CN114526810A - Frequency measurement method of vibrating wire type sensor - Google Patents

Frequency measurement method of vibrating wire type sensor Download PDF

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CN114526810A
CN114526810A CN202111632216.6A CN202111632216A CN114526810A CN 114526810 A CN114526810 A CN 114526810A CN 202111632216 A CN202111632216 A CN 202111632216A CN 114526810 A CN114526810 A CN 114526810A
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frequency
sensor
sweep
vibrating wire
range
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赵雄
晁鹏飞
何杰
陈亚亮
蓝启强
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Fujian Yongzheng Construction Quality Inspection Co Ltd
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Fujian Yongzheng Construction Quality Inspection Co Ltd
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    • G01MEASURING; TESTING
    • G01HMEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
    • G01H13/00Measuring resonant frequency

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Abstract

The invention discloses a frequency measuring method of a vibrating wire type sensor, and belongs to the technical field of health monitoring. The method comprises the steps of firstly carrying out full-frequency scanning to obtain the response frequency of a sensor, carrying out frequency scanning in a second scanning process by taking the response frequency obtained in the first scanning process as a median value and reducing a frequency scanning range, wherein the obtained frequency is compared with the response frequency obtained in the first scanning process; if the difference value of the two acquired frequencies meets the requirement, determining the initial frequency of the sensor to be the average value of the sum of the first response frequency and the second response frequency; the method has the advantages of short measurement period and high precision, greatly reduces the labor input and labor intensity, improves the measurement efficiency and reduces the application difficulty of the vibrating wire sensor.

Description

一种振弦式传感器的频率测量方法A frequency measurement method of a vibrating wire sensor

技术领域technical field

本发明涉及一种振弦式传感器的频率测量方法,属于健康监测技术领域。The invention relates to a frequency measurement method of a vibrating wire sensor, belonging to the technical field of health monitoring.

背景技术Background technique

随着经济和科学技术的快速发展,越来越多的大型复杂工程结构体得以兴建,如大跨度桥梁、体育馆、高层建筑、水利设施等,这些工程结构体对保障人民生命、财产安全非常重要。通常采用振弦式传感器来监测工程的压力,位移,温度,形变量,渗漏等物理量,以此来判定工程项目的运行状况,预测一些地质灾害或者项目漏洞。为保证大型结构体的安全使用,建立可靠的结构体健康监测系统十分必要。With the rapid development of economy and science and technology, more and more large-scale complex engineering structures have been built, such as long-span bridges, gymnasiums, high-rise buildings, water conservancy facilities, etc. These engineering structures are very important to protect people's lives and property safety. . Vibrating wire sensors are usually used to monitor the pressure, displacement, temperature, deformation, leakage and other physical quantities of the project, so as to determine the operation status of the project and predict some geological disasters or project loopholes. In order to ensure the safe use of large structures, it is necessary to establish a reliable structural health monitoring system.

振弦式传感器,主要有单线圈和双线圈两种结构,其中,单线圈是指激励线圈和拾振线圈为同一个线圈的结构,其振弦一端固定,另一端连结在弹性感压膜片上。弦的中部装有一块软铁,置于磁铁和线圈构成的激励器的磁场中。激励器在停止激励时兼作拾振器。工作时,振弦在激励器的激励下振动,其振动频率与膜片所受压力的大小有关,在停止激励时,该线圈又能当做拾振线圈,检测到振弦振动产生的电动势。通过测该电动势的频率,即可测得振弦的频率。单线圈结构的缺点是无法连续测量,但是装置简单稳定。双线圈结构是指激励线圈和拾振线圈分开,一般采取电磁法,电磁法采用两个装有线圈的磁铁,分别作为激励线圈和拾振线圈。拾振线圈的感应信号被放大后又送至激励线圈去补充振动的能量。为减小传感器非线性对测量精度的影响,需要选择适中的最佳工作频段和设置预应力,或采用在感压膜的两侧各设一根振弦的差动式结构。双线圈结构可连续测量,测量精度也更好,可是结构较为复杂,稳定性不好。The vibrating wire sensor mainly has two structures: single coil and double coil. Among them, the single coil refers to the structure in which the excitation coil and the pickup coil are the same coil. One end of the vibrating wire is fixed, and the other end is connected to the elastic pressure-sensitive membrane. a. The middle of the string is equipped with a piece of soft iron, which is placed in the magnetic field of the exciter formed by the magnet and the coil. The exciter doubles as a vibration pickup when the excitation is stopped. During operation, the vibrating wire vibrates under the excitation of the exciter, and its vibration frequency is related to the magnitude of the pressure on the diaphragm. When the excitation is stopped, the coil can also be used as a pickup coil to detect the electromotive force generated by the vibration of the vibrating wire. By measuring the frequency of the electromotive force, the frequency of the vibrating wire can be measured. The disadvantage of the single-coil structure is that it cannot be continuously measured, but the device is simple and stable. The double-coil structure means that the excitation coil and the pickup coil are separated, and the electromagnetic method is generally adopted. The electromagnetic method uses two magnets equipped with coils, which are used as the excitation coil and the pickup coil respectively. The induction signal of the pickup coil is amplified and sent to the excitation coil to supplement the vibration energy. In order to reduce the influence of the sensor nonlinearity on the measurement accuracy, it is necessary to select a moderate optimal working frequency band and set the prestress, or adopt a differential structure with a vibrating wire on each side of the pressure-sensitive membrane. The double-coil structure can be continuously measured, and the measurement accuracy is better, but the structure is more complicated and the stability is not good.

振弦式传感器振荡的固有频率存在一个大致范围,通常为400-4500HZ。根据物理学中的共振原理,当作用到传感器上的激励信号的频率与传感器钢弦固有频率接近或相等时,钢弦发生共振。共振状态下,钢弦振荡的幅度较大。振弦式传感器激振模式有两种,一种是高压拨弦激振,一种是低压扫频激振。There is an approximate range for the natural frequency of vibration of a vibrating wire sensor, usually 400-4500 Hz. According to the resonance principle in physics, when the frequency of the excitation signal applied to the sensor is close to or equal to the natural frequency of the steel string of the sensor, the steel string will resonate. In the resonance state, the steel string oscillates with a larger amplitude. There are two excitation modes for vibrating wire sensors, one is high-voltage strumming excitation, and the other is low-voltage sweeping excitation.

发明内容SUMMARY OF THE INVENTION

针对现有的振弦式传感器的频率测量方式的不足,本发明提供一种振弦式传感器的频率测量方法,大大提高了测量精度、测量效率以及测量的稳定性,同时降低了传感器的损耗。Aiming at the shortcomings of the existing frequency measurement methods of the vibrating wire sensor, the present invention provides a frequency measurement method of the vibrating wire sensor, which greatly improves the measurement accuracy, measurement efficiency and measurement stability, and reduces the loss of the sensor.

一种振弦式传感器的频率测量方法,包括以下步骤:A frequency measurement method of a vibrating wire sensor, comprising the following steps:

步骤1,首次测量时,根据振弦式传感器频率范围分布范围以一定的步进频率进行全频段低电压扫频,执行步骤2;Step 1: During the first measurement, perform a full-band low-voltage sweep at a certain step frequency according to the frequency range distribution of the vibrating wire sensor, and perform step 2;

步骤2,判断是否存在响应频率f1,若存在,则将测量得到的频率加权计算得到f1存入存储器中后执行步骤3;否则,缩小扫描的步进频率返回步骤1;Step 2, determine whether there is a response frequency f 1 , if there is, then perform step 3 after the frequency weighted calculation obtained by measurement is obtained f 1 is stored in the memory; otherwise, the step frequency of the reduced scan returns to step 1;

步骤3,以首次频率f1为中值,缩小扫频范围,减小步进频率进行扫频,则将测量得到的频率通过取中位数f2存入存储器中,执行步骤4;Step 3, take the first frequency f 1 as the median, reduce the frequency sweep range, reduce the step frequency to sweep the frequency, then store the measured frequency in the memory by taking the median f 2 , and execute step 4;

步骤4,判断是频率f1和频率f2之间差值是否符合要求,若符合,执行步骤5;否则,返回步骤1执行;Step 4, judge whether the difference between the frequency f 1 and the frequency f 2 meets the requirements, if so, go to step 5; otherwise, return to step 1 to execute;

步骤5,把f3存入存储器中,作为传感器频率的初始值,执行步骤6;Step 5, store f3 in the memory as the initial value of the sensor frequency, and execute step 6;

步骤6,以首次频率f3为中值,缩小扫频范围,减小步进频率进行扫频,得到传感器响应频率f,执行步骤7;Step 6, take the initial frequency f3 as the median value, reduce the frequency sweep range, reduce the step frequency to sweep the frequency, obtain the sensor response frequency f, and perform step 7;

步骤7,判断是频率f和频率f3之间差值是否符合要求,若符合,执行步骤8;否则,返回步骤1执行;Step 7, determine whether the difference between the frequency f and the frequency f 3 meets the requirements, if so, execute step 8; otherwise, return to step 1 to execute;

步骤8,输出传感器的频率f。Step 8, output the frequency f of the sensor.

优选的,步骤1中,所述的振弦式传感器频率范围分布范围为400Hz-6000Hz。Preferably, in step 1, the frequency distribution range of the vibrating wire sensor is 400Hz-6000Hz.

优选的,步骤1或3或6中,所述的步进频率为每次扫频所增加的Δf。Preferably, in step 1 or 3 or 6, the step frequency is Δf that is increased by each frequency sweep.

优选的,步骤2中,所述的加权计算为`x=(x1f1+x2f2+x3f3+…+xkfk)/∑1 kfi,其中xk是每次相邻频率数据,fk是每个差值的权重,随着距离时间的增加,权重从10到1递减。Preferably, in step 2, the weighting calculation is `x=(x 1 f 1 +x 2 f 2 +x 3 f 3 +...+x k f k )/∑ 1 k f i , where x k is For each adjacent frequency data, fk is the weight of each difference, and the weight decreases from 10 to 1 as the distance time increases.

优选的,5.根据权利要求1所述的振弦式传感器的频率测量方法,其特征在于,步骤3及步骤6中,所述的扫频范围对应为(f1±10)Hz和(f3±10)Hz。Preferably, 5. The method for measuring the frequency of a vibrating wire sensor according to claim 1, wherein in steps 3 and 6, the frequency sweep range corresponds to (f 1 ±10) Hz and (f 3 ±10) Hz.

优选的,步骤4或7中,f1和频率f2之间差值要求为绝对值小于5Hz和f和频率f3之间差值要求为绝对值小于5Hz。Preferably, in step 4 or 7, the difference between f 1 and frequency f 2 is required to be less than 5 Hz in absolute value, and the difference between f and frequency f 3 is required to be less than 5 Hz in absolute value.

优选的,步骤5中f3为(f1+f2)/2。Preferably, in step 5, f 3 is (f 1 +f 2 )/2.

本发明在后续扫频测量时,每一次测量都初始频率结果为中值,能迅速确定大致频率范围,避免了传统扫频测量定位慢,需要测量速度慢的缺点,同时,每次扫频的频段受近期测量结果影响,实际测量时,历史数据越来越多,扫频范围越来越小,在每次扫频采样次数一定的情况下,每一次扫频精度都比前一次高。如果扫描的的当前频率和初始值相差太大,会重新校准初始值。具有高精度,高效率的特点。本发明有测量周期短、精度高的优点,大大降低人工投入和劳动强度、提高了测量效率,降低了振弦传感器的应用难度。In the subsequent frequency sweep measurement, the initial frequency result of each measurement is the median value, and the approximate frequency range can be quickly determined, avoiding the disadvantages of slow positioning and slow measurement speed in the traditional sweep frequency measurement. The frequency band is affected by the recent measurement results. During the actual measurement, there are more and more historical data, and the frequency sweep range is getting smaller and smaller. Under the condition of a certain number of sampling times for each frequency sweep, the accuracy of each frequency sweep is higher than the previous one. If the scanned current frequency is too different from the initial value, the initial value will be re-calibrated. It has the characteristics of high precision and high efficiency. The invention has the advantages of short measurement period and high precision, greatly reduces labor input and labor intensity, improves measurement efficiency, and reduces the application difficulty of the vibrating wire sensor.

采用本发明的测量方法,当扫频范围内无符合要求的振动频率时,可以采用重新采到初始值原始重置法,确保了本方法测量的可靠性。With the measurement method of the present invention, when there is no vibration frequency that meets the requirements within the frequency sweep range, the original reset method can be adopted to re-collect the initial value, which ensures the reliability of the measurement of the method.

附图说明Description of drawings

图1为本发明振弦式传感器的频率测量方法的流程示意图。FIG. 1 is a schematic flowchart of the frequency measurement method of the vibrating wire sensor of the present invention.

具体实施方式Detailed ways

下面结合说明书附图对本发明的实施方式进行描述。Embodiments of the present invention will be described below with reference to the accompanying drawings.

如图1所示,本发明为一种振弦式传感器的频率测量方法,包括以下步骤:As shown in Figure 1, the present invention is a frequency measurement method of a vibrating wire sensor, comprising the following steps:

步骤1,首次测量时,根据振弦式传感器频率范围分布范围以一定的步进频率进行全频段低电压扫频,执行步骤2;Step 1: During the first measurement, perform a full-band low-voltage sweep at a certain step frequency according to the frequency range distribution of the vibrating wire sensor, and perform step 2;

步骤2,判断是否存在响应频率f1,若存在,则将测量得到的频率加权计算得到f1存入存储器中后执行步骤3;否则,缩小扫描的步进频率返回步骤1;Step 2, determine whether there is a response frequency f 1 , if there is, then perform step 3 after the frequency weighted calculation obtained by measurement is obtained f 1 is stored in the memory; otherwise, the step frequency of the reduced scan returns to step 1;

步骤3,以首次频率f1为中值,缩小扫频范围,减小步进频率进行扫频,则将测量得到的频率通过取中位数f2存入存储器中,执行步骤4;Step 3, take the first frequency f 1 as the median, reduce the frequency sweep range, reduce the step frequency to sweep the frequency, then store the measured frequency in the memory by taking the median f 2 , and execute step 4;

步骤4,判断是频率f1和频率f2之间差值是否符合要求,若符合,执行步骤5;否则,返回步骤1执行;Step 4, judge whether the difference between the frequency f 1 and the frequency f 2 meets the requirements, if so, go to step 5; otherwise, return to step 1 to execute;

步骤5,把f3存入存储器中,作为传感器频率的初始值,执行步骤6;Step 5, store f3 in the memory as the initial value of the sensor frequency, and execute step 6;

步骤6,以首次频率f3为中值,缩小扫频范围,减小步进频率进行扫频,得到传感器响应频率f,执行步骤7;Step 6, take the initial frequency f3 as the median value, reduce the frequency sweep range, reduce the step frequency to sweep the frequency, obtain the sensor response frequency f, and perform step 7;

步骤7,判断是频率f和频率f3之间差值是否符合要求,若符合,执行步骤8;否则,返回步骤1执行;Step 7, determine whether the difference between the frequency f and the frequency f 3 meets the requirements, if so, execute step 8; otherwise, return to step 1 to execute;

步骤8,输出传感器的频率f。Step 8, output the frequency f of the sensor.

下面举实例说明,例子中采用长沙金码测控科技股份有限公司生产的振弦式应力计,其编号为101,规格为-1500με-+1500με,电阻为470欧姆,线长18m。The following is an example to illustrate. In the example, a vibrating wire stress gauge produced by Changsha Jinma Measurement and Control Technology Co., Ltd. is used.

首先,将该传感器安装在现场的采集系统中,给传感器施加应力500με,此时理论的频率因为1860HZ。采集系统工作时,首次测量开始,采用的低压扫频对线圈进行激励,扫频范围为400HZ-6000HZ,步进值为50HZ,即用450,500,550…6000HZ等频率的低电压信号依次激励传感器线圈。此单线圈传感器的激振线圈即为拾振线圈,通过拾振线圈测得当扫频电压为1855HZ时,其共振幅度最大,且其共振电动势强度大于最小强度,因此首次测量频率结果为1860HZ,f1=1850HZ。First, install the sensor in the on-site acquisition system, apply a stress of 500με to the sensor, and the theoretical frequency at this time is 1860HZ. When the acquisition system is working, the first measurement starts, and the low-voltage sweep frequency is used to excite the coil, the sweep frequency range is 400HZ-6000HZ, and the step value is 50HZ, that is, the low-voltage signal of 450, 500, 550...6000HZ and other frequencies is used to sequentially stimulate sensor coil. The excitation coil of this single-coil sensor is the pickup coil. When the frequency sweep voltage is 1855HZ measured by the pickup coil, its resonance amplitude is the largest, and its resonance electromotive force strength is greater than the minimum strength, so the first measurement frequency result is 1860HZ, f 1 = 1850Hz.

然后,系统中的嵌入式控制器,将获得的f1存取系统的存储器;Then, the embedded controller in the system will access the memory of the system with the obtained f1;

第二次测量频率时,控制器读取存储器中的历史数据,f1=1855HZ。此时,第二次扫频测量的扫频中值为前一次的结果,即中值等于f1,扫频范围为f1±10,步进值为1HZ,即用1745,1746,1757…1965等频率的低电压信号依次激励传感器线圈,得到最大共振频率为1860HZ,同时确认该频率下的共振电动势强度大于最小强度,因此f2=1860HZ,将f2存入存储器。When measuring the frequency for the second time, the controller reads the historical data in the memory, f 1 =1855HZ. At this time, the sweep frequency median value of the second sweep frequency measurement is the result of the previous time, that is, the median value is equal to f 1 , the sweep frequency range is f 1 ±10, and the step value is 1HZ, that is, 1745, 1746, 1757… The low-voltage signal of 1965 and other frequencies excites the sensor coil in turn, and the maximum resonant frequency is 1860HZ. At the same time, it is confirmed that the resonant electromotive force intensity at this frequency is greater than the minimum intensity, so f 2 =1860HZ, and f 2 is stored in the memory.

比较f1和f2的频率差值小与5Hz,f3的频率为(f1+f2)/2=1857.5HZ存入存储器作为传感器的初始频率。Comparing the frequency difference between f 1 and f 2 is smaller than 5Hz, the frequency of f 3 is (f 1 +f 2 )/2=1857.5HZ, which is stored in the memory as the initial frequency of the sensor.

接着,之后的测量,控制器取存储器中的历史数据,f3=1857.5,此时,低压扫频的中值为f3扫频结果,即为1857.5HZ,扫频频段为f3±5,步进值为1HZ,即用1852,1853,1854,1859…1830等频率的低电压信号依次激励传感器线圈,得到最大共振频率为1860HZ,因此f=1860HZ,将f存入存储器。Then, in the subsequent measurement, the controller takes the historical data in the memory, f 3 =1857.5, at this time, the median value of the low-voltage sweep frequency is f 3 sweep frequency result, that is, 1857.5HZ, and the sweep frequency band is f 3 ±5, The step value is 1HZ, that is, the sensor coil is excited by low-voltage signals with frequencies of 1852, 1853, 1854, 1859...1830 in turn, and the maximum resonance frequency is 1860HZ, so f=1860HZ, and f is stored in the memory.

以上所述的实施例仅表达了对本发明优选实施方式,其描述较为具体和详细,但本发明不仅限于这些实施例,应当指出的是,对于本领域的普通技术人员来说。在未脱离本发明宗旨的前提下,所为的任何改进均落在本发明的保护范围之内。因此,本发明专利的保护范围应以所附权利要求为准。The above-mentioned embodiments only represent the preferred embodiments of the present invention, and the descriptions thereof are specific and detailed, but the present invention is not limited to these embodiments, and it should be pointed out that those skilled in the art are of ordinary skill in the art. Any improvements made without departing from the spirit of the present invention fall within the protection scope of the present invention. Therefore, the protection scope of the patent of the present invention should be subject to the appended claims.

Claims (7)

1. A frequency measurement method of a vibrating wire sensor is characterized by comprising the following steps:
step 1, during first measurement, performing full-band low-voltage frequency sweeping at a certain stepping frequency according to the frequency range distribution range of the vibrating string type sensor, and executing step 2;
step 2, judging whether a response frequency f exists1If yes, calculating the measured frequency weight to obtain f1Step 3 is executed after the data is stored in the memory; otherwise, the step frequency of the reduced scanning returns to the step 1;
step 3, using the first frequency f1For the median value, the sweep frequency range is narrowed, the step frequency is reduced for sweep frequency, and the measured frequency is subjected to median f2Storing the data into a memory, and executing the step 4;
step 4, judging the frequency f1And frequency f2Whether the difference value meets the requirement or not, if so, executing the step 5; otherwise, returning to the step 1 for execution;
step 5, f is processed3Storing the initial value of the sensor frequency in a memory, and executing the step 6;
step 6, using the first frequency f3For the median value, reducing the sweep frequency range, reducing the step frequency to sweep frequency to obtain the response frequency f of the sensor, and executing the step 7;
step 7, judging whether the frequency f and the frequency f are the same3Whether the difference value meets the requirement or not, if so, executing a step 8; otherwise, returning to the step 1 for execution;
and 8, outputting the frequency f of the sensor.
2. The method for measuring the frequency of the vibrating wire sensor according to claim 1, wherein in step 1, the frequency range of the vibrating wire sensor is distributed in a range of 400Hz to 6000 Hz.
3. The method of claim 1, wherein the step frequency is Δ f increased for each frequency sweep in step 1, 3 or 6.
4. The method as claimed in claim 1, wherein the weight calculation in step 2 is' x = (x) in the method1f1+x2f2+x3f3+…+xkfk)/∑1 kfi
Wherein xkIs each time adjacent frequency data, fkIs the weight of each difference, decreasing from 10 to 1 as the distance time increases.
5. The method according to claim 1, wherein the sweep frequency range in steps 3 and 6 corresponds to (f)110) Hz and (f)3±10)Hz。
6. The method for measuring the frequency of a vibrating wire sensor according to claim 1, wherein in step 4 or 7, f1And frequency f2The difference between f and f is required to be less than 5Hz and f3The difference between them is required to be less than 5Hz in absolute value.
7. The method of claim 1, wherein f is the step 53Is (f)1+f2)/2。
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