The detection of small side branches within underground water pipe networks can be challenging since they are usually subject to many unknown uncertainties. A transient-based method was proposed to detect multi-branching pipes in pipeline systems having uncertainties associated with unknown abnormalities. To isolate the uncertainty signal from the original pressure signal, a polynomial transient model was developed that can address nonlinear transient introduction. Through the superimposition of different pressure signals, the uncertainty signal was delineated to obtain the processed signal for multi-branch prediction. Pipeline systems with two branching pipes were tested under various uncertainties to detect multi-branching pipes. In this study, two transient generation conditions were used: an instant valve closure and a pressure injection. Under several uncertainty conditions, hydraulic pressure damping can be obtained for the detection of two branching pipes under both transient generation conditions. It is possible to predict the locations of multi-branching pipes with a prediction error of less than 10% by using proper signal processing and manipulation for two distinct transient generation methods in a pilot-scale pipeline system with several uncertainties. This study demonstrates the potential for detecting multi-branching pipes in a pipeline system, even with unknown uncertainties for a pipeline system.

  • A systematic signal processing method was proposed for the isolation of uncertain signals.

  • The polynomial transient model was improved for the representation of real transient introduction.

  • A transient-based multi-branching pipe detection scheme was developed in an n-branching pipeline system having uncertainties.

  • Multi-branching pipes could be identified by transient-based distinct pressure damping in processed signals.

A

cross-sectional area of pipeline

a

isolated wave speed of the pipe

D

pipe diameter

f

Darcy–Weisbach friction factor

g

gravitational acceleration

H

pressure head

n1, n2, n3, n4

nonlinear transient constants in a specific transient injection

Q

flow rate

t

time

x

distance of the pipeline system

τ

dimensionless coefficient of the relative valve opening

A water transmission pipeline system, consisting of main underground pipelines, plays a critical role in the sustainability of urban life. There are several types of pipeline elements in urban water pipelines, including series, branched, and lopped elements (Che et al. 2021). Distribution of drinking water to domestic users is largely dependent on how branched pipeline elements are arranged.

Branching pipe systems can provide drinking water efficiently according to demand and protect continuous resource supply even if one element fails (Meniconi et al. 2021a). It is essential to understand the role and to check the functions of the branches for reliable management of urban water systems. It is suspected that uncountable branches of urban water systems are being used illegally. The branched elements are illegally connected to the main pipelines, resulting in unexpected pressure fluctuations and adversely affecting urban water systems (Ebrahimi et al. 2022).

This results in a mismatch between water bills and total water usage, which is one of the most pressing problems with water management (Lee 2005; Stephens 2008). Detecting and predicting leaks in urban water systems have been the keys to addressing the water loss issue (Yu et al. 2023; McMillan et al. 2024; Sostero et al. 2024). It is also crucial to pay attention to branching elements because they can contribute significantly to water loss (Meniconi et al. 2011).

Several issues relating to branched pipeline elements can be addressed by considering the actual flow characteristics of urban water systems. It is important to recognize that pipeline systems are fundamentally unsteady in nature, meaning that pressure and flowrate continuously change over time and space. Flow changes or stagnation within such a system result in unexpected pressure waves with abnormal fluctuations in head and flowrate. As fluctuation patterns converge to specific flow conditions, a hydraulic transient is defined as the transition from one equilibrium condition to another under certain flow conditions.

As field pipeline systems are always subject to transient flow due to valve operations in each household, conducting research under hydraulic transient flow conditions will enhance the practical applicability of pipeline studies (Marsili et al. 2023; Kim et al. 2024). Hence, many pipeline studies have been conducted using hydraulic transients, usually induced by fast valve closures to reduce costs (Castellani et al. 2024; Kim 2024; Maietta et al. 2024; Toumi & Sekiou 2024; Zhang et al. 2024).

An instant valve closure makes a high-pressure wave propagate into a pipeline system, inducing pressure variations that are both positive and negative. It can cause cavitation within the pipe, resulting in failure of pipe components such as pipes, valves, and fittings, making it difficult to apply to field pipeline systems (Yuce & Omer 2019). Several researchers have explored alternatives that induce minimal hydraulic transients in a pipeline system without valve closure to avoid the risks associated with instant valve closure. A portable pressure wave maker device, connected to a pipeline system via a connecting valve, injects high-pressure waves into a pipeline system (Brunone et al. 2008). Brunone et al. (2021) studied the optimal design procedure for a smart portable device and assessed the device's effectiveness in detecting leaks in water transmission systems. The leak detection process was facilitated with minimal pressure disturbance due to this enhanced portable performance. Using wavelet analysis of pressure measurements from regulated pressure injection, Lee et al. (2021) developed a leak detection method for a simple pipeline system. Analyzing injected pressure data with wavelet analysis, they can determine the leak location in a pilot-scale pipeline system using the pressure damping wave and pressure vibration wave. By injecting safe transient flow into an actual pipeline system with a portable pressure wave maker, Capponi et al. (2024) proposed a transient test-based method for detecting the open status of an in-line valve under inverse transient analysis and correctly capturing the transient response of a series junction.

A pressure injection method involves injecting pressurized water into a pipeline system, which propagates a smaller pressure wave rather than valve closure, reducing pipeline damage risk (Meniconi et al. 2021b). In order to improve its applicability in real-life pipeline systems, this study carried out numerical and experimental analyses not only under an instant valve closure but also using a transient pressure injection.

A transient-based method should also be considered for detecting branching pipes in urban water systems. Unknown branched pipe elements, such as leaks and blockages, are also treated as abnormalities in a pipeline system. The pressure signal fluctuates meaningfully when a transient pressure wave is generated in a pipeline system. It is possible to detect an abnormality in a pipeline system using this fluctuation by analyzing the direct pressure responses in transient signals and the characteristics of overall pressure reflection in frequency responses (Che et al. 2021; Castellani et al. 2024). Transient-based studies have mainly been conducted for the purpose of diagnosing such abnormalities in urban water systems, mostly focusing on research aimed at addressing leakage detection issues in a pipeline system (Kim 2020; Choura et al. 2021; Meniconi et al. 2021b; Brunone et al. 2022; Pan et al. 2022; Keramat et al. 2023). Leakage in a pipeline system can be detected using the frequency response method owing to the leak characteristic causing pressure oscillation without altering the system's boundary conditions (Stephens 2008; Kim 2020). It has also been successfully developed to detect single-branching pipes by using wavelet transforms and frequency response functions (Meniconi et al. 2011; Duan & Lee 2016).

Nevertheless, it is challenging to explain the frequency response of branching pipes because of the boundary conditions that exist both at the ends and sides. A pipeline system with branching pipes deforms the boundary conditions and complicates the frequency-based detection of branching pipes, which worsens as the number of branching elements increases (Kim 2023).

Therefore, branching pipes will be detected by analyzing the direct pressure response of transient signals. For detecting branching pipes, research had previously focused on single-branching pipes (Meniconi et al. 2011; Duan & Lee 2016; Meniconi et al. 2018; Ebrahimi et al. 2022); however, multi-branching pipeline system research focused on addressing issues such as multi-leak detection (Torres et al. 2021) and reliable skeletonization (Meniconi et al. 2021a; Kim 2023). Detecting multi-branching pipelines accurately was first proposed by Ko et al. (2024). Based on real valve action and interference effects between different branching pipes, this study demonstrated transient-based multi-branching pipes detection (TBMBD) in a numerical reservoir-pipe-valve system. However, real-life systems need to address issues related to unknown pipeline components in field systems, such as features of unknown sections of the pipeline that may alter pressure signals. In this paper, a direct pressure response analysis of an experimental pipeline system is performed to support the reliability of TBMBD for field systems.

This means that uncertainties within urban water supply systems should be properly considered for practical research on TBMBD. The uncertainty of unknown information affects pressure fluctuations in normal hydraulic responses and hampers the prediction of several water problems in real pipeline systems. Two broad categories of uncertainties had been identified and addressed: epistemic uncertainties and empirical uncertainties (Wang & Ghidaoui 2018; Alawadhi & Tartakovsky 2020; Wang et al. 2020a; Wang 2021; Duan & Keramat 2022; Tjuatja et al. 2023), as well as aleatoric uncertainties in repeated experimental attempts (Basse 2019; Wang et al. 2020b; Hu et al. 2023; Wang et al. 2023).

Many uncertainty studies have proposed advanced methods for identifying, analyzing, and quantifying them, but their practical application still suffers from limitations. In particular, most urban water systems are complicated networks with many unknown components and present a wide range of uncertainties, making it very challenging to determine which types exist and where they are located. These uncertainties introduce problems in both diagnosing and addressing the hydraulic issues caused by specific abnormalities or components. Therefore, this paper proposed TBMBD under the assumption that uncertainties of unknown states exist as boundary conditions within the pipeline system. With the developed TBMBD, uncertainty assessment will be quicker and easier in the real field, reducing labour-intensive processes.

To improve the field applicability of TBMBD methods, this study extends the development of Ko et al. (2024) for pipeline systems with unknown uncertainties. Identifying the hidden uncertainty signals for a pipeline system is the key element of this research. Using the polynomial transient model (PTM), experimental pressure signals from a rectilinear pipeline system with uncertainties are acquired and calculated. The original uncertainty signal can be recovered through signal processing techniques such as superimposition. This uncertainty signal is used to introduce advanced signal manipulation techniques. Following the isolation of uncertainty responses, two superimposing processes are applied to the signals from each of the three branched elements of the experimental system. Verifications were performed under two different transient generation conditions, valve closures and pressure injections, taking into account three different uncertainty factors.

This paper is organized as follows: Section 2.1 explains the systematic processing for uncertainty signal separation used in transient analysis. Section 2.2 presents a method for TBMBD using uncertainty signals. Section 2.3 introduces the experimental pipeline system, which includes multi-branching pipes and uncertainties. Based on signal processing and experiments, we present a multi-branching pipe detection system under rectilinear flange conditions in Section 3.1, small and large leak flange conditions in Section 3.2, and 0.25 m series flange conditions in Section 3.3. As a final step, Section 3.4 compares the method with previous studies to evaluate its performance in detecting multi-branching pipes.

The systematic signal processing for uncertainty separation in transient analysis

Figure 1 illustrates the outline of the systematic signal processing for the isolation of uncertainty signals from pressure measurement, which will improve the applicability of TBMBD.
Figure 1

Flowchart of systematic signal processing for uncertainty separation.

Figure 1

Flowchart of systematic signal processing for uncertainty separation.

Close modal

Two distinct approaches address the difference between a real-life system and its mathematical approximation. These were expressed in terms of the acquisition of experimental data from transient events for a pipeline system having multiple unknown uncertainties and the analysis of the pressure signal from the numerical analysis of the corresponding intact system. The PTM was used for the accurate evaluation of the transient introduction condition (Ko et al. 2024), which solved the mass and momentum balance equation for pressurized pipeline systems.

Pressure and flowrate in an elastic pipeline system can be determined by continuity and momentum conservations, which were expressed as the following first-order partial differential equations (Wylie & Streeter 1993; Chaudhry 2014):
(1)
(2)
where H is the pressure head, Q is the flowrate, x is the distance along the pipe, t is the time, a is the wave speed in a pipe, g is the gravitational acceleration, A is the pipe cross-sectional area, D is the pipe diameter, and f is the Darcy–Weisbach friction factor.
Partial differential equations can be transformed into ordinary differential equations, namely, as the method of characteristics (MOC) and integrating along characteristic lines. Ordinary differential equations can be obtained by combining Equations (1) and (2).
(3)
The PTM was a developed model for the representation of nonlinear transient manoeuvres using a high-order polynomial approximation with a dimensionless coefficient (τ) of the relative valve opening for MOC application as follows (Funk et al. 1972; Ko et al. 2024):
(4)
where t is the time for transient initiation, and coefficients n1, n2, n3, and n4 are nonlinear transient constants determined by the pressure signals in a specific transient injection.

The raw pressure signals can be normalized for signal processing between distinct signals. The Joukowsky pressure can be used for the normalization of experimental and numerical pressure signal responses from transient introduction, which provides an identical scale in signal reconstruction. Finally, the inherent uncertainty signal can be extracted by superimposing multiple normalized pressure signals. The signal processing procedure described here is a systematic method of identifying uncertainties in a system response arising from unknown boundary conditions without the process of physical implementation or mathematical description.

Developed method of TBMBD

Figure 2 shows the flowchart for the developed TBMBD scheme for the n-branching pipeline system having multiple uncertainties. Signal processing in Figure 1 was used to incorporate uncertainty in an experimental pipeline system based on TBMBD (Ko et al. 2024). We conduct transient experiments under several transient conditions, such as instant valve closures or pressure injections, and for multiple combinations of pipeline layouts, from a simple pipeline to that with n number of branching pipeline elements.
Figure 2

Flowchart of developed TBMBD in an experimental n-branching pipeline system with uncertainties.

Figure 2

Flowchart of developed TBMBD in an experimental n-branching pipeline system with uncertainties.

Close modal

Using n-branching pipeline elements, we are able to obtain experimental raw pressure signals per one transient condition. Through proper signal superimposition, we can isolate the uncertainty and rectilinear pipeline signals in these normalized signals based on Joukowsky pressure responses in transient initiation. This results in the acquisition of signals for uncertainties-rectilinear-isolated signals (URIS).

The interference impact in an n-branching pipeline system can be determined by subtracting URIS from the sum of the combinations of uncertainties-rectilinear-isolated interference signals from one branching pipe to n − 1 branching pipes, as follows:
(5)
where n represents the number of branches, and URIS can be obtained by isolating the signals of uncertainties and rectilinear pipeline system in raw pressure signals.
In TBMBD, the signal is derived from the combination of interference–uncertainties–rectilinear–isolated signal (IURIS) for pipes with two to n branches:
(6)

As a result of separating the interference effect between n-branching pipes, this method can be used to identify a specific element from multi-branching pipeline elements.

Experimental pipeline system with multi-branching pipes and uncertainties

Figure 3 shows a schematic of a reservoir–pipe–uncertainties–branching pipes–valve system for TBMBD experiments. It consists of an upstream reservoir, a stainless main pipe, an uncertainty zone, two stainless branching pipes with control valves, and a downstream control valve. This system captures various transient pressure signals in different layouts of pipelines through controlling valves for branched pipeline elements. The main pipe length is 90 m, and the internal diameter and wall thickness of all pipes are 0.02 and 0.0021 m, respectively. This system exhibits a steady flowrate of 39 mL/s, and the Darcy–Weisbach friction factor is 0.0697 by the Darcy–Weisbach equation (Wylie & Streeter 1993).
Figure 3

The schematic of a reservoir–pipe–uncertainties–branching pipes–valve system.

Figure 3

The schematic of a reservoir–pipe–uncertainties–branching pipes–valve system.

Close modal

In order to validate the performance of the TBMBD scheme in this system, three points should be pre-checked. First, the length of the branched pipe element closest to the downstream valve and the distance between the two branching pipes should be properly spaced. Due to interference effects between adjacent branching pipes, pressure responses for TBMBD can be disturbed (Ko et al. 2024). As a result, branching pipes were installed at points 26.5 and 39.7 m from the downstream valves, with a distance of 13.2 m between them, and their lengths of 3.0 and 6.3 m, respectively. Second, downstream control valves must be closed when pressure waves are injected into this system. The pressure injection device is attached to the connecting valve of the main pipe at 0.3 m from the downstream valve, allowing regulated pressure waves to be injected into the system when the connecting valve is opened. Lastly, various pipe fittings introduce unknown fluctuations into a pressure signal to create artificial uncertainties. A pipe flange is a component that connects pipeline elements, but it can also deteriorate the ability to detect abnormalities by changing acoustic waves to propagate acoustically in an unexpected manner (Li et al. 2018; Williams et al. 2020). Therefore, a stainless flange is installed 57.1 m from the downstream valve, and its length is 0.93 m. Three types of stainless flange were used to generate distinct pressure signals corresponding to different uncertainty levels: rectilinear flange, leak flange, and series flange. There is no difference in the pipe property of all flanges, except that the inner diameter of the series flanges is 0.25 m. A high-frequency pressure transducer was used to obtain transient signals at 0.6 m from the downstream valve (Lee et al. 2021).

Transient-based signal processing and experiments for multi-branching pipe detection under rectilinear flange condition

The signal processing for characterizing the uncertainty signal uses raw pressure signals obtained by the transient experiment and those simulated by a transient model. As shown in Figure 3, the uncertainty is related to the arbitrary flange used in the experiment. The transient events are either caused by an instant valve closure at the downstream control valve or by pressure injection that rapidly opens the connecting valve between the main pipeline system and the pressure injection device. The simulated pressure signal was calculated using PTM based on Equations (1)–(4) in the intact pipeline system. These pressure signals were normalized using the Joukowsky pressure responses of transient initiation for processing the pressure signal.

Figure 4(a) presents the normalized head signals of the experiment signal in a rectilinear pipeline system with a rectilinear flange and those of PTM signals in a rectilinear pipeline system without a flange on transient condition of instant valve closure. The experimental signal initially showed a small pressure damping due to rectilinear flange before 0.1 s and subsequently showed substantially different responses. Specifically, the overall amplitude reduction and the smooth shape of the pressure response curve in the experiment signal were caused by unsteady friction unlike, the steady friction in the PTM signal. The phase mismatch between these signals can be attributed to the fact that the wave speed (a) in the experiment signal was approximately 1,198.40 m/s, unlike the 1,413.43 m/s of the PTM signal, calculated using the values of the main pipe length and the signal period (Chaudhry 2014; Che et al. 2021).
Figure 4

Normalized head signals of the experiment signal in the rectilinear pipeline system with rectilinear flange and the PTM signal in the intact pipeline system on both transient conditions of (a) instant valve closure and (b) pressure injection.

Figure 4

Normalized head signals of the experiment signal in the rectilinear pipeline system with rectilinear flange and the PTM signal in the intact pipeline system on both transient conditions of (a) instant valve closure and (b) pressure injection.

Close modal

These results are also shown in Figure 4(b), which presents the normalized head signals on transient conditions of pressure injection under identical boundary conditions. The overall decreasing pattern in the experiment signal was associated with the unsteady friction effect along the pipeline extension. The largest pressure damping in these signals was observed between 0.1 and 0.15 s due to the pressure wave reflected upstream of the reservoir, and the phase difference indicates the variation of the wave speed within the experimental pipeline system (Lee et al. 2021). In spite of these discrepancies between experiment signals, it is not necessary to consider them explicitly because multi-branch pipe detection only utilizes the initial pressure response before 0.1 s (Ko et al. 2024). Additionally, unexpected pressure fluctuations caused by uncertain parts, including rectilinear flanges, were generated before the pressure damping unlike the transient condition of instant valve closure, as depicted in Figure 4(a). For handling these unexpected pressure responses, this study introduced a systematic signal processing method for separating uncertainty signals (Figure 1). The uncertainty signal was isolated from Joukowsky-normalized head signals of all pipeline system layouts to perform TBMBD.

Figure 5(a) illustrates the IURIS obtained using the developed TBMBD method (Figure 2) in a pipeline system with two branching pipes and rectilinear flanges on transient conditions of instant valve closure. This figure shows that the pressure-damping phases of Branch A and Branch B were in good agreement between 0.04 and 0.08 s when comparing the IURIS of Branch AB with those of Branch A and Branch B, respectively. It is possible to detect two branching pipes in a pipeline system with uncertainties by conducting signal processing (Figure 1) and applying the developed TBMBD method (Figure 2). According to Figure 5(b), IURIS detected two branching pipes, A and B, between 0.035 and 0.07 s during transient conditions of pressure injection. Comparing Figure 5(a) with Figure 5(b), there are several differences in these signals for detecting two branching pipes. Transient initiation times between two experimental transient generators can explain the timing difference in pressure damping between Figure 5(a) and 5(b). This means that the amplitude difference in pressure damping can also be attributed to the method of transient generation. In Figure 5(a), the amplitude of pressure damping was proportional to the length of the branching pipe. However, on the transient condition of pressure injection, the small amplitude of pressure damping was generated regardless of the length of the branching pipe. This is because the transient waves of pressure injection into a pipeline system propagate with amplitude regulated to a safe range (Brunone et al. 2008). The obtained results indicate that two branching pipes can be detected on both transient generation conditions with rectilinear flange and other uncertainties.
Figure 5

IURIS in an experimental pipeline system with two branching pipes and a rectilinear flange on both transient conditions of (a) instant valve closure and (b) pressure injection.

Figure 5

IURIS in an experimental pipeline system with two branching pipes and a rectilinear flange on both transient conditions of (a) instant valve closure and (b) pressure injection.

Close modal

TBMBD experiments with leak flange

The field applicability of the developed TBMBD method can be enhanced with additional experiment validation using different uncertainty conditions. An experiment with different uncertainty conditions was conducted by converting the uncertainty zone of the pipeline system (Figure 3) into a leak flange made of the same materials as the rectilinear flange. Combining the flange and leak effects, the leak flange introduces complicated uncertainties that alter normal pressure responses, making them more unpredictable. Two distinct leak conditions can be produced by two flanges: a small leak flange with a leak flowrate of 20 mL/s, which represents 32.9% of the steady flowrate for a small leak flange, and a large leak flange with a 50 mL/s leak flowrate, which represents 67.3% of the steady flowrate for a large leak flange.

As shown in Figure 4, signals from the experiment under different leak flange conditions were recorded in the same format under the same transient conditions as in Section 3.1.

Compared to Figure 4(a), the experiment signal of the leaky flange included pressure responses of a pressure drop, greater pressure oscillations, and greater pressure attenuation in the overall experiment signal than the intact flange (Covas & Ramos 2010; Choura et al. 2021). Under transient conditions of pressure injection, the small leaky flange caused pressure oscillations in the experiment signal. Furthermore, this signal exhibited unexpected pressure fluctuations before pressure damping at 0.15 s, similar to Figure 4(b), making it difficult to identify the precise pressure response of the small leak flange.

Large leak flange conditions resulted in much greater responses than small leak flange conditions (Covas & Ramos 2010; Zhang et al. 2024). It was found that the experiment signal was more convergent under the large leak flange condition than in the rectilinear and small leak flange condition. This signal also showed unexpected pressure fluctuations prior to pressure damping at 0.15 s. Therefore, the leak effects cannot be clearly defined on the pressure injection condition, whereas they can be on the instant valve closing condition. This property enabled the characterization of the uncertainty signal and conducting TBMBD, as described in Section 3.1, under small and large leak flange conditions.

Figure 6(a) shows IURIS treated using uncertainty signal processing and the developed TBMBD method in two branching pipe systems. Two phases of pressure damping were successfully captured between 0.05 and 0.09 s, corresponding to Branches A and B. The IURIS results for Branch AB based on pressure injection show apparent phase matching of pressure damping between 0.04 and 0.08 s for a small leaky flange, as presented in Figure 6(b). The transient method followed the same pattern as observed using the rectilinear flange condition in Figure 5 regarding damping amplitude and branching pipe length.
Figure 6

IURIS in an experimental pipeline system with two branching pipes and a small leaky flange on both transient conditions of (a) instant valve closure and (b) pressure injection.

Figure 6

IURIS in an experimental pipeline system with two branching pipes and a small leaky flange on both transient conditions of (a) instant valve closure and (b) pressure injection.

Close modal
An example of an IURIS result for an instant valve closure condition for a pipeline system is illustrated in Figure 7(a). The pipeline system has two branching pipes and a large leaky flange. There are two distinct pressure-damping phases observed between 0.04 and 0.08 s when the leaky flange is large. Due to larger leak condition, two damping phases in Figure 7(a) involved more sharp and significant pressure drops than those in Figure 6(a). A good agreement between the two pressure-damping phases between 0.03 and 0.08 s indicates that multiple branching pipes can be detected under the large leak flange condition, as illustrated in Figure 7(b). Figures 6 and 7 demonstrate that two branching pipes may be detected regardless of the method of transient generation, the presence of complicated uncertainties, or the size of the leak.
Figure 7

IURIS in an experimental pipeline system with two branching pipes and a large leaky flange on both transient conditions of (a) instant valve closure and (b) pressure injection.

Figure 7

IURIS in an experimental pipeline system with two branching pipes and a large leaky flange on both transient conditions of (a) instant valve closure and (b) pressure injection.

Close modal

TBMBD experiments with series flange

TBMBD was further validated in the pipeline system using a series flange as the uncertainty zone (Figure 3). This series pipeline flange has the same material as the main pipeline, but its inner diameter is 0.25 m, which is greater than that of the main pipeline. As a pipeline system undergoes transient events, the wall thicknesses, wave speed, and friction factor differ from those of the standard pipe system (Chaudhry 2014; Jha et al. 2018; Malesińska et al. 2021). Under the same transient conditions as in the previous sections, an experiment signal was obtained based on an unknown assumed uncertainty.

A series flange in the experiment signal of valve closure condition caused pressure damping without a pressure drop or an overall pressure attenuation after damping. There are unexpected pressure fluctuations that obscure a confirmation of a series flange pressure response in the experiment signal under the pressure injection condition. The experiment signal experienced more pressure damping with more complicated noise responses than those in rectilinear and leaky flanges. By separating uncertainty from the developed TBMBD method, signal acquisition for TBMBD can be facilitated, despite these pressure responses in the extended flange condition.

As shown in Figure 8(a), IURIS results are shown for an instant valve closure with two branching pipes with 0.25 m series flanges. Compared to IURIS for Branches A and B, IURIS for Branch AB reveals a different scale of two pressure-damping phases between 0.04 and 0.09 s. The IURIS of Branch A involves smaller responses in terms of pressure-damping and weaker resilience in reflecting pressure waves. However, two branching pipes can be detected based on the timing of two distinct pressure-damping phases. The IURIS results for a pressure injection in the pipeline system are shown in Figure 8(b). Two branching pipes are detected in two distinct pressure-damping phases between 0.04 and 0.07 s by IURIS for Branch AB. It was difficult to detect Branch A in IURIS because pressure-damping between 0.03 and 0.04 s occurred frequently for both Branches A and B. Despite unexpected pressure fluctuations in the results, Branch A can be identified because of a larger pressure damping at 0.04 s. Under uncertainty conditions associated with the sudden expansion of the pipeline cross-sectional area, Figure 8 demonstrates the effectiveness of the proposed method for detecting two branching pipes.
Figure 8

IURIS in an experimental pipeline system with two branching pipes and 0.25 m series flange on both transient conditions of (a) instant valve closure and (b) pressure injection.

Figure 8

IURIS in an experimental pipeline system with two branching pipes and 0.25 m series flange on both transient conditions of (a) instant valve closure and (b) pressure injection.

Close modal

Specific evaluation and discussion for multi-branching pipes detection

Comprehensive IURIS was delineated for all flanges and transient conditions, and the locations of two branching pipes, A and B, were predicted as the distance from the pressure transducer to the branching pipe. Based on the wave speed of the main pipe and the specific timing of transient to a notable response in pressure damping of IURIS for Branch AB, the location of two branching pipes can be predicted. The wave speed in an experimental pipeline system is determined by the following equation (Chaudhry 2014):
(7)
where Le is the distance from the upstream reservoir to the pressure transducer and te is the corresponding reflection time of the pressure wave. Le is the extension of the pipeline, by 89.4 m (Figure 3). The value of te can be obtained from the experiment signal of a rectilinear pipeline system in transient condition by an instant valve closure. This is determined by measuring the elapsed time between the initial time when the normalized head is zero and the reflected time when the normalized head downed to zero. Alternatively, on pressure injection conditions, te can be estimated as the elapsed time from the specific timing of notable responses in reservoir pressure damping after transient initiation to the specific timing of the reflection of the corresponding signal. The ae appeared differently under the flange and transient conditions due to the presence of different flanges and other uncertainties in the system, and different ae were applied, respectively, to the location predictions for two branching pipes. The location of a branching pipe in the system can be predicted as follows:
(8)
where ae is the wave speed under specific conditions and tb is the reflection time of the pressure wave for a branching pipe. The tb can be found in IURIS for Branch AB (Figures 58) through the elapsed time from the moment of transient initiation to the specific timing showing notable response in pressure damping as presented in Table 1. The real positions of the Branching pipes A and B are 25.9 and 39.1 m from the pressure transducer, respectively (Figure 3). The potential position Lb is predicted using ae and tb, which indicates the distance from the pressure transducer to a branching pipe.
Table 1

The specific timing showing a notable response in pressure damping of IURIS under various uncertainties

Flange typesThe timing on instant valve closure (s)
The timing on pressure injection (s)
Branch ABranch BBranch ABranch B
Rectilinear flange 0.042 0.065 0.044 0.065 
Small leaky flange 0.055 0.074 0.045 0.066 
Large leaky flange 0.049 0.067 0.044 0.067 
0.25 m series flange 0.051 0.071 0.040 0.063 
Flange typesThe timing on instant valve closure (s)
The timing on pressure injection (s)
Branch ABranch BBranch ABranch B
Rectilinear flange 0.042 0.065 0.044 0.065 
Small leaky flange 0.055 0.074 0.045 0.066 
Large leaky flange 0.049 0.067 0.044 0.067 
0.25 m series flange 0.051 0.071 0.040 0.063 

According to Table 1, each condition showed different timing of the pressure damping phases. These differences resulted from different injection times of transient flow and partially by nonlinear ball valves, as well as different pressure wave speeds in the main pipe. Based on distinct specific timings, Table 2 presents predicted distances for two branching pipes, A and B, from the pressure transducer. The prediction errors for Branches A and B were less than 10% compared to the real positions. The conditions of the leaky flange showed the largest prediction error among all flanged conditions. Two branching pipes, A and B, may be hampered in their position prediction by the leaky flange, which causes greater pressure oscillations. For several uncertainties in the pipeline system, hydraulic pressure damping can be observed for detecting two branching pipes. However, it has been demonstrated that there are limited errors in determining the accurate positions for the two branching pipes.

Table 2

The location predictions of two branched elements using IURIS under various uncertainties

 Flange typesThe predicted position on instant valve closure (m)
The predicted position on pressure injection (m)
Branch A (real = 25.9 m)Branch B (real = 39.1 m)Branch A (real = 25.9 m)Branch B (real = 39.1m)
Rectilinear flange 25.2 38.8 26.6 39.3 
Small leaky flange 28.3 41.1 27.8 41.5 
Large leaky flange 27.8 39.3 28.1 42.8 
0.25 m series flange 26.9 40.1 25.2 40.0 
 Flange typesThe predicted position on instant valve closure (m)
The predicted position on pressure injection (m)
Branch A (real = 25.9 m)Branch B (real = 39.1 m)Branch A (real = 25.9 m)Branch B (real = 39.1m)
Rectilinear flange 25.2 38.8 26.6 39.3 
Small leaky flange 28.3 41.1 27.8 41.5 
Large leaky flange 27.8 39.3 28.1 42.8 
0.25 m series flange 26.9 40.1 25.2 40.0 

This study developed an abnormality detection scheme for multi-branching elements in a pilot-scale pipeline system with uncertainties using transient analysis and experiments. The key point is that even though uncertainties in the pipeline system were left in an unknown state, detecting multi-branching pipes can be achieved through the application of the developed systematic signal processing. This means that the uncertainty of a pipeline system can be properly treated without realistic configuration, such as characterization and quantification, which had been explored in most existing uncertainty studies (Duan & Keramat 2022; Hu et al. 2023; Tjuatja et al. 2023; Wang et al. 2023). Consequently, the method proposed in this study has the potential to expand to diagnose the other specific unknown components (e.g., blockage) as well as unknown branching elements for pipeline systems while the other uncertainties (e.g., wave speed and transient condition) were treated as the unknown components. We believe that the proposed method can substantially relax the limitations of pipeline diagnosis, which are associated with unknown uncertainty.

This paper proposed a method to enhance the field applicability of the TBMBD scheme as an extended study from the authors’ previous work. The key objective of the method is to identify multi-branching pipes in pilot-scale pipeline systems with several unknown uncertainty conditions. Systematic signal processing for the isolation of uncertainty signals was proposed. Uncertainty signals were separated by superimposing transient-based experimental signals with unknown uncertainty signals and numerical data without uncertainties from the PTM. Original uncertainty signals were utilized in the developed TBMBD method to acquire IURIS for detecting multi-branching pipes from experimental pressure signals. The developed TBMBD method was experimentally validated with a two-branching-pipes system with uncertainties of various pipe flanges under two transient conditions, instant valve closure and pressure injection.

The two branching pipes in the pilot-scale pipeline system with uncertainties can be detected under all conditions of various pipe flanges and transients. It was identified in two distinct phases of hydraulic pressure damping in IURIS for Branch AB. Even though there were limited errors (<10%) in determining the accurate positions for the two branching pipes, the distinct responses for detecting the two branching pipes can be achieved through systematic signal processing for separating uncertainty signals and the developed TBMBD method. It can be applicable to a rectilinear pipeline system regardless of the number of branches, the method of transient generation, the wave speed in the system, and the presence of complicated uncertainties.

However, it is only possible to detect multi-branching pipes in a rectilinear reservoir-pipe-valve system with reasonable distances between branching pipes. A multi-branching pipe that has pipes too close to each other makes it challenging to accurately identify its position due to interference between reflected waves from the branches. Nevertheless, this paper shows meaningful results that it enables the diagnosis of a pipeline system in terms of handling uncertainties in the system itself. A noteworthy contribution is the detection of multi-branching pipes without the use of unknown uncertainties. This approach can increase the revenue water ratio in urban water systems by reducing unexpected water use. It can be further improved for field applicability by considering more uncertainties in a pipeline system, such as the presence of looped pipes or outflow from branching pipes, which significantly affect steady flowrate. Further study needs to be carried out under conditions of more disturbances in various pipeline systems and elaboration of the developed signal processing method, which can be a promising direction simply because of the viewpoint of uncertainty itself, which can not only relax the existing understanding of uncertainty but also provide an effective isolation platform for distinct uncertainties in transient signals.

This work was supported by the Daegu Gyeongbuk Institute of Science and Technology (DGIST) Research and Development (R&D) of the Ministry of Science and Information & Communications Technology (ICT) (Grant number 2024010409), the Electronics and Telecommunications Research Institute (ETRI) grant funded by the Korean government (Grant number 24ZD1120, Regional Industry Information Technology (IT) Convergence Technology Development and Support Project), and the National Research Foundation of South Korea (Grant number 2022R1A4A5028840).

All relevant data are included in the paper or its Supplementary Information.

The authors declare there is no conflict.

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