The present invention relates to a technique of estimating strength of a pipe.
There is a case where a pipe constituting a piping network for transporting a resource such as water, petroleum, or gas is used beyond a service life. Therefore, problems such as leakage of fluid due to deterioration of a pipe, and rapture accident of a pipe are caused. In order to prevent these problems, a method of inspecting or estimating strength of a pipe is developed.
PTL 1 describes a buried-pipe inspection method of inspecting, with high accuracy, a degree of deterioration of a buried pipe such as a buried pipe and a ceramic pipe forming a sewer pipeline, an agricultural water pipeline, and the like, by performing an impact elastic wave test.
[PTL 1] Japanese Unexamined Patent Application Publication No. 2012-118047
The inspection method of a buried pipe described in PTL 1 is a method in which a deterioration state of a buried pipe is inspected from an inside of the pipe. However, in a pipe (hereinafter, referred to as a “water-filled pipe”) like a water supply pipe in which the inside of the pipe is filled with a fluid such as water, it is not easy to inspect a deterioration state from the inside of the pipe.
The present invention is made for solving the above-described problem, and a main object of the present invention is to provide an estimating device and the like that are capable of easily estimating strength of a water-filled pipe.
An estimating device according to one aspect of the present invention includes: a frequency response calculating unit for calculating a frequency response function of a pipe on the basis of an excitation force when the pipe is excited and a vibration response propagating through the pipe; a pipe rigidity variable estimating unit for estimating a parameter relating to rigidity of the pipe on the basis of a frequency response function model being a model representing a frequency response of the pipe, and the frequency response function; and a strength estimating unit for estimating strength of the pipe on the basis of a relation between the parameter and the strength of the pipe.
An estimating method according to one aspect of the present invention includes: calculating a frequency response function of a pipe on the basis of an excitation force when the pipe is excited and a vibration response propagating through the pipe; estimating a parameter relating to rigidity of the pipe on the basis of a frequency response function model being a model representing a frequency response of the pipe, and the frequency response function; and estimating strength of the pipe on the basis of a relation between the parameter and the strength of the pipe.
A program storing medium according to one aspect of the present invention stores a computer program causing a computer to execute: processing of calculating a frequency response function of a pipe on the basis of an excitation force when the pipe is excited and a vibration response propagating through the pipe; processing of estimating a parameter relating to rigidity of the pipe on the basis of a frequency response function model being a model representing a frequency response of the pipe, and the frequency response function; and processing of estimating strength of the pipe on the basis of a relation between the parameter and the strength of the pipe.
According to the present invention, an estimating device and the like that are able to estimate strength of a water-filled pipe with ease can be provided.
Each example embodiment of the present invention is described with reference to the accompanying drawings. First, a first example embodiment of the present invention is described.
As illustrated in
One example of a case in which strength of a pipe is estimated by using the estimating device 100 is described with reference to
In the example illustrated in
As illustrated in
An exciter 161 is installed on the accessory 302-1. The exciter 161 excites, for example, the accessory 302-1. With the excitation by the exciter 161, an elastic wave is excited in the fluid such as water filled inside the pipe 301. The elastic wave is also excited in the pipe 301.
As the exciter 161, a mechanism that is capable of exciting a vibration of a broad bandwidth is desirably used. As the exciter 161, for example, an impulse hammer, a hydraulic actuator, a pneumatic actuator, or a water-releasing pressure-variation generator is used, but another mechanism may be used as the exciter 161.
Further, the exciter 161 records an excitation force, which is magnitude of force when the accessory 302-1 is excited. Excitation force data, which are data recording the excitation force, are sent to, for example, the frequency response calculating unit 110 of the estimating device 100 via a wired or wireless communication network or another mechanism for data transmission.
A measuring instrument 162 is installed on the accessory 302-2. The measuring instrument 162 measures an elastic wave propagating through the fluid such as water inside the pipe 301 and the pipe 301. The measuring instrument 162 mainly measures an elastic wave generated by excitation by the exciter 161 and propagating through the fluid such as water inside the pipe 301 and the pipe 301.
As the measuring instrument 162, a sensor for measuring a vibration of a solid body is used. Examples of the measuring instrument 162 include a piezoelectric type acceleration sensor, a capacitive type acceleration sensor, an optical velocity sensor, a dynamic strain sensor, an eddy-current displacement sensor, a dial gauge, a digital image correlation measuring device, an optical fiber type strain gauge, a contact type displacement sensor, and a speckle light interferometer. However, another instrument may be used as the measuring instrument 162.
A measurement result by the measuring instrument 162 is sent to, for example, the frequency response calculating unit 110 of the estimating device 100 via a wired or wireless communication network or another mechanism for data transmission. With a time point at which the exciter 161 performs excitation as a reference, the measuring instrument 162 may send a result of a measurement performed for a time period from before to after the time point to each component of the estimating device 100. In the case described above, a length of the time period from before to after the reference time point at which the exciter 161 performs the excitation may be determined according to a time required for an elastic wave generated by the excitation to the accessory 302-1 by the exciter 161 to propagate to the measuring instrument 162.
Note that, as described above, the pipe 301 is assumed to be buried underground, and visual observation and contact of the pipe 301 is assumed to be difficult. Therefore, the exciter 161 and the measuring instrument 162 are exemplified in such a way as to be attached to the accessories 302. However, when it is possible to make contact with the pipe 301, each of the exciter 161 and the measuring instrument 162 may be directly installed on, for example, the pipe 301.
Further, in the example illustrated in
Similarly, in the example illustrated in
Next, each component of the estimating device 100 according to the present example embodiment is described. Note that, in each example embodiment of the present invention, each component of the estimating device 100 represents a block of a function unit. Some or all of each component of each device is achieved by, for example, any combination of an information processing device 500 and a program, such as illustrated in
Each component of each device according to each example embodiment is achieved by the CPU 501 acquiring and executing the program 504 achieving a function of each component. The program 504 achieving a function of each component of each device is, for example, previously stored in the storing device 505 or the RAM 503, and read out by the CPU 501 as necessary. Note that, the program 504 may be provided to the CPU 501 via the communication network 509, or may be previously stored in the recording medium 506, read out by the drive device 507, and thereby provided to the CPU 501.
There are various modification examples of a method of achieving each device. For example, each device may be achieved by any combination of the information processing device 500 that is separated for each component and a program. Further, a plurality of components included in each device may be achieved by any combination of one information processing device 500 and a program.
Some or all of each component of each device is achieved by a dedicated or general-purpose circuit including a processor and the like, or a combination thereof. The dedicated or general-purpose circuit may be configured by a single chip, or may be configured by a plurality of chips connected to each other via a bus. Some or all of each component of each device may be achieved by a combination of the above-described circuit and the like and a program.
When some or all of each component of each device is achieved by a plurality of information processing devices and circuits and the like, the plurality of information processing devices and circuits and the like may be concentratedly or distributedly disposed. For example, the information processing devices and circuits and the like may be achieved as a form, such as a client-and-sever system and a cloud computing system, in which each of the information processing devices and circuits and the like is connected via a communication network.
Among the components of the estimating device 100, the frequency response calculating unit 110 is described first. The frequency response calculating unit 110 calculates, based on an excitation force when a pipe is excited and a vibration response propagating through the pipe, a frequency response function of the pipe. The frequency response function of the pipe is a function expressed in a frequency domain as a ratio of magnitude of the vibration response to the excitation force applied to the pipe.
The excitation force indicates, in a case where a pipe is excited, a temporal change in magnitude of force applied to the pipe. As one example, the excitation force indicates a temporal change in magnitude of force applied to the pipe 301 by the exciter 161 illustrated in
The vibration response is a response of the pipe or the fluid such as water inside the pipe to the excitation performed by the exciter 161. In the example illustrated in
The frequency response calculating unit 110 acquires, as one example, a frequency response function of the pipe as follows. First, let excitation force data be f(t), and response data be x(t). Further, let functions in a frequency domain into which f(t) and x(t) are Fourier transformed be F(ω) and X(ω), respectively. The frequency response calculating unit 110 acquires F(ω) and X(ω) with respect to f(t) and x(t), respectively. ω represents an angular frequency.
Then, the frequency response calculating unit 110 acquires, by using the following expression (1), a frequency response function Hexp(ω).
Note that, the frequency response calculating unit 110 may perform processing for improving a signal-to-noise ratio, as necessary. For example, the frequency response calculating unit 110 may perform averaging processing for acquiring an average value of frequency response functions acquired by a plurality of times of excitation and measurement of a response.
The pipe rigidity variable estimating unit 120 estimates a parameter relating to rigidity of the pipe, on the basis of the frequency response function model representing the frequency response of the pipe, and the frequency response function. As the frequency response function, Hexp(ω) acquired by the frequency response calculating unit 110 is used.
In the pipe rigidity variable estimating unit 120, an expression of the frequency response function model is determined in advance, according to a characteristic of the pipe being a target and Hexp(ω) acquired by the frequency response calculating unit 110. A frequency response function model specifically representing a frequency response of a pipe being a target is acquired by approximating an expression of the frequency response function model to a frequency response function that is actually measured. Therefore, the parameter relating to the rigidity of the pipe is acquired by approximating the frequency response function model to the frequency response function.
The pipe rigidity variable estimating unit 120 estimates the parameter relating to the rigidity of the pipe by acquiring such a parameter that the expression of the frequency response function model approximates the frequency response function Hexp(ω) acquired by the frequency response calculating unit 110.
Prior to a description of the parameter acquired by the pipe rigidity variable estimating unit 120, the expression of the frequency response function model used in the pipe rigidity variable estimating unit 120 is described. In the following description, the pipe is assumed to be a water-filled pipe whose inside is filled with water.
First, when it is assumed that a weight is applied from both sides of the pipe as illustrated in
In the expression (2), R is a radius of the pipe, E is an elasticity modulus of the pipe, I is a second moment of area of the pipe, and θ is an angle of a position at which the displacement w is considered with respect to a reference direction. In the expression (2), one of the directions perpendicular to a direction in which the weight is applied is assumed to be the above-described reference direction, and θ is determined thereby.
Then, a pipe rigidity, which is the rigidity of the pipe, is defined by transforming the expression (2) and expressing the expression (2) in a form of the Hooke's law. Specifically, a pipe rigidity K is expressed as the following expression (3).
In the expressions (2) and (3), when a wall thickness of the pipe is assumed to be t, and a unit length of the pipe is assumed to be L, the second moment of area I is expressed as I=Lt3/12. Specifically, the pipe rigidity K is determined by the elasticity modulus E of the pipe, the wall thickness t, and the radius R of the pipe. Among those variables, the radius R of the pipe can be generally known from a drawing and the like of the pipe. Further, the elasticity modulus E and the wall thickness t of the pipe may change with deterioration of the pipe. Thus, in the present example embodiment, the pipe rigidity variable estimating unit 120 estimates, as one example of the parameter relating to the rigidity of the pipe, either one or both of the elasticity modulus E of the pipe or/and a value of the wall thickness t of the pipe. The parameter acquired by the pipe rigidity variable estimating unit 120 may be appropriately determined according to a relation and the like used in the strength estimating unit 130 to be described later.
The expression of the frequency response function model is expressed as H(ω|θM, θF), as a function of an angular frequency ω, a pipe rigidity variable θM, and an accessory parameter θF. The pipe rigidity variable θM is a parameter relating to the rigidity of the pipe, and is defined as θM=[E, t, R]. The accessory parameter θF is a parameter relating to a structure of an accessory such as the accessories 302 illustrated in
A frequency response function model with respect to an example illustrated in
In the expression (5), M, K, and C respectively indicate an equivalent mass, an equivalent rigidity, and an equivalent damping coefficient when the ring unit illustrated in
Note that, the expression H(ω|θM, θF) of the frequency response function model expressed by the expressions (4) and (5) is assumed in a case in which the exciter 161 and the measuring instrument 162 are attached to the accessories. However, as described above, a position to which the exciter 161 or the measuring instrument 162 is attached is not limited thereto, and in such a case, for example, each accessory parameter θF may be set to an appropriate value.
The pipe rigidity variable estimating unit 120 acquires an estimated value of the pipe rigidity variable by approximating the expression H(ω|θM, θF) of the frequency response function model to the frequency response function Hexp(ω) acquired by the frequency response calculating unit 110. Specifically, the pipe rigidity variable estimating unit 120 acquires the estimated value of the pipe rigidity variable by approximating H(ω|θM, θF) to Hexp(ω) in such a way that a difference between H(ω|θM, θF) and Hexp(ω) is within a predetermined range. The pipe rigidity variable estimating unit 120 acquires the estimated value of the pipe rigidity variable by using the following expression (6), for example.
Hereinafter, a left-side value of the expression (6) is referred to as “the estimated value of the pipe rigidity variable”. In the expression (6), argmin indicates a set of arguments that minimizes the function given in the brackets. Specifically, the pipe rigidity variable estimating unit 120 acquires the estimated value of the pipe rigidity variable in such a way that a sum of squares of an absolute value of the difference between H(ω|θM, θF) and Hexp(ω) is minimized.
The pipe rigidity variable estimating unit 120 acquires the estimated value of the pipe rigidity variable by using, for example, a nonlinear optimization method such as a Levenberg-Marquardt method. However, when acquiring the estimated value of the pipe rigidity variable, the pipe rigidity variable estimating unit 120 may use any other method of curve-fitting.
The strength estimating unit 130 estimates strength of the pipe, on the basis of a relation between the parameter estimated by the pipe rigidity variable estimating unit 120 and the strength of the pipe. The strength estimating unit 130 estimates, mainly as the strength of the pipe, tensile strength of the pipe. The tensile strength of the pipe may change with deterioration of the pipe. Specifically, a degree of deterioration of the pipe is estimated by acquiring the tensile strength of the pipe.
The strength estimating unit 130 estimates the strength of the pipe by using, for example, a relation, as illustrated in
The relation illustrated in
The tensile strength, which is one of the strengths acquired by the strength estimating unit 130, is related to deterioration of the pipe. Specifically, the tensile strength indicates a degree of deterioration of the pipe. Therefore, the degree of deterioration of the pipe can be estimated by estimating the tensile strength.
Next, an operation of the estimating device 100 according to the present example embodiment is described with reference to the flowchart illustrated in
First, excitation of the pipe, and measurement of a vibration response of the pipe and the fluid inside the pipe to the excitation are performed (Step S101).
In the configuration example illustrated in
Next, the frequency response calculating unit 110 acquires a frequency response function of the pipe, on the basis of the excitation force and the vibration response acquired in Step S101, (Step S102).
Next, the pipe rigidity variable estimating unit 120 estimates a parameter, on the basis of the frequency response function model in which a frequency response of the pipe is modeled and the frequency response function of the pipe acquired in Step S102 (Step S103). As described above, the pipe rigidity variable estimating unit 120 estimates, as one example, the elasticity modulus E and the wall thickness t of the pipe, which are values each included in the pipe rigidity variable θM.
Next, the strength estimating unit 130 estimates strength of the pipe, on the basis of the parameter relating to rigidity of the pipe acquired in Step S103, and a relation between, for example, the parameter and the strength of the pipe (Step S104). As the relation between the parameter and the strength of the pipe, a relation stored in the strength information storing unit 152 is used. Further, as described above, tensile strength of the pipe is estimated as the strength of the pipe. The acquired strength of the pipe is output via any means including a display and a communication network, as appropriate.
As described above, the estimating device 100 according to the present example embodiment estimates the parameter relating to the rigidity of the pipe, on the basis of the frequency response function model representing the frequency response of the pipe, and the frequency response function calculated on the basis of an actually measured value. Then, the estimating device 100 according to the present example embodiment estimates the strength of the pipe including the tensile strength, on the basis of the relation between the estimated parameter and the strength of the pipe.
The estimating device 100 is further described in comparison with the method described in PTL 1, by using a more detailed example.
Referring to
On the other hand, in the method described in PTL 1, an interval between a striking unit and a vibration receiving unit is assumed to be about several meters at most. Further, in the method described in PTL 1, a frequency domain of 0.5 kHz (kilohertz) to 7.0 kHz is assumed to be an entire frequency domain, and a frequency domain of 3.5 kHz to 7.0 kHz is assumed to be a high frequency domain. Then, strength of a pipe is estimated on the basis of an area ratio of the high frequency domain to the entire frequency domain.
However, it may be difficult to dispose the striking unit and the vibration receiving unit on a buried water-filled pipe at the interval assumed in PTL 1. Further, as described in
On the other hand, in the estimating device 100 according to the present example embodiment, the pipe rigidity variable M described above is acquired by using the frequency response function model according to a generation mechanism of a resonance peak in the response spectrum with respect to the response data. Specifically, in the estimating device 100 according to the present example embodiment, a parameter relating to the rigidity of the pipe is acquired by using an appropriate frequency response function model. Since the parameter relating to the rigidity of the pipe is acquired, strength of the pipe such as tensile strength is estimated in the estimating device 100. Specifically, the estimating device 100 according to the present example embodiment can estimate the strength of the water-filled pipe with ease.
While the invention has been particularly shown and described with reference to exemplary embodiments thereof, the invention is not limited to these embodiments. It will be understood by those of ordinary skill in the art that various changes in form and details may be made therein without departing from the spirit and scope of the present invention as defined by the claims. Further, a configuration according to each example embodiment may be combined with each other without departing from the scope of the present invention.
This application is based upon and claims the benefit of priority from Japanese patent application No. 2017-215729 filed on Nov. 8, 2017, the disclosure of which is incorporated herein its entirety by reference.
Number | Date | Country | Kind |
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2017-215729 | Nov 2017 | JP | national |
Filing Document | Filing Date | Country | Kind |
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PCT/JP2018/041089 | 11/6/2018 | WO | 00 |