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CN113435040B - Inversion method of burst diameter based on transient flow - Google Patents

Inversion method of burst diameter based on transient flow Download PDF

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CN113435040B
CN113435040B CN202110715140.7A CN202110715140A CN113435040B CN 113435040 B CN113435040 B CN 113435040B CN 202110715140 A CN202110715140 A CN 202110715140A CN 113435040 B CN113435040 B CN 113435040B
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CN113435040A (en
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郑国磊
田一梅
彭森
李政翾
程景
梁建文
何楠
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Tianjin University
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Abstract

The invention relates to a method for realizing the inversion of the diameter of a burst pipe, in order to realize the location of the burst pipe in a pipe network, a high-frequency SCADA system is applied to monitor a pressure abnormal signal in the pipe network, and on the basis of the location of the burst pipe, a total monitoring signal is decomposed into branch monitoring signals from each propagation path according to the propagation characteristics of transient flow; inverting the propagation path and characteristics of the transient flow, namely inverting the local loss and the friction loss in the original propagation process to obtain the reciprocal of the local loss and the friction loss, converting the reciprocal of the local loss and the friction loss into gain, inverting the excitation signals from each path, and superposing the excitation signals to form a total inversion excitation signal; and according to the relation between the detonation excitation signal and the detonation diameter, the excitation signal takes the maximum amplitude, the detonation diameter takes the maximum value, and the detonation diameter is calculated. The comparison of the diameter of the detonation calculated by the method with the actual diameter of the detonation and the instantaneous flow attenuation method proves that the positioning precision of the method is higher, and the method can effectively solve the problem of the diameter inversion of the detonation.

Description

基于瞬变流的爆管直径反演方法Inversion method of burst diameter based on transient flow

技术领域technical field

本发明涉及一种爆管直径反演方法,属于工程学领域,具体讲,涉及基于瞬变流的爆管直径反演方法。The invention relates to a method for inversion of the diameter of a burst pipe, belonging to the field of engineering, in particular to a method for inversion of the diameter of a burst pipe based on a transient flow.

背景技术Background technique

供水管网是城市基础设施的重要组成部分,被称为城市的生命线。当爆管发生时,需要根据爆管信息为爆管修复提供决策。近年来,SCADA系统被广泛引入供水管网中,对流量和压力进行实时监测,应用监测数据对爆管进行定位方法有很多,然无法推断爆管面积,这给爆管修复决策带来一定困难。因此,实现爆管口径的反演具有重要意义。The water supply network is an important part of the urban infrastructure and is called the lifeline of the city. When a pipe burst occurs, it is necessary to provide decision-making for burst pipe repair based on the burst pipe information. In recent years, SCADA systems have been widely introduced into the water supply network to monitor flow and pressure in real time. There are many methods for locating burst pipes using monitoring data. However, the area of burst pipes cannot be inferred, which brings certain difficulties to the decision-making of burst pipe repairs. . Therefore, it is of great significance to realize the inversion of the burst diameter.

近年来,SCADA系统中高频压力监测被引入供水管网中,利用该系统监测到的瞬变流可以实现复杂管网的精确的定位,但爆管口径信息难以推断。因此研究一种爆管口径的反演方法对提供爆管修复决策是有必要的。In recent years, high-frequency pressure monitoring in the SCADA system has been introduced into the water supply pipe network. The transient flow monitored by the system can be used to accurately locate the complex pipe network, but it is difficult to infer the burst diameter information. Therefore, it is necessary to study an inversion method for the diameter of the burst pipe to provide the decision of the burst pipe repair.

SCADA系统监测的瞬变流是爆管激发的瞬变流经多路径传播至监测点又叠加形成,在传播途中存在局部损失和摩阻损失。本发明在爆管定位的基础上,将传播路径反向,两种损失换成两种增益,瞬变流从监测点经多路径传播至爆管点叠加后形成激励信号,根据激励信号与爆管口径对应关系计算爆管口径。The transient flow monitored by the SCADA system is the transient flow excited by the burst pipe that propagates through multiple paths to the monitoring point and is superimposed. There are local losses and friction losses during the propagation. Based on the location of the burst pipe, the invention reverses the propagation path, and replaces the two losses with two gains. The transient current propagates from the monitoring point to the burst pipe point through multiple paths to form an excitation signal after superposition. The corresponding relationship of the pipe diameter is used to calculate the burst pipe diameter.

发明内容SUMMARY OF THE INVENTION

针对供水管网中爆管口径难以反演问题,本发明在爆管定位的基础上提出一种基于瞬变流的爆管直径反演方法,有效实现供水管网中爆管口径的反演。为此,本发明的技术方案如下:Aiming at the problem that the diameter of the burst pipe in the water supply pipe network is difficult to invert, the invention proposes a burst pipe diameter inversion method based on transient flow on the basis of the location of the burst pipe, which effectively realizes the inversion of the burst pipe diameter in the water supply pipe network. For this reason, the technical scheme of the present invention is as follows:

一种基于瞬变流的爆管直径反演方法,步骤如下:A method for inversion of burst diameter based on transient flow, the steps are as follows:

S1、根据瞬变流的传播特征,将总的监测信号分解为来自每条传播路径的分支监测信号;S1. According to the propagation characteristics of the transient flow, the total monitoring signal is decomposed into branch monitoring signals from each propagation path;

S2、将瞬变流的传播路径及特征逆向,反演激励信号;S2. Reverse the propagation path and characteristics of the transient flow to invert the excitation signal;

S3、根据爆管激励信号与爆管直径的关系,计算爆管直径。S3. Calculate the diameter of the burst tube according to the relationship between the burst tube excitation signal and the burst tube diameter.

进一步地,在步骤S1中,总的监测信号分解的具体方法为:Further, in step S1, the specific method for decomposing the total monitoring signal is:

根据瞬变流的传播理论,计算在爆管点至监测点的每条传播路径中的传播瞬变流信号,称为分支模拟信号,将其叠加形成总的模拟信号,称为总模拟信号,来自每条传播路径的监测信号振幅可表达为:According to the propagation theory of transient current, the propagation transient current signal in each propagation path from the pipe burst point to the monitoring point is calculated, which is called the branch analog signal, and it is superimposed to form a total analog signal, which is called the total analog signal, The monitoring signal amplitude from each propagation path can be expressed as:

Figure BDA0003134881970000011
Figure BDA0003134881970000011

式(1)中,k为瞬变流的传播路径序号,Ek(t)为分支模拟信号在t时刻的振幅,M(t)为总的监测信号在在t时刻的振幅,εk(t)为在t时刻第k条路径中监测信号所占的比例。In formula (1), k is the propagation path number of the transient flow, E k (t) is the amplitude of the branch analog signal at time t, M(t) is the amplitude of the total monitoring signal at time t, ε k ( t) is the proportion of monitoring signals in the k-th path at time t.

进一步地,在步骤S2中,反演激励信号的具体方法为:Further, in step S2, the specific method of inverting the excitation signal is:

将每条路径中的信号按原路径反向从监测点传播至爆管点,原传播过程中的局部损失和摩阻损失取其倒数,变为增益,则来自每条路径的激励信号振幅表达式为:The signal in each path is propagated from the monitoring point to the burst point in the reverse direction of the original path, and the reciprocal of the local loss and frictional loss in the original propagation process is taken as the gain, and the excitation signal amplitude from each path is expressed as The formula is:

Figure BDA0003134881970000021
Figure BDA0003134881970000021

式(2)中,Tk为瞬变流在第k条路径的传播时间,Aki第i个节点的透射或反射系数,Rkj第j段管段单位长度的摩阻因子,e-Rkj第j段管段单位长度的摩阻损失,Lkj为第j段管段的长度。In formula (2), T k is the propagation time of the transient flow on the k-th path, A ki is the transmission or reflection coefficient of the i-th node, R kj is the friction factor per unit length of the j-th pipe section, and e -Rkj is the The friction loss per unit length of the j-section pipe, L kj is the length of the j-th pipe section.

将来自每条路径的激励信号进行叠加,叠加后的信号即为总的激励信号,其振幅表达式为:The excitation signals from each path are superimposed, and the superimposed signal is the total excitation signal, and its amplitude expression is:

Figure BDA0003134881970000022
Figure BDA0003134881970000022

进一步地,在步骤S3中,计算爆管直径的具体方法为:Further, in step S3, the concrete method that calculates the diameter of burst pipe is:

将爆管面视为圆形,根据激励信号与爆管直径的关系式,激励信号取最大振幅,爆管直径取最大值,则表达式为:Considering the surface of the squib as a circle, according to the relationship between the excitation signal and the diameter of the squib, the excitation signal takes the maximum amplitude, and the squib diameter takes the maximum value, then the expression is:

Figure BDA0003134881970000023
Figure BDA0003134881970000023

式(4)中,Imax为激励信号的最大振幅,μ为爆管系数,D为爆管直径。In formula (4), Imax is the maximum amplitude of the excitation signal, μ is the squib coefficient, and D is the squib diameter.

通过式(4)可计算出爆管直径。The burst diameter can be calculated by formula (4).

附图说明Description of drawings

图1为实验管网示意图;Figure 1 is a schematic diagram of the experimental pipe network;

图2为总的监测信号曲线图;Fig. 2 is the overall monitoring signal curve diagram;

图3为反演的总激励信号曲线图;Fig. 3 is the total excitation signal curve diagram of inversion;

图4为本发明流程图。Figure 4 is a flow chart of the present invention.

具体实施方式Detailed ways

下面结合附图及具体实施例对本发明做进一步说明,但下述实施例绝非对本发明有任何限制。The present invention will be further described below with reference to the accompanying drawings and specific embodiments, but the following embodiments by no means limit the present invention.

以下通过在实验管网中实现爆管直径反演,具体操作步骤如下:In the following, the diameter inversion of the burst pipe is realized in the experimental pipe network, and the specific operation steps are as follows:

S1、监测信号分解S1, monitoring signal decomposition

实验设备主要包括:水泵、水箱、高频压力传感器(3个)、DN100、DN50、DN25钢管、DN50PVC管、水阀,各管段组合成具有2个环的管网,高频压力传感器采集频率为10000Hz。用一个字母“B”和一个数字对管网内各节点进行编号,例如:B1、B5、B10。各管段编号用一个字母“T”和管段两端节点数字编号进行编号,例如:T2-3、T10-13(图1)。在实验管网,通过快速打开水阀,制作一次爆管事件,监测事件前后的压力信号(图2),应用基于瞬变流的爆管定位方法把爆管点定位在T9-10管段上且距B9节点2.3m处。The experimental equipment mainly includes: water pump, water tank, high-frequency pressure sensor (3), DN100, DN50, DN25 steel pipe, DN50 PVC pipe, water valve. Each pipe section is combined into a pipe network with two rings. 10000Hz. Number each node in the pipe network with a letter "B" and a number, for example: B1, B5, B10. The number of each pipe segment is numbered with a letter "T" and the number number of the nodes at both ends of the pipe segment, for example: T2-3, T10-13 (Figure 1). In the experimental pipe network, by quickly opening the water valve, a pipe burst event was created, the pressure signals before and after the event were monitored (Fig. 2), and the burst pipe location method based on transient flow was used to locate the pipe burst point on the T9-10 pipe section and 2.3m away from the B9 node.

根据瞬变流的传播理论,计算在爆管点至监测点的每条传播路径中的传播瞬变流信号,称为分支模拟信号,将其叠加形成总的模拟信号,称为总模拟信号,来自每条传播路径的监测信号振幅可表达为:According to the propagation theory of transient current, the propagation transient current signal in each propagation path from the pipe burst point to the monitoring point is calculated, which is called the branch analog signal, and it is superimposed to form the total analog signal, which is called the total analog signal, The monitoring signal amplitude from each propagation path can be expressed as:

Figure BDA0003134881970000031
Figure BDA0003134881970000031

式(1)中,k为瞬变流的传播路径序号,Ek(t)为分支模拟信号在t时刻的振幅,M(t)为总的监测信号在在t时刻的振幅,εk(t)为在t时刻第k条路径中监测信号所占的比例。In formula (1), k is the propagation path number of the transient flow, E k (t) is the amplitude of the branch analog signal at time t, M(t) is the amplitude of the total monitoring signal at time t, ε k ( t) is the proportion of monitoring signals in the k-th path at time t.

S2、激励信号反演S2, excitation signal inversion

将每条路径中的信号按原路径反向从监测点传播至爆管点,原传播过程中的局部损失和摩阻损失取其倒数,变为增益,则来自每条路径的激励信号振幅表达式为:The signal in each path is propagated from the monitoring point to the pipe burst point in the reverse direction of the original path, and the reciprocal of the local loss and frictional loss in the original propagation process is taken as the gain, and the excitation signal amplitude from each path is expressed as The formula is:

Figure BDA0003134881970000032
Figure BDA0003134881970000032

式(2)中,Tk为瞬变流在第k条路径的传播时间,Aki第i个节点的透射或反射系数,Rkj第j段管段单位长度的摩阻因子,e-Rkj第j段管段单位长度的摩阻损失,Lkj为第j段管段的长度。In formula (2), T k is the propagation time of the transient flow on the k-th path, A ki is the transmission or reflection coefficient of the i-th node, R kj is the friction factor per unit length of the j-th pipe section, and e -Rkj is the The friction loss per unit length of the j-section pipe, L kj is the length of the j-th pipe section.

将来自每条路径的激励信号进行叠加,叠加后的信号即为总的激励信号,其振幅表达式为:The excitation signals from each path are superimposed, and the superimposed signal is the total excitation signal, and its amplitude expression is:

Figure BDA0003134881970000033
Figure BDA0003134881970000033

将步骤S1获得的来自每条传播路径的监测信号逆向传播后用式(2)获得来自每条路径的激励信号,再用式(3)获得总的激励信号(图3)。After back-propagating the monitoring signal from each propagation path obtained in step S1, use formula (2) to obtain the excitation signal from each path, and then use formula (3) to obtain the total excitation signal (Fig. 3).

S3、计算爆管直径S3. Calculate the diameter of the burst pipe

将爆管面视为圆形,根据激励信号与爆管直径的关系式,激励信号取最大振幅,爆管直径取最大值,则表达式为:Considering the surface of the squib as a circle, according to the relationship between the excitation signal and the diameter of the squib, the excitation signal takes the maximum amplitude, and the squib diameter takes the maximum value, then the expression is:

Figure BDA0003134881970000034
Figure BDA0003134881970000034

式(4)中,Imax为激励信号的最大振幅,μ为爆管系数,D为爆管直径。In formula (4), Imax is the maximum amplitude of the excitation signal, μ is the squib coefficient, and D is the squib diameter.

取图3中的最大振幅(1.617Mpa),通过式(4)可计算出爆管直径为32.92mm。Taking the maximum amplitude (1.617Mpa) in Figure 3, the diameter of the squib can be calculated to be 32.92mm by formula (4).

表1:本发明与瞬变流衰减法爆管直径反演成果对比表Table 1: Comparison table of inversion results of the present invention and transient flow attenuation method burst diameter

Figure BDA0003134881970000041
Figure BDA0003134881970000041

从表1中可以看出,本发明爆管直径反演存在0.92mm的绝对误差和2.88%的相对误差;与瞬变流衰减法相比,本发明爆管直径反演精度绝对值提高4.52mm,相对值提高14.12%;综上,本发明爆管直径反演的绝对误差和相对误差都较小,解决了管网中爆管直径难以反演的问题。As can be seen from Table 1, there is an absolute error of 0.92 mm and a relative error of 2.88% in the inversion of the squib diameter of the present invention; The relative value is increased by 14.12%; in conclusion, the absolute error and relative error of the inversion of the diameter of the burst pipe in the present invention are small, and the problem that the diameter of the burst pipe in the pipe network is difficult to invert is solved.

Claims (1)

1.基于瞬变流的爆管直径反演方法,其特征在于,步骤如下:1. based on the inversion method of burst diameter of transient flow, it is characterized in that, step is as follows: S1、根据瞬变流的传播特征,将总的监测信号分解为来自每条传播路径的分支监测信号,具体方法为:S1. According to the propagation characteristics of the transient flow, decompose the total monitoring signal into branch monitoring signals from each propagation path. The specific method is as follows: 根据瞬变流的传播理论,计算在爆管点至监测点的每条传播路径中的传播瞬变流信号,称为分支模拟信号,将其叠加形成总的模拟信号,称为总模拟信号,则来自每条传播路径的监测信号振幅可表达为:According to the propagation theory of transient current, the propagation transient current signal in each propagation path from the pipe burst point to the monitoring point is calculated, which is called the branch analog signal, and it is superimposed to form a total analog signal, which is called the total analog signal, Then the monitoring signal amplitude from each propagation path can be expressed as:
Figure FDA0003791359820000011
Figure FDA0003791359820000011
式(1)中,k为瞬变流的传播路径序号,Ek(t)为分支模拟信号在t时刻的振幅,M(t)为总的监测信号在在t时刻的振幅,εk(t)为在t时刻第k条路径中监测信号所占的比例;In formula (1), k is the propagation path number of the transient flow, E k (t) is the amplitude of the branch analog signal at time t, M(t) is the amplitude of the total monitoring signal at time t, ε k ( t) is the proportion of the monitoring signal in the k-th path at time t; S2、将瞬变流的传播路径及传播特征逆向,反演激励信号,具体方法为:S2. Reverse the propagation path and propagation characteristics of the transient flow to invert the excitation signal. The specific method is as follows: 将每条路径中的信号按原路径反向从监测点传播至爆管点,原传播过程中的局部损失和摩阻损失取其倒数,变为增益,则来自每条路径的激励信号振幅表达式为:The signal in each path is propagated from the monitoring point to the pipe burst point in the reverse direction of the original path, and the reciprocal of the local loss and frictional loss in the original propagation process is taken as the gain, and the excitation signal amplitude from each path is expressed as The formula is:
Figure FDA0003791359820000012
Figure FDA0003791359820000012
式(2)中,Tk为瞬变流在第k条路径的传播时间,Aki为第i个节点的透射或反射系数,Rkj为第j段管段单位长度的摩阻因子,e-Rkj为第j段管段单位长度的摩阻损失,Lkj为第j段管段的长度,In formula (2), T k is the propagation time of the transient flow on the k-th path, A ki is the transmission or reflection coefficient of the i-th node, R kj is the friction factor per unit length of the j-th pipe section, e − Rkj is the friction loss per unit length of the jth pipe section, Lkj is the length of the jth pipe section, 将来自每条路径的激励信号进行叠加,叠加后的信号即为总的激励信号,其振幅表达式为:The excitation signals from each path are superimposed, and the superimposed signal is the total excitation signal, and its amplitude expression is:
Figure FDA0003791359820000013
Figure FDA0003791359820000013
S3、根据爆管激励信号与爆管直径的关系,计算爆管直径,具体方法为:S3. Calculate the diameter of the burst tube according to the relationship between the excitation signal of the burst tube and the diameter of the burst tube. The specific method is: 将爆管面视为圆形,根据激励信号与爆管直径的关系式,激励信号取最大振幅,爆管直径取最大值,则表达式为:Considering the surface of the squib as a circle, according to the relationship between the excitation signal and the diameter of the squib, the excitation signal takes the maximum amplitude, and the squib diameter takes the maximum value, then the expression is:
Figure FDA0003791359820000014
Figure FDA0003791359820000014
式(4)中,Imax为激励信号的最大振幅,μ为爆管系数,D为爆管直径。In formula (4), Imax is the maximum amplitude of the excitation signal, μ is the squib coefficient, and D is the squib diameter.
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