CN108680607A - Pipeline crack corrosion monitoring process based on multi-communication potential drop - Google Patents

Pipeline crack corrosion monitoring process based on multi-communication potential drop Download PDF

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CN108680607A
CN108680607A CN201810998931.3A CN201810998931A CN108680607A CN 108680607 A CN108680607 A CN 108680607A CN 201810998931 A CN201810998931 A CN 201810998931A CN 108680607 A CN108680607 A CN 108680607A
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CN108680607B (en
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甘芳吉
黄仕磊
李文洋
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Sichuan University
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Abstract

The present invention provides the pipeline crack corrosion detecting method based on multi-communication potential drop, present invention firstly provides multidirectional current methods, it is passed through exciting current from four different directions, obtain four groups of voltage ratios, according to the relationship of electrode direction of check and voltage ratio, maximum voltage ratio is selected to substitute into depth solving formula, solution obtains the depth of crackle.The multidirectional current method of the present invention makes crack position and angle (complementary angle) range of electric current pole line become 67.5 90 degree from 0 90 degree, significantly improves the precision of crack depth solution.

Description

基于多向交流电位降的管道裂纹腐蚀监测方法Pipeline Crack Corrosion Monitoring Method Based on Multidirectional AC Potential Drop

技术领域technical field

本发明属于管道检测技术领域,尤其涉及基于多向交流电位降的管道裂纹腐蚀监测方法。The invention belongs to the technical field of pipeline detection, and in particular relates to a pipeline crack corrosion monitoring method based on multidirectional alternating current potential drop.

背景技术Background technique

管道腐蚀是油气管线所面临的诸多风险中最危险的一个,70%-90%的管道安全事故由管道腐蚀引发。Pipeline corrosion is the most dangerous of many risks faced by oil and gas pipelines, and 70%-90% of pipeline safety accidents are caused by pipeline corrosion.

目前,常用的管道腐蚀检测技术,包括相对先进的场指纹技术(Field SignatureMethod,FSM),也只对局部腐蚀(localized corrosion)和均匀腐蚀(general corrosion)的检测精度高;最新提出的交流场指纹法(Alternating Current Field SignatureMethod,ACFSM),利用多个频率点的测量数据评估腐蚀深度,能够提高裂纹腐蚀的检测精度,但是该方法要求裂纹方向与电流极连线方向的夹角大于45度,不能求解夹角小于45度的裂纹,当前的电流激励电极的连线方向与管道轴向平行,会限制裂纹缺陷的检测范围。At present, commonly used pipeline corrosion detection technologies, including the relatively advanced Field Signature Method (FSM), only have high detection accuracy for localized corrosion and general corrosion; the latest AC field fingerprint technology Alternating Current Field Signature Method (ACFSM), using the measurement data of multiple frequency points to evaluate the corrosion depth, can improve the detection accuracy of crack corrosion, but this method requires that the angle between the crack direction and the current electrode connection direction is greater than 45 degrees, and cannot To solve cracks with an included angle of less than 45 degrees, the connection direction of current excitation electrodes is parallel to the pipeline axis, which will limit the detection range of crack defects.

因此,为了满足实际的检测需求,深入研究随机裂纹腐蚀检测技术显得极为必要。Therefore, in order to meet the actual detection requirements, it is extremely necessary to study the random crack corrosion detection technology in depth.

发明内容Contents of the invention

本发明的目的在于解决上述现有技术存在的缺陷,提供基于多向交流电位降的管道裂纹腐蚀检测方法,通过向被测管道施加不同方向的激励电流,使裂纹方向与电流极连线方向的夹角(余角)范围从0-90度变为67.5-90度,可以更精确的检测随机裂纹的腐蚀深度。The object of the present invention is to solve the above-mentioned defects in the prior art, and provide a pipeline crack corrosion detection method based on multi-directional AC potential drop. The included angle (complimentary angle) ranges from 0-90 degrees to 67.5-90 degrees, which can detect the corrosion depth of random cracks more accurately.

本发明采用如下技术方案:The present invention adopts following technical scheme:

基于多向交流电位降的管道裂纹腐蚀检测方法,步骤包括:A pipeline crack corrosion detection method based on multi-directional AC potential drop, the steps include:

步骤1.在测试管道的周向上焊接布置若干组测试电极。Step 1. Weld and arrange several groups of test electrodes on the circumference of the test pipeline.

步骤2.信号发生器产生激励信号通过功率放大器产生激励电流,从四个不同方向,向输入电极依次通入激励电流,功率放大器的频率可调整,激励电流幅值可调整。Step 2. The signal generator generates an excitation signal. The excitation current is generated through the power amplifier, and the excitation current is sequentially passed to the input electrode from four different directions. The frequency of the power amplifier can be adjusted, and the amplitude of the excitation current can be adjusted.

步骤3.用高精度锁相放大器测量无裂纹正常管道的电压,得到正常管道测试电压值并输入计算机,再利用高精度锁相放大器分别在测试管道待测区域测量待测电压,将测量结果输入计算机,得到四组不同的电压比值;Step 3. Use a high-precision lock-in amplifier to measure the voltage of a normal pipeline without cracks, obtain the test voltage value of the normal pipeline and input it into the computer, then use a high-precision lock-in amplifier to measure the voltage to be tested in the area to be tested in the test pipeline, and input the measurement results Computer, get four groups of different voltage ratios;

步骤4.根据裂纹方向与电压比值的关系,选择最大的电压比值代入如下深度求解公式,并使用计算机求解:Step 4. According to the relationship between the crack direction and the voltage ratio, select the largest voltage ratio and substitute it into the following depth solution formula, and use a computer to solve it:

步骤5.根据计算机显示的结果得出管道裂纹的深度。Step 5. Obtain the depth of the pipeline crack according to the results displayed by the computer.

进一步的技术方案是,步骤2中,周向上布置的4组测试电极是指,水平方向,竖直方向,对角线方向,其中输入电极与输出电极相对布置,其连线均通过待测试部位。A further technical solution is that in step 2, the four groups of test electrodes arranged in the circumferential direction refer to the horizontal direction, the vertical direction, and the diagonal direction, wherein the input electrodes and the output electrodes are arranged oppositely, and their connections all pass through the parts to be tested .

进一步的技术方案是,步骤3中,利用高精度锁相放大器测试待测区域电压时,输入激励电流的输入电极与输出激励电流的输出电极的连线与测量探针连线测试方向一致。A further technical solution is that in step 3, when using a high-precision lock-in amplifier to test the voltage of the area to be tested, the connection between the input electrode for inputting the excitation current and the output electrode for outputting the excitation current is consistent with the test direction of the measurement probe connection.

优选的技术方案是,功率放大器的频率选择59-500Hz,激励电流幅值选择2A。The preferred technical solution is that the frequency of the power amplifier is selected to be 59-500 Hz, and the amplitude of the excitation current is selected to be 2A.

优选的技术方案是,步骤2中,功率放大器的频率选择100Hz。The preferred technical solution is that in step 2, the frequency of the power amplifier is selected to be 100 Hz.

本发明的有益效果:Beneficial effects of the present invention:

1.本发明首次提出了多向电流法,从四个不同方向通入激励电流,得到四组电压比值,根据电极裂纹方向与电压比值的关系,选择最大的电压比值代入深度求解公式;本发明的多向电流法使得裂纹位置与电流极连线的夹角(余角)范围从0-90度变为67.5-90度,显著提高了裂纹深度和求解精度。1. The present invention proposes the multi-directional current method for the first time, and the excitation current is fed from four different directions to obtain four sets of voltage ratios. According to the relationship between the direction of the electrode crack and the voltage ratio, the maximum voltage ratio is selected and substituted into the depth solution formula; the present invention The multi-directional current method makes the angle (complimentary angle) between the crack position and the current electrode line changed from 0-90 degrees to 67.5-90 degrees, which significantly improves the crack depth and solution accuracy.

2.本发明由于采用交流电位降技术的原理,所以具有激励电流小、测量灵敏度高、抗干扰能力强等优点。2. Since the present invention adopts the principle of AC potential drop technology, it has the advantages of small excitation current, high measurement sensitivity, and strong anti-interference ability.

3.本发明方法与传统的电位降技术ACFSM采用单一的与管道轴线平行激励电流比较而言,本发明方法首次定量求解随机裂纹缺陷的深度,根据仿真和实验数据结果显示,电流流经裂纹缺陷时,裂纹的方向会影响电流场的分布,从而改变测量电极的电压。3. Compared with the traditional potential drop technology ACFSM using a single excitation current parallel to the pipeline axis, the method of the present invention quantitatively solves the depth of random crack defects for the first time. According to the results of simulation and experimental data, the current flows through the crack defects When , the direction of the crack will affect the distribution of the current field, thereby changing the voltage of the measuring electrode.

附图说明Description of drawings

图1为趋肤电流分布示意图;Figure 1 is a schematic diagram of skin current distribution;

图2为表一测试的不同厚度处的电压分布图;Fig. 2 is the voltage distribution diagram at different thicknesses tested in Table 1;

图3(a)、图3(b)、图3(c)、图3(d)、图3(e)为五种裂纹方向与电极连线的示意图;Figure 3(a), Figure 3(b), Figure 3(c), Figure 3(d), and Figure 3(e) are schematic diagrams of five crack directions and electrode connections;

图4为不同角度裂纹的比值深度图;Figure 4 is the ratio depth map of cracks at different angles;

图5为本发明的多向电流测量示意图;Fig. 5 is the schematic diagram of multidirectional current measurement of the present invention;

图6为仿真测试两种裂纹缺陷的最大比值深度图。Fig. 6 is the maximum ratio depth diagram of two kinds of crack defects in the simulation test.

图7为本发明方法的实验装置图;Fig. 7 is the experimental setup figure of the inventive method;

图8为金属平板探针布局示意图;Figure 8 is a schematic diagram of the layout of the metal flat probe;

图9为实验平板背部示意图。Figure 9 is a schematic diagram of the back of the experimental plate.

具体实施方式Detailed ways

为使本发明的目的、技术方案和优点更加清楚,下面本发明中的技术方案进行清楚、完整地描述,显然,所描述的实施例是本发明一部分实施例,而不是全部的实施例。基于本发明中的实施例,本领域普通技术人员在没有作出创造性劳动前提下所获得的所有其他实施例,都属于本发明保护的范围。In order to make the purpose, technical solutions and advantages of the present invention clearer, the following technical solutions in the present invention are clearly and completely described. Obviously, the described embodiments are some embodiments of the present invention, rather than all embodiments. Based on the embodiments of the present invention, all other embodiments obtained by persons of ordinary skill in the art without creative efforts fall within the protection scope of the present invention.

术语解释:Explanation of terms:

1.1、趋肤效应1.1, skin effect

在管道中通以不同频率的交流激励电流(AC),电流分布遵循趋肤效应。趋肤深度δ的计算公式:The alternating current (AC) of different frequencies is passed through the pipeline, and the current distribution follows the skin effect. Calculation formula of skin depth δ:

上式中μr为材料的相对磁导率;μ0为真空磁导率;σ为材料的电导率;f为激励电流的频率。电流分布示意图如图1所示。In the above formula, μ r is the relative magnetic permeability of the material; μ 0 is the vacuum magnetic permeability; σ is the electrical conductivity of the material; f is the frequency of the excitation current. The schematic diagram of current distribution is shown in Fig. 1.

由式(1)可知,施加高频激励电流时,电流集中存在于管道外壁,随着激励电流频率的降低,电流将逐渐向内壁渗透,管道壁中的电流密度J(r)满足公式:It can be seen from formula (1) that when a high-frequency excitation current is applied, the current concentrates on the outer wall of the pipe, and as the frequency of the excitation current decreases, the current will gradually penetrate into the inner wall, and the current density J(r) in the pipe wall satisfies the formula:

其中, in,

式中I是角频率为ω的电流幅值;R是管道的外半径;r是径向距离;J0(kr)是第一类零阶贝塞尔函数,J1(kR)是第一类一阶贝塞尔函数。In the formula, I is the current amplitude with angular frequency ω; R is the outer radius of the pipeline; r is the radial distance; J 0 (kr) is the zero-order Bessel function of the first kind, and J 1 (kR) is the first A class of first-order Bessel functions.

根据电流密度与电压之间的关系,电压值U(r)的表达式为:According to the relationship between current density and voltage, the expression of voltage value U(r) is:

式中l是测量电极的间距。where l is the distance between the measuring electrodes.

将(3)式中的贝塞尔函数用指数函数近似代替,则电压值幅值可表示为:The Bessel function in formula (3) is approximately replaced by an exponential function, then the voltage amplitude can be expressed as:

测量电极与管道外壁的接触深度d0=R-r≈0.5mm,此时通入激励电流后,测量电极测得的电压幅值U可用式(5)表示:The contact depth between the measuring electrode and the outer wall of the pipeline is d 0 =Rr≈0.5mm. At this time, after the excitation current is applied, the voltage amplitude U measured by the measuring electrode can be expressed by formula (5):

管道壁厚为T,未经腐蚀前测得的原始电压值为U(d=0),管道投入生产后,实际测得的电压值为U(d)。当管道内壁的腐蚀缺陷极浅时(d≈0),随着频率的降低始终满足:The wall thickness of the pipeline is T, and the original voltage value measured before corrosion is U (d=0) . After the pipeline is put into production, the actual measured voltage value is U (d) . When the corrosion defect on the inner wall of the pipeline is extremely shallow (d≈0), as the frequency decreases, it always satisfies:

U(d)/U(d=0)≈1;U (d) /U (d=0) ≈1;

若底部存在深度为d的均匀腐蚀缺陷,则当δ=T-d后,测得电压值U(d)保持不变,U(d)/U(d=0)≈m/U(d=0)(m为常数);而当缺陷为裂纹缺陷时,当δ=T-d后,随着频率降低,缺陷“层”周围的电流还会向下渗透,U(d)<m,U(d)/U(d=0)<m/U(d=0)If there is a uniform corrosion defect with a depth of d at the bottom, then when δ=Td, the measured voltage value U (d) remains unchanged, U (d) /U (d=0) ≈m/U (d=0) (m is a constant); and when the defect is a crack defect, when δ=Td, as the frequency decreases, the current around the defect "layer" will penetrate downward, U (d) <m, U (d) / U (d=0) <m/U (d=0) .

因此裂纹缺陷的U(d)/U(d=0)值可由两种极限情况(无腐蚀缺陷,均匀腐蚀缺陷)下的U(d)/U(d=0)线性叠加近似:Therefore, the U (d) /U (d=0) value of crack defects can be approximated by the linear superposition of U (d) /U (d=0) under the two limit cases (no corrosion defects, uniform corrosion defects):

式中a1,a2,a3为与被测材料特性相关的常数。In the formula, a 1 , a 2 and a 3 are constants related to the properties of the measured material.

1.2、多向电流1.2, multi-directional current

对长度为400mm,内径为140mm,外径为160mm的管道进行有限元分析,有限元软件为COMSOL Multiphysics 5.0。测量区域位于管道中间,探针间距为20mm,注入电流幅值为2A,缺陷深度为2mm、2.5mm、3mm、3.5mm、4mm、4.5mm、5mm、5.5mm、6mm。A finite element analysis is performed on a pipe with a length of 400mm, an inner diameter of 140mm, and an outer diameter of 160mm. The finite element software is COMSOL Multiphysics 5.0. The measurement area is located in the middle of the pipeline, the probe spacing is 20mm, the injection current amplitude is 2A, and the defect depth is 2mm, 2.5mm, 3mm, 3.5mm, 4mm, 4.5mm, 5mm, 5.5mm, 6mm.

材料参数见表1:The material parameters are shown in Table 1:

由公式(3)可知激励电流频率不同时,不同“厚度层”处的电压分布不同,为了保证渗透电流接触到“缺陷层”,需要设定合适的激励电流,以直流时各径向距离处电压(电压等值分布)为基准,通入频率为2.5KHz和500Hz时电压分布,如图2所示。It can be known from formula (3) that when the excitation current frequency is different, the voltage distribution at different "thickness layers" is different. In order to ensure that the permeation current touches the "defect layer", it is necessary to set a suitable excitation current. The voltage (voltage equivalent distribution) is used as the reference, and the voltage distribution is shown in Figure 2 when the input frequency is 2.5KHz and 500Hz.

从图中可以看出,激励电流频率过高,如2.5KHZ时,电流无法完全渗透管道壁,在这种情况下,渗透电流无法接触到深度浅的“缺陷层”,测得信号不能反映缺陷信息;降低激励电流频率,趋肤深度增加,渗透电流能达到各个深度的“缺陷层”,如频率为500Hz时。It can be seen from the figure that if the excitation current frequency is too high, such as 2.5KHZ , the current cannot completely penetrate the pipeline wall. In this case, the penetration current cannot touch the shallow "defect layer", and the measured signal cannot reflect Defect information: reduce the excitation current frequency, increase the skin depth, and the penetration current can reach the "defect layer" at various depths, such as when the frequency is 500Hz.

考虑到管道壁厚为10mm,最大趋肤深度为10mm即可,根据公式(1)及表1参数可以计算出此时对应的电流频率为59Hz。Considering that the pipe wall thickness is 10mm, the maximum skin depth is 10mm. According to the formula (1) and the parameters in Table 1, the corresponding current frequency at this time can be calculated as 59Hz.

以图3(b)、图3(e)四种位置缺陷为例(为裂纹方向与电极连线方向的夹角)。Taking the four positional defects in Figure 3(b) and Figure 3(e) as examples ( is the angle between the crack direction and the electrode connection direction).

图3(a)为无缺陷管道,此时测得的电压值为U(d=0,f=100Hz),作为原始电压:Figure 3(a) is a non-defective pipeline, and the measured voltage value at this time is U(d=0,f=100Hz), which is used as the original voltage:

将图3(b)-图3(e)四种位置的缺陷在不同深度下测得电压值U(d)与U(d=0)作比,得到的结果如图4所示。Comparing the measured voltage values U (d) and U (d=0) at different depths of the defects in the four positions in Figure 3(b)-Figure 3(e), the results are shown in Figure 4.

由图4可知,当裂纹方向与电极连线方向的夹角小于45°时,U(d)/U(d=0)的值与裂纹深度的关系不符合公式(6),此时U(d)/U(d=0)不能用于求解缺陷深度;It can be seen from Figure 4 that when the angle between the crack direction and the electrode connection direction When it is less than 45°, the relationship between the value of U (d) /U (d=0) and the crack depth does not conform to the formula (6), and at this time U (d) /U (d=0) cannot be used to solve the defect depth;

大于45°时,越接近90°,U(d)/U(d=0)的值与裂纹深度的关系越遵循式(6)的指数分布形式,将U(d)/U(d=0)的代入式(6)后计算的裂纹深度越接近实际深度,为90°时求解精度可以达到97.16%;同时仿真数据也显示处:越接近90度,U(d)/U(d=0)的值越大。when When greater than 45°, The closer to 90°, the more the relationship between the value of U (d) /U (d=0) and the crack depth follows the exponential distribution form of formula (6). Substituting the value of U (d) /U (d=0) into the formula ( 6) The closer the calculated crack depth is to the actual depth, When it is 90°, the solution accuracy can reach 97.16%; at the same time, the simulation data is also displayed: The closer to 90 degrees, the larger the value of U (d) /U (d=0) .

因此,对于随机裂纹的深度求解问题,利用越接近90度,测量精度越高的特点,创新性的提出了多向电流法。通过增加三组激励电流,使得范围从0-90°变为67.5-90度,图5为测量示意图。Therefore, for the depth solution problem of random cracks, using The closer to 90 degrees, the higher the measurement accuracy, innovatively proposed the multi-directional current method. By increasing three groups of excitation currents, making The range changes from 0-90° to 67.5-90°. Figure 5 is a schematic diagram of the measurement.

同一缺陷在同一频率下可以获得一组表征信号:A set of characteristic signals can be obtained for the same defect at the same frequency:

取最大的U(d)/U(d=0)值代入公式(6)求解裂纹深度。Take the maximum U (d) /U (d=0) value and substitute it into formula (6) to solve the crack depth.

2、基于多向交流电位降的管道裂纹腐蚀检测方法,步骤包括:2. A pipeline crack corrosion detection method based on multi-directional AC potential drop, the steps include:

步骤1.在测试管道的周向上焊接布置若干组测试电极。Step 1. Weld and arrange several groups of test electrodes on the circumference of the test pipeline.

步骤2.信号发生器产生激励信号通过功率放大器产生激励电流,从四个不同方向,向输入电极依次通入激励电流,功率放大器的频率可调整,激励电流幅值可调整。Step 2. The signal generator generates an excitation signal. The excitation current is generated through the power amplifier, and the excitation current is sequentially passed to the input electrode from four different directions. The frequency of the power amplifier can be adjusted, and the amplitude of the excitation current can be adjusted.

步骤3.用高精度锁相放大器测量无裂纹正常管道的电压,得到正常管道测试电压值并输入计算机,再利用高精度锁相放大器分别在测试管道待测区域测量待测电压,将测量结果输入计算机,得到四组不同的电压比值;Step 3. Use a high-precision lock-in amplifier to measure the voltage of a normal pipeline without cracks, obtain the test voltage value of the normal pipeline and input it into the computer, then use a high-precision lock-in amplifier to measure the voltage to be tested in the area to be tested in the test pipeline, and input the measurement results Computer, get four groups of different voltage ratios;

步骤4.根据裂纹方向与电压比值的关系,选择最大的电压比值代入如下深度求解公式,并使用计算机求解:Step 4. According to the relationship between the crack direction and the voltage ratio, select the largest voltage ratio and substitute it into the following depth solution formula, and use a computer to solve it:

步骤5.根据计算机显示的结果得出管道裂纹的深度。Step 5. Obtain the depth of the pipeline crack according to the results displayed by the computer.

进一步的技术方案是,步骤2中,周向上布置的4组测试电极是指,水平方向,竖直方向,对角线方向,其中输入电极与输出电极相对布置,其连线均通过待测试部位。A further technical solution is that in step 2, the four groups of test electrodes arranged in the circumferential direction refer to the horizontal direction, the vertical direction, and the diagonal direction, wherein the input electrodes and the output electrodes are arranged oppositely, and their connections all pass through the parts to be tested .

进一步的技术方案是,步骤3中,利用高精度锁相放大器测试待测区域电压时,输入激励电流的输入电极与输出激励电流的输出电极的连线与测量探针连线测试方向一致。A further technical solution is that in step 3, when using a high-precision lock-in amplifier to test the voltage of the area to be tested, the connection between the input electrode for inputting the excitation current and the output electrode for outputting the excitation current is consistent with the test direction of the measurement probe connection.

优选的技术方案是,功率放大器的频率选择59-500Hz,激励电流幅值选择2A。The preferred technical solution is that the frequency of the power amplifier is selected to be 59-500 Hz, and the amplitude of the excitation current is selected to be 2A.

优选的技术方案是,步骤2中,功率放大器的频率选择100Hz。The preferred technical solution is that in step 2, the frequency of the power amplifier is selected to be 100 Hz.

3.实施例1.利用一平板模型进行仿真测试3. Embodiment 1. Utilize a plate model to carry out simulation test

先对平板模型进行精确求解。The flat plate model is firstly solved accurately.

平板长220mm,宽220mm,厚度为10mm,测量探针间距为20mm,注入电流幅值为2A,频率为100HZ,详见如图6所示。The length of the plate is 220mm, the width is 220mm, the thickness is 10mm, the distance between the measuring probes is 20mm, the amplitude of the injected current is 2A, and the frequency is 100HZ, as shown in Figure 6 for details.

缺陷深度为2mm、2.5mm、3mm、4mm、4.5mm、5mm、5.5mm、6mm,材料参数如下表2:The defect depth is 2mm, 2.5mm, 3mm, 4mm, 4.5mm, 5mm, 5.5mm, 6mm, and the material parameters are as follows in Table 2:

以0度裂纹缺陷和45度裂纹缺陷为例,二者在上述仿真条件下获得的测量结果为:Taking the 0-degree crack defect and the 45-degree crack defect as examples, the measurement results obtained by the two under the above simulation conditions are:

取0度缺陷的值做深度拟合,公式为:Take the value of 0 degree defect for depth fitting, the formula is:

45度缺陷用公式(7)计算的结果如上表2所示。The results calculated by formula (7) for 45-degree defects are shown in Table 2 above.

实施例2利用5块铝板做测试Embodiment 2 utilizes 5 aluminum plates to do the test

实验材料:5块220mm×220mm×10mm的铝板,整体实验装置如图7-8所示。Experimental materials: five aluminum plates of 220mm×220mm×10mm. The overall experimental device is shown in Figure 7-8.

在未加工缺陷前,依次由Iin1、Iin2、Iin3、Iin4电极向平板注入2A,100Hz的交流电,如图5,图8所示,用高精密数字锁相放大器SR850分别测量探针对(P1-P2)、(P1-P3)、(P2-P3)、(P2-P4)间的原始电压U1(d=0)、U2(d=0)、U3(d=0)、U4(d=0)Before the defects are not processed, 2A, 100Hz alternating current is injected into the plate from the I in1 , I in2 , I in3, and I in4 electrodes in sequence, as shown in Figure 5 and Figure 8, and the probes are measured with a high-precision digital lock-in amplifier SR850 The original voltage U 1 ( d = 0 ) and U 2 ( d = 0 ) , U 3(d=0) , U 4(d=0) .

接着,在5块平板底部分别刻画出5条裂纹,其中1-3号平板为0度裂纹缺陷,深度分别为2mm、4mm、6mm,宽度均为2mm;4-5号平板为45度裂纹缺陷,深度分布为3mm、5mm,如图9所示。Then, 5 cracks were drawn on the bottom of the 5 plates respectively, among which No. 1-3 plates are 0 degree crack defects, the depths are 2mm, 4mm, 6mm respectively, and the width is 2mm; No. 4-5 plates are 45 degree crack defects , and the depth distribution is 3mm and 5mm, as shown in Figure 9.

然后,由Iin1、Iin2、Iin3、Iin4电极,见如图8所示,依次可向平板注入2A电流,59-500Hz交流电,本次实验优选使用100Hz的交流电,测量U1(d)、U2(d)、U3(d)、U4(d)Then, from the I in1 , I in2 , I in3 , and I in4 electrodes, as shown in Figure 8, 2A current, 59-500Hz alternating current can be injected into the plate in turn, and 100Hz alternating current is preferably used in this experiment to measure U 1(d ) , U 2(d) , U 3(d) , U 4(d) .

将测得电压与原始电压作比值,得到的结果如下表3所示:The measured voltage is compared with the original voltage, and the results obtained are shown in Table 3 below:

注:U10=U1(d=0),U20=U2(d=0),U30=U3(d=0),U40=U4(d=0)Note: U 10 =U 1(d=0) , U 20 =U 2(d=0) , U 30 =U 3(d=0) , U 40 =U 4(d=0) .

将每个深度对应的最大U(d)/U(d=0)值代入公式(7),结果如下表4所示。Substituting the maximum value of U (d) /U (d=0) corresponding to each depth into formula (7), the results are shown in Table 4 below.

因此,与以往随机位置缺陷不能检测的情况相比,多向电流法能够求解随机裂纹深度。Therefore, compared with the previous situation where random position defects cannot be detected, the multi-directional current method can solve the random crack depth.

用公式(7)中电压比值求解深度的方法,可以消除环境干扰,提高了测量系统的抗干扰能力。Using the voltage ratio in formula (7) to solve the depth method can eliminate environmental interference and improve the anti-interference ability of the measurement system.

结论分析:Conclusion analysis:

传统的电位降技术采用单一的与管道轴线平行激励电流,本发明利用电流与裂纹的夹角为90度时,测量电压与原始电压比值最大、同时比值与缺陷深度函数特性最好的特点,从四个方向通入交流激励电流,使得的范围从0-90度变为67.5-90度,选择最大的电压比值计算缺陷深度。The traditional potential drop technology uses a single excitation current parallel to the pipeline axis, and the present invention utilizes the angle between the current and the crack When the temperature is 90 degrees, the ratio of the measured voltage to the original voltage is the largest, and the ratio and the defect depth function characteristics are the best at the same time. The AC excitation current is fed from four directions, so that The range is changed from 0-90 degrees to 67.5-90 degrees, and the maximum voltage ratio is selected to calculate the defect depth.

仿真测试的实验数据显示,新的计算方法提高了随机裂纹的检测精度,可以更有效的检测腐蚀情况。The experimental data of the simulation test shows that the new calculation method improves the detection accuracy of random cracks and can detect corrosion more effectively.

最后应说明的是:以上实施例仅用以说明本发明的技术方案,而非对其限制;尽管参照前述实施例对本发明进行了详细的说明,本领域的普通技术人员应当理解:其依然可以对前述各实施例所记载的技术方案进行修改,或者对其中部分技术特征进行等同替换;而这些修改或者替换,并不使相应技术方案的本质脱离本发明各实施例技术方案的精神和范围。Finally, it should be noted that: the above embodiments are only used to illustrate the technical solutions of the present invention, rather than to limit them; although the present invention has been described in detail with reference to the foregoing embodiments, those of ordinary skill in the art should understand that: it can still be Modifications are made to the technical solutions described in the foregoing embodiments, or equivalent replacements are made to some of the technical features; and these modifications or replacements do not make the essence of the corresponding technical solutions deviate from the spirit and scope of the technical solutions of the various embodiments of the present invention.

Claims (5)

1. The pipeline crack corrosion detection method based on the multidirectional alternating current potential drop is characterized by comprising the following steps of:
step 1, welding and arranging a plurality of groups of test electrodes in the circumferential direction of a test pipeline;
step 2, the signal generator generates an excitation signal and generates an excitation current through the power amplifier, the excitation current is sequentially introduced to the input electrode from four different directions, the frequency of the power amplifier can be adjusted, and the amplitude of the excitation current can be adjusted;
step 3, measuring the voltage of the crack-free normal pipeline by using a high-precision phase-locked amplifier to obtain a normal pipeline test voltage value, inputting the normal pipeline test voltage value into a computer, measuring the voltage to be measured in the area to be measured of the test pipeline by using the high-precision phase-locked amplifier, and inputting the measurement result into the computer to obtain four groups of different voltage ratios;
and 4, selecting the maximum voltage ratio to substitute the following depth solving formula according to the relation between the crack direction and the voltage ratio, and solving by using a computer:
and 5, obtaining the depth of the pipeline crack according to the result displayed by the computer.
2. The method for detecting the pipeline crack corrosion based on the multi-directional alternating current potential drop is characterized in that in the step 2, the frequency of a power amplifier is selected to be 59-500Hz, and the amplitude of an excitation current is selected to be 2A.
3. The method for detecting pipeline crack corrosion based on multidirectional alternating current potential drop as claimed in claim 2, wherein the frequency of the power amplifier is selected to be 100 Hz.
4. The method for detecting pipeline crack corrosion based on multi-directional alternating current potential drop as claimed in claim 1, wherein in step 2, 4 groups of test electrodes arranged in the circumferential direction are in the horizontal direction, the vertical direction and the diagonal direction, wherein the input electrode and the output electrode are arranged oppositely, and the connecting lines of the input electrode and the output electrode pass through the part to be tested.
5. The method for detecting pipeline crack corrosion based on multi-directional alternating current potential drop as claimed in claim 1, wherein in step 3, when the high-precision phase-locked amplifier is used for testing the voltage of the area to be tested, the connection line of the input electrode for inputting the excitation current and the output electrode for outputting the excitation current is consistent with the connection line test direction of the measurement probe.
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