方框中所标注的 功能也可以以不同于附图中所标注的顺序发生。例如,两个接连地表示的方 框实际上可以基本并行地执行,它们有时也可以按相反的顺序执行,这依所 涉及的功能而定。也要注意的是,框图和/或流程图中的每个方框、以及框图 和/或流程图中的方框的组合,可以用执行规定的功能或操作的专用的基于硬 件的系统来实现,或者可以用专用硬件与计算机指令的组合来实现。It should be noted that the flowcharts and block diagrams in the accompanying drawings illustrate the architecture, functions and operations of possible implementations of systems, methods and computer program products according to various embodiments of the present disclosure. In this regard, each block in the flowchart or block diagram may represent a module, program segment, or part of code that includes at least one executable program for implementing specified logical functions. instruction. It should also be noted that, in some alternative implementations, the functions noted in the block may occur out of the order noted in the figures. For example, two blocks shown in succession may, in fact, be executed substantially concurrently, or they may sometimes be executed in the reverse order, depending upon the functionality involved. It should also be noted that each block of the block diagrams and/or flowchart illustrations, and combinations of blocks in the block diagrams and/or flowchart illustrations, can be implemented by a dedicated hardware-based system that performs the specified functions or operations , or may be implemented by a combination of dedicated hardware and computer instructions.
一般而言,本公开的各种示例实施例可以在硬件或专用电路、软件、固 件、逻辑,或其任何组合中实施。某些方面可以在硬件中实施,而其他方面 可以在可以由控制器、微处理器或其他计算设备执行的固件或软件中实施。 当本公开的实施例的各方面被图示或描述为框图、流程图或使用某些其他图 形表示时,将理解此处描述的方框、装置、系统、技术或方法可以作为非限 制性的示例在硬件、软件、固件、专用电路或逻辑、通用硬件或控制器或其 他计算设备,或其某些组合中实施。In general, the various example embodiments of the present disclosure may be implemented in hardware or special purpose circuits, software, firmware, logic, or any combination thereof. Certain aspects may be implemented in hardware, while other aspects may be implemented in firmware or software, which may be executed by a controller, microprocessor or other computing device. When aspects of the embodiments of the present disclosure are illustrated or described as block diagrams, flowcharts, or using some other graphical representation, it is to be understood that the blocks, devices, systems, techniques, or methods described herein may serve as non-limiting Examples are implemented in hardware, software, firmware, special purpose circuits or logic, general purpose hardware or controllers or other computing devices, or some combination thereof.
在上面详细描述的本公开的示例实施例仅仅是说明性的,而不是限制性 的。本领域技术人员应该理解,在不脱离本公开的原理和精神的情况下,可 对这些实施例或其特征进行各种修改和组合,这样的修改应落入本公开的范 围内。The exemplary embodiments of the present disclosure described in detail above are illustrative only and not restrictive. Those skilled in the art should understand that without departing from the principle and spirit of the present disclosure, various modifications and combinations can be made to the embodiments or their features, and such modifications should fall within the scope of the present disclosure.
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