Pipe bursts in water distribution systems (WDS) must be rapidly detected to minimize the loss of system functionality and recovery time. Pipe burst is the most common failure in WDS. It results in water loss out of the system, increased head losses, and low pressure at the customers' taps. Therefore, effective and efficient detection of pipe bursts can improve system resilience. To this end, this study proposes an optimal meter placement model to identify meter locations that maximize detection effectiveness for a given number of meters and type of meter. The linear programming model is demonstrated on a modified Austin EPANET hydraulic network. Receiver operating characteristic (ROC) curves for alternative pressure and flow meters are applied to investigate the relationship between the level of available information and pipe burst detection effectiveness. The optimal sensor locations were distinctly different depending on the type of meter and the objective to be considered. The ROC curves for alternative pressure and pipe flow meters showed that pipe flow meters are vulnerable to false alarms, and that using many pipe flow meters could detect all pipe bursts. Pressure meters could detect up to 82% of the burst events.

## NOMENCLATURE

*a*emitter pressure exponent

*C*emitter discharge coefficient

**D**detection matrix

*D*_{ij}an element of

**D**having a value of 1 or 0, indicating whether the*i*th burst event would be or would not be detected, respectively, by the*j*th meter*i*index for burst events

*j*index for meters

*m*total number of nodes or pipes

*N*_{d}number of burst events that were detected

*N*_{tb}total number of burst events

*p*_{t,i}pressure at node

*i*at time*t**q*_{t,i}burst flow at node

*i*at time*t**t*_{di}time (h) of detection of the

*i*th detected burst event*t*_{bi}time (h) of occurrence of the

*i*th detected burst event**X**configuration vector

*X*_{j}an element of

**X**indicating whether there is a meter at the*j*th location (i.e., node or pipe) or not*X*_{max}number of available meters

- ADT
average detection time

- CUSUM
cumulative sum

- CL
control limit

- DP
detection probability

- EWMA
exponentially weighted moving average

- MCUSUM
multivariate CUSUM

- MEWMA
multivariate EWMA

- ROC
receiver operating characteristic

- RF
rate of false alarm

- SCADA
supervisory control and data acquisition

- SPC
statistical process control

- WL
warning limit

- WEC
Western Electric Company

## INTRODUCTION

Pipe burst refers to the rupture of a pipe due to pipe deterioration, excessive pressure, or ground shifts caused by temperature changes or earthquakes. Water loss through the rupture increases the total flow entering the system, overall pipe flow rates, and head losses through pipes, which in turn, lowers the pressure at the customers' taps. Morrison (2004) reported that the time for detection and location of a 1.1 lps burst was approximately 5 days. Degradation of system functionality (i.e., performance level) persists until the broken pipe is fully repaired. Therefore, early detection of pipe bursts helps improve system resilience by minimizing water losses and system impact. In addition, it saves the energy cost spent in lifting the additional quantity of water.

Over the last two decades, several methodologies have been developed to detect pipe bursts. Most approaches assume the availability of information on measured pipe flows and/or system pressures from supervisory control and data acquisition (SCADA) systems, and include artificial neural networks (Mounce *et al.* 2002, 2003, 2010; Mounce & Machell 2006), state estimation (Andersen & Powell 2000; Ye & Fenner 2011, 2013), Bayesian approach (Poulakis *et al.* 2003), and time series modeling (Quevedo *et al.* 2010). Constructing a district metered area (DMA)-structured network was considered the most common alternative for detecting unreported leakages and small bursts (Morrison 2004; Misiunas *et al.* 2005; Sturm & Thornton 2005; Alkasseh *et al.* 2013).

Statistical process control (SPC) methods are most widely applied in the detection of pipe bursts (Misiunas *et al.* 2006; Romano *et al.* 2010, 2014; Palau *et al.* 2012; Jung *et al.* 2015). SPC methods apply statistical theory to the system output parameters (i.e., the measurable quality parameters, also known as quality characteristics) to identify non-random patterns that may be caused by bursts.

Romano *et al.* (2010) applied the Western Electric Company (WEC) rules (Western Electric Company 1958) to the pressure data from a 13 m long pipeline deployed in a DMA to identify pipe bursts generated by opening hydrants. Normal pressure data were used to compute time-varying mean and standard deviation that are the bases of Shewhart control chart and the resulting warning and control limits (CLs). Violating any of the four rules in the WEC rules caused an alarm. In a follow-up paper, Romano *et al.* (2014) employed the WEC rules in a real-time event detection model that included preprocessing of pipe flow/pressure measurements, forecasting pipe flows/pressures, detecting pipe bursts/other events, and estimating the probability of the events. The WEC rules are fixed as identifiers, thus making its application straightforward.

Jung *et al.* (2015) compared the performance of six SPC methods for pipe burst detection with respect to their detection effectiveness and efficiency: three univariate methods (the WEC rules, the cumulative sum (CUSUM), and the exponentially weighted moving average (EWMA) methods) and three multivariate methods (Hotelling *T*-squared, multivariate CUSUM (MCUSUM), and multivariate EWMA (MEWMA) methods). Hypothetical pipe flow and pressure measurements were generated at predefined locations in a modified Austin network (Brion & Mays 1991). The EWMA had the best detection effectiveness and efficiency among the six SPC methods.

### Optimal sensor network design to detect bursts

In addition to being affected by the detection method, pipe bursts' detectability is affected also by the network structure and the available information. During design, the network structure is largely determined by land use, topography, and water demand distribution; pipe burst detection is not a primary concern at this stage. The amount of information on pipe burst detection in a measurement is a function of the number and types of meters and their locations, as well as the network structure and burst location. As such, measurements at some locations can include more signals of an anomaly than measurements at other locations.

To improve pipe burst detectability, the number of meters within the system can be increased. However, the number of meters that can be installed is normally limited by the network's structure, and more importantly, by the available budget. Therefore, finding an optimal sensor network design under budget constraints is a challenging task. Sensor network design methodology must identify: (1) the optimal number of meters, (2) the optimal combination of meters (pressure and pipe flow meters), and (3) the locations of the meters, and incorporate an optimal methodology for pipe burst detection.

In the water distribution systems (WDS) domain, a few studies have proposed sensor placement methodologies for pipe burst detection. Farley *et al.* (2010) have developed a sensor placement methodology to determine the most sensitive locations of pressure meters to detect pipe bursts at different locations. The approach was based on the Jacobian sensitivity matrix of pressure change as a function of burst rate at a given location. The Jacobian matrix was converted to a binary matrix where ‘1’ indicates that the pressure change is less than an arbitrary chosen threshold value, and ‘0’ indicates otherwise. The number of burst events detected was maximized using the generated binary matrix. In a follow-up paper, they proposed a pipe burst localization method using the Jacobian matrix (Farley *et al.* 2013). Perez *et al.* (2009) proposed a sensor placement method that determines the location of the smallest number of pressure meters for burst detection and localization. An enumeration technique was used to determine the threshold value for the Jacobian-binary matrix conversion. Wu & Song (2012) developed a pressure meter location method that maximizes the number of unique leakage events detected for a given number of candidate locations. Analogous to Farley *et al.* (2013) the Jacobian matrix of the pressure change was converted to a binary matrix, using the sensor instrument's measurement error as the threshold value. Huang *et al.* (2012) developed a clustering-based pressure meter placement method for pipe burst detection, by which the optimal number of meters was determined. A few studies considered a different criterion (e.g., accuracy of state estimation) for determining sensor locations (Kang & Lansey 2010).

While most previous studies were based on the Jacobian matrix of pressure change as a function of burst rate, an arbitrary threshold value was applied to convert the Jacobian matrix to a binary matrix. However, a more efficient pipe burst detection methodology (e.g., SPC method) should be applied to the raw field measurements to develop the binary matrix. In addition, most of the previous sensor placement studies focused on pressure meters only, without considering the potential detection effectiveness of pipe flow meters. Further, they neglected the importance of false alarms in determining sensor locations.

In this study, we develop and solve an optimal WDS meter placement model to identify the optimal meter locations that maximize detection effectiveness for a given number of meters and type of meter. An SPC method is used to populate the detection matrix (i.e., binary matrix) in the model. The linear programming-based model is demonstrated on a modified Austin network (Brion & Mays 1991). First, the pipe burst detection characteristics are investigated based on a single meter's performance. Then, the optimal sensor networks for pressure and flow meters are independently determined and compared. Finally, the trade-off relationship between the number of available meters and pipe burst detection effectiveness (with respect to not only detection probability (DP), but also false alarm frequency) is investigated by plotting the latter against the former.

## METHODOLOGY

### Detectability measures

*DP*and the rate of false alarm (

*RF*).

*DP*is the proportion of burst events that were detected (

*N*) among the total number of burst events (

_{d}*N*):

_{tb}*RF* is the proportion of natural random events in which a false alarm is issued among the total number of natural events. Therefore, *DP* is related to the false negative (type II error) rate, while *RF* indicates false positive (type I error) rate. The receiver operating characteristic (ROC) curve (Egan 1975), a graphical plot that illustrates the performance of a binary classifier system, is created by plotting the true positive rate against the false positive rate at various threshold settings. Therefore, the ROC curve for a sensor network for pipe burst detection displays plots of *DP* and *RF* for different number of meters to explore the trade-off between the two metrics.

*ADT*, h), i.e., the averaged value of the time taken for detection, is used here as the detection efficiency indicator:where

*t*is the time (h) of detection of the

_{di}*i*th detected burst event, and

*t*is the time (h) of occurrence of the

_{bi}*i*th detected burst event. Normally,

*t*of a burst is not known in real life, so this statistic is tested using synthetic data. Given the same detection effectiveness (i.e., the same

_{bi}*DP*and

*RF*), a sensor network with a shorter

*ADT*is more favorable. As the detection time is infinite for a non-detected pipe burst, water utilities generally place more importance on the effectiveness measures than the

*ADT*. In summary, to improve resilience, it is desirable to have a high

*DP*, low

*RF*, and low

*ADT*.

### Binary integer programming model for optimal meter location

*DP*for a given number of meters (

*X*).subject towhere

_{max}*m*is the total number of potential meter locations (i.e., total number of nodes or pipes). Prior to optimizing the system, a detection matrix () is generated. The rows and columns of

**D**correspond to potential burst events and potential meter locations, respectively. The elements of

**D**(i.e.,

*D*) are 1 or 0, which indicate whether the

_{ij}*i*th burst event would be or would not be detected, respectively, by the

*j*th meter. The development of

**D**is described in detail below. The problem decisions are also binary and are denoted by the configuration vector (). If

*X*= 1, a meter is placed at location

_{j}*j*(zero for no meter). For a given burst event

*i*, the product of

*D*and

_{ij}*X*in Equation (4) equals 1, if a meter is installed at location

_{j}*j*(

*X*= 1) and the burst can be detected by the meter at that location (

_{j}*D*= 1).

_{ij}The problem's objective (Equation (3)) is to maximize *DP* that is computed from the intermediate binary problem variable *α _{i}*. If one or more meters would detect burst

*i*, then

*α*is set equal to 1 (Equations (4) and (5)). If all possible sets of meters are considered, the search space of the problem will be 2

_{i}^{m}. Here, the number of meters is included as a constraint (Equation (6)): (1) to reduce the search space, (2) to consider a field situation where the possibility of placing meters in the system is limited, and (3) to exclude the need for system-specific meter cost data.

Cost can be the main decision driver in this problem; the other drivers are meter types' access to power or SCADA data lines, and the location relative to these lines. For example, installing flow meters in a WDS is more expensive than installing pressure meters, because they require excavation, installation of a valve and a meter, backfilling, and pavement work (Walski 2012). On the other hand, pressure meters can often be installed inexpensively on fire hydrants. The flow meter is also more expensive than a pressure meter. To minimize cost, the above problem could be modified by deleting Equation (6) and changing the objective to the cost of installed meters and introducing a budget constraint. Equation (3) would become a constraint with a lower bound on the acceptable *DP*. Similarly, the false alarm rate can also be bounded by adding a false alarm matrix similar to **D,** but corresponding to a set of non-burst conditions that some meter locations identify as bursts. An alternative approach is to minimize *RF*; this also requires a false detection matrix (**D**_{f}) analogous to **D**. The rows and columns of **D**_{f} correspond to natural random events and potential meter locations, respectively. As in the case of **D**, the elements of **D**_{f}**(***D _{f,ij}*

**)**are 1 or 0 indicating whether a false alarm would be or would not be raised, respectively, on the

*i*th natural event by the

*j*th=meter.

### Overview of model development

**D**. For a given WDS, a period of random demands is simulated to determine the mean and variance of nodal pressures and pipe flow rates throughout a diurnal cycle. Demands are based on a historical record or a predicted range of variability. These statistics are the basis for the Shewhart control charts for each node or pipe. Shewhart control charts and the WEC detection rules form the foundation for this application, but other detection tools can be substituted, if desired.

*et al.*2005; Jung

*et al.*2015).

To assess a sensor network's effectiveness, control measurements are generated considering randomness in nodal demands only, while out-of-control measurements are produced considering both random pipe bursts and random demands. The latter is used to develop a detection matrix, and the former is used to form a false alarm matrix. For both conditions, the WEC rules described below are applied to detect the outliers. With the detection matrix **D**, the optimization problem (Equations (3)–(6)) can be formed and solved. The optimal locations to limit the frequency of false alarms are also determined. Therefore, the objective function is to minimize *RF* by replacing *D _{ij}* with

*D*in Equation (4).

_{f,ij}### Burst simulation

*i*at time

*t*,

*C*is the emitter discharge coefficient, is the pressure at node

*i*at time

*t*, and

*a*is the emitter pressure exponent. Lambert (2001) conducted an experimental study to investigate the accuracy of the power function model represented by Equation (7), and provided guidelines on using the exponent

*a*based on the pipe material and the level of burst/leakage. He has suggested that an exponent of 0.5 be used to simulate large detectable leakages in metal pipes, while an exponent of 1.0 (indicating a linear relationship between discharge and pressure) can be used if no information on the pipe material is available. Fuchs-Hanusch

*et al.*(2015) summarized and reported the exponent values derived from field and experimental studies, which cover various pipe materials and failure modes (e.g., round hole and longitudinal cracks). While a wide parameter range was observed for the exponent, the most commonly identified range was around 0.5 (May 1994; Greyvenstein & van Zyl 2007; Walski

*et al.*2009). To simulate pipe bursts of various magnitudes, the emitter discharge coefficient

*C*is considered as a random variable.

### WEC rules

The WEC rules (1958) are a set of decision rules based on the Shewhart control chart for detecting non-random patterns in measured data (Montgomery 2009). Romano *et al.* (2010) modified the original WEC rules for WDS pipe burst detection and for identifying a non-random pattern, if the measured quality characteristic satisfies any of the following rules.

Rule 1. Any single measurement is beyond the CL.

Rule 2. Two out of three consecutive measurements are beyond the WLs.

Rule 3. Four out of five consecutive measurements are beyond the WLs.

Rule 4. Eight consecutive measurements are beyond the WLs.

The term refers to the warning/CL that is plus or minus *n* standard deviations from the mean. The WEC rules are applied to one side of the centerline at a time. In other words, a measurement on one side, immediately followed by a measurement on the other side of the centerline outside the WLs will not be taken into account as a non-random pattern. The WEC rules consider, at most, the eight most recent past measurements, having a potential to consider series of previous measurements in decision. Most of the previous detection methods used in sensor placement methodologies took into account a single/current measurement (Farley *et al.* 2010; Wu & Song 2012).

The WEC rules are easy to implement with no parameters to be estimated. Jung *et al.* (2015) confirmed that the WEC rules outperformed multivariate SPC methods with respect to *DP*. A *DP* of over 76% was obtained by applying the WEC rules when measurements of five meters are provided in a loop-dominated system. The *DP* increased up to 93% when pressure measurements of five meters are used for applying the WEC rules. On the other hand, application of the WEC rules results in relatively high false alarm rates when multiple meters are used. Therefore, determining the location of meters that yields minimum false alarm is also important while applying the WEC rules.

### Detection and false alarm matrix

The detection matrix (**D**) has binary elements in which the *i*th row lists all the pressure/pipe flow meters that detect the *i*th pipe burst as per the WEC rules; its *j*th column lists all the pipe bursts detected by the *j*th pressure/pipe flow meter. The following steps are followed to populate **D** (Figure 2).

Step 1. Generate a large number of pipe bursts with random magnitudes and locations.

Step 2. Generate 100 2-day traces of pressure/pipe flow measurements considering random demands and the pipe bursts generated in Step 1.

Step 3. Assuming that the

*j*th pressure/pipe flow meter is installed in the network, determine if the*i*th burst is detected by examining the post-burst pressure/pipe flow measurements as per the WEC rules.Step 4. Set the element at the

*j*th column's*i*th row as 1 if the*i*th pipe burst is detected by the*j*th meter and 0 otherwise.Step 5. Repeat Step 4 for all pipe bursts (

*i*= 1, …,*N*).Step 6. Repeat Steps 3–5 for all pressure/pipe flow meters (

*j*= 1, … ,*m*).

To identify the optimal meter locations that yield minimum false alarm rates, a false alarm matrix can be developed in a similar manner, but constructed for random demand conditions without pipe bursts. The false alarm matrix has binary elements in which the *i*th row lists all pressure/pipe flow meters that raise a false alarm from the measurements resulting from the *i*th series of natural variability.

## APPLICATION NETWORK

The optimal meter placement model was applied to a modified Austin network (Brion & Mays 1991). The modified network is a branch-dominated transmission system with several looped subareas. It consists of 125 nodes, a fixed head reservoir, 90 pipes, and seven pumps. The pipe sizes range from 152 mm (6 in) to 1,829 mm (72 in). Three out of the seven pumping units were consistently operated.

The other data sets were (1) a control sample and (2) the out-of-control set used to construct the false alarm and detection matrices, respectively. The control sample considers only natural demand randomness. The out-of-control data set includes demand randomness and pipe bursts. In total, 100 burst events and 100 natural random events were considered. The random burst characteristics are the burst location, initiation time, and burst magnitude. The burst magnitude is defined by the emitter coefficient *C* that was assumed to be uniformly distributed over the range of 1 to 50. A leakage exponent *a* of 0.5 is used for all the bursts. The resulting burst magnitudes ranged from 0.1 to 3.3% of the total system mean demand (726 lps). The quality characteristics' control and out-of-control measurements from a location were provided at a time for evaluation as per the WEC rules to populate the false alarm and detection matrices, respectively.

Shewhart control charts with a centerline, three WLs, and a single CL were constructed from the historical data set generated (Figure 3) for each potential meter location (i.e., all nodes and pipes). The mean nodal pressures and pipe flow rates vary over time because of the diurnal demand pattern. While the variances of pipe flow rates are relatively constant through the day, the nodal pressures have high uncertainty during peak demand hours, resulting in wider CLs. Low variations in nodal pressure were observed at night and early morning because of the low demand and low variability during these periods. Control and out-of-control measurements were evaluated as per the WEC rules, using the Shewhart control chart for the desired meter location, to construct the false alarm and detection matrices, respectively. The results for a pressure meter installed at node 15 and representing 15 burst events are summarized in Table 1.

Burst events . | Detection (Yes/No) . | Detected by rule . | ||||||
---|---|---|---|---|---|---|---|---|

Event ID . | Location (node ID) . | Burst time index* . | Detection time index . | Time to detect (h) . | Emitter coefficient . | Burst flow rate (lps) . | ||

1 | 89 | 307 | 314 | 0.6 | 29 | 16.6 | Yes | 4 |

2 | 77 | 345 | 8 | 4.0 | No | |||

3 | 26 | 522 | 13 | 6.5 | No | |||

4 | 22 | 504 | 910 | 33.8 | 15 | 7.5 | Yes | 1 |

5 | 35 | 56 | 57 | 0.1 | 41 | 22.2 | Yes | 1 |

6 | 76 | 291 | 313 | 1.8 | 27 | 14.4 | Yes | 1 |

7 | 108 | 378 | 540 | 13.5 | 32 | 18.3 | Yes | 1 |

8 | 99 | 444 | 848 | 33.7 | 9 | 5.2 | Yes | 1 |

9 | 48 | 92 | 13 | 7.3 | No | |||

10 | 59 | 92 | 281 | 15.8 | 29 | 15.5 | Yes | 4 |

11 | 94 | 516 | 563 | 3.9 | 48 | 27.4 | Yes | 2 |

12 | 5 | 320 | 330 | 0.8 | 45 | 20.1 | Yes | 1 |

13 | 5 | 58 | 586 | 44.0 | 23 | 10.3 | Yes | 3 |

14 | 34 | 316 | 320 | 0.3 | 38 | 20.5 | Yes | 2 |

15 | 61 | 406 | 10 | 5.3 | No |

Burst events . | Detection (Yes/No) . | Detected by rule . | ||||||
---|---|---|---|---|---|---|---|---|

Event ID . | Location (node ID) . | Burst time index* . | Detection time index . | Time to detect (h) . | Emitter coefficient . | Burst flow rate (lps) . | ||

1 | 89 | 307 | 314 | 0.6 | 29 | 16.6 | Yes | 4 |

2 | 77 | 345 | 8 | 4.0 | No | |||

3 | 26 | 522 | 13 | 6.5 | No | |||

4 | 22 | 504 | 910 | 33.8 | 15 | 7.5 | Yes | 1 |

5 | 35 | 56 | 57 | 0.1 | 41 | 22.2 | Yes | 1 |

6 | 76 | 291 | 313 | 1.8 | 27 | 14.4 | Yes | 1 |

7 | 108 | 378 | 540 | 13.5 | 32 | 18.3 | Yes | 1 |

8 | 99 | 444 | 848 | 33.7 | 9 | 5.2 | Yes | 1 |

9 | 48 | 92 | 13 | 7.3 | No | |||

10 | 59 | 92 | 281 | 15.8 | 29 | 15.5 | Yes | 4 |

11 | 94 | 516 | 563 | 3.9 | 48 | 27.4 | Yes | 2 |

12 | 5 | 320 | 330 | 0.8 | 45 | 20.1 | Yes | 1 |

13 | 5 | 58 | 586 | 44.0 | 23 | 10.3 | Yes | 3 |

14 | 34 | 316 | 320 | 0.3 | 38 | 20.5 | Yes | 2 |

15 | 61 | 406 | 10 | 5.3 | No |

*****Burst time index refers to the index of time, starting from a value of 0 at midnight and increasing by 1 every 5 min.

A number of assumptions and simplifications were made in this hypothetical case study: (1) the hydraulic model perfectly represents the real system; (2) the pipe roughness coefficients and other system parameters are known with certainty; (3) a burst that is not detected within 48 h after its occurrence is considered as a non-detected event; (4) a natural random event that does not cause a false alarm within 48 h is considered as a non-false alarming event; (5) only one burst occurs in a span of 48 h; (6) the measurement error of a meter is negligible; (7) measurements are available every 5 min without any missing measurement; (8) only one meter is installed per node/pipe; and (9) the pressure and pipe flow rates are normally distributed around their mean centerlines in the Shewhart control chart, as confirmed in the study by Jung *et al.* (2015). In order to compare alternative pressure/pipe flow meters' configurations, detectability measures (Equations (1) and (2)) are calculated.

## APPLICATION RESULTS

### Impact of pipe burst characteristics on detectability

*DP*for pressure and flow meters is given in Figure 5. Nearly all the pressure meters have a

*DP*of approximately 70%, while the pipe flow meters generally have relatively low

*DP*s. The few locations with low

*DP*s are in the fringes of the network. In many cases, common events are detected by all the pressure meters, as shown in Figure 6(a) (heat plot of detections on the vertical axis and meters on the horizontal axis). Each flow meter detects different events (Figure 6(b)). A black spot indicates that a burst is detected by the given meter, so a dark row shows detection by many meters. In this case, 63% of the bursts are detected by all the pressure meters (Figure 7). The remaining 37% are identified by much smaller subsets; this result suggests the need for a study of the optimal sensor placement problem. However, burst detection by meters at many locations raises questions on the value in locating a burst after a detection using pressure meters that is beyond the scope of this study.

*DP*of 66% was for the pipe connecting the source to the pump station. The other flow meters with

*DP*higher than 60% also have high flow rates (the pipe just downstream of the pump station, the transmission pipe closest to the pump station, and a distribution pipe within the southwestern loop). This result is reinforced by the plot of

*DP*versus flow rate (Figure 9), which suggests that transmission lines are the best locations for flow meters. In practice, therefore, flow meters are installed on each inlet pipe (i.e., transmission pipe) in a DMA-structured network (Alkasseh

*et al.*2013). It is important to note that while many pressures meters can detect a large set of the same bursts, each flow meter detects fewer events that are likely to be more localized (Figure 6(b)). As might be expected, the ratio of the number of meters that detect a pipe burst to the total number of meters (i.e., detection rate) is related to the burst magnitude (Figure 10). All the bursts greater than 1.2% of the total demand were detected by all the pressure meters, while only some of the flow meters identified the bursts.

*RFs*are small for most pressure and flow meters in this system. A few flow meter locations did have high

*RFs*(e.g., a distribution pipe within the southeast loop has an

*RF*of 50%) (Figure 11).

*et al.*2013).

*et al.*2015).

### Optimal meter placements

The meter location problem (Equations (3)–(6)) was solved for the Austin system for pressure meters with *X _{max}* ranging from 1 to 125. For pipe flow meters, a maximum of 90 pressure meter locations was available. The

*RF*for the best

*DP*set was computed. In addition to optimizing the

*DP*, meter locations that minimized false alarm were also determined. The three results were combined in the ROC curves. A hundred random pipe bursts events were considered for the optimization. The detection and false alarm matrices had dimensions of 100 by 125 binary matrices for pressure meters, and 100 by 90 for flow meters. The binary integer programming problem was solved by the general reduced gradient (Abadie 1970) nonlinear solver in Microsoft Excel 2007. The solver was implemented on a 3.4 GHZ Intel Core i7 Quad processor with 8 GB of memory, running Window 7. A CPU time of approximately 0.27 s was required to find an optimal solution of the problem with a predefined number of available meters.

*X*ranging from 1 to 4. While the optimal flow meter locations were near the source (Figure 15), the best sites for pressure meters were in the distal network locations (Figure 14). For example, when only a single meter was permitted, a pressure meter was installed at node 98 within the northeast loop with a

_{max}*DP*of 68% (Figure 14), while a flow meter was installed in pipe 2 with a

*DP*of 63% (Figure 15). Although node 98 is an optimal location for the pressure meter, many other nodes in this system provide almost equivalent coverage. In the case of two allowable pressure meters, the meters were located in the north end of the network at nodes 58 and 65. On the other hand, one of the two flow meters was located at the source connecting pipe, while the other meter was installed within the southwestern loop. Similarly, one of the four flow meters was located near the source (Figure 15). It may be noted that several optimal or near-optimal solutions are available. As more meters were used, the

*ADT*decreased sharply.

The differences in the optimal meter layout are because of the hydraulic characteristics of pressure and pipe flows. The pressure meter location having the most information for pipe burst detection is at the end of the network, because the pressure will drop when any nodal demand in the system is increased because of higher upstream head losses. On the other hand, the best flow meter location is in the pipes near the source, because pipe flows are affected most by the changes in flow downstream of the meter location.

*RF*. In contrast to the best

*DP*locations, pressure meters were located near the source, and flow meters were installed in pipes in the network extremities. For example, a single flow meter's location that yields the lowest false alarm rate is pipe 91 which is connected to a dead end node. The pipe flows at the local pipes provide little information to detect a burst. This result demonstrates that maximizing the

*DP*and minimizing the

*RF*are contradictory goals, and the best

*DP*locations are not likely to be the minimum

*RF*locations. In practice, an alternative is to install sensors at both the best

*DP*and minimum

*RF*locations, and determine an alarm considering the decisions made from the two locations.

*DP*and

*RF*. As the number of meters in the sensor network increases, both

*DP*and

*RF*increase. Figures 18(a) and 18(b) show the ROC curves for the pressure and flow meters, respectively. The x-axes represent the percentage of nodes (Figure 18(a)) or pipes (Figure 18(b)) with the installed meters, and the y-axes represent the pipe burst detection and false alarm rates, respectively, in the two figures. For a given number of meters, the optimal meter placement model identified their best locations in the network. Pressure and flow meter sensor networks were determined independently. The

*RF*computed for the optimal

*DP*sensor networks and the minimum

*RF*for the same number of meters are also plotted.

Both meter types show a rapid increase in *DP* when the sensor network has only a few meters. For example, the five optimally located pressure meter network (meter installation level of 4%) has a *DP* of 72%, while the best five flow meter network (meter installation level of 5.6%) has a DP of 87%. When 10% of the pipes are monitored with flow meters, the *DP* is nearly 100%, and the *DP* is virtually 100% with 37 flow meters (meter installation level of 30%) (Figure 18(b)). The highest *DP* for pressure meters is approximately 82%. Although the *DP* is higher for flow meters, the false alarm rate is also high. The *RF* for the optimal pressure meters is consistent and lies between 10 and 20%. On the other hand, increasing the number of flow meters increases the *RF* until an *RF* of approximately 96% is reached.

## SUMMARY AND CONCLUSIONS

Burst detectability is related to the magnitude of the burst and proximity to a sensor. Given the ability to install meters at many locations, it is difficult to identify the best sensor locations using only engineering judgment. Hence, a general optimal meter placement model to maximize the detectability of pipe bursts has been formulated as a binary integer optimization problem, and solved for a real network with hypothetical demands. The model designs a sensor network that attempts to detect a set of randomly generated bursts.

A multi-step process is required to formulate the meter placement problem, including: (1) developing Shewhart control charts for each possible flow and pressure meter location using the network's hydraulic model and random nodal demands; (2) generating control and out-of-control events to test the sensor network's ability to detect anomalies; (3) applying the WEC rules to produce false alarm and detection matrices for the test events; and (4) solving the binary integer optimization problem. Two objective functions, to maximize the *DP* and minimize the *RF*, were posed while constraining the allowable number of meters. The ROC curves were evaluated for the resulting designs, and the sensitivities of *DP* and *RF* were investigated with respect to the level of available information.

Prior to solving the optimization problem, the results from the first three process steps were studied to better understand the burst detection monitoring. Pipe burst detection characteristics were investigated based on a single meter's performance. Most pressure meters had a *DP* of approximately 70%, which is much higher than the overall *DP* of the flow meters. On the other hand, the *RF* was less than 10% regardless of the type of meter. Many pressure meters can detect a large set of the same bursts, while each flow meter detects fewer events that are likely to be more localized. Finally, most pipe bursts were detected at night and early morning because of low demand variability during these periods.

The optimal sensor networks were distinctly different depending on whether pressure or flow meters were installed. While maximizing the *DP*, the pressure meters were located at distal locations relative to the water source, while the pipe flow meters were installed near the source. The meter locations that yield minimum false alarm were also identified. The results were opposite to those corresponding to the best *DP* locations. The optimum location for pressure meters is near the source, while the optimum location is near the end of the network for pipe flow meters. It appears that the downstream nodes are impacted more by bursts due to higher head losses that accumulate through the network during a burst. Conversely, the flow at the upstream pipes is more sensitive to the downstream anomalies. The ROC curves for the alternative pressure and pipe flow meters showed that using many pipe flow meters could detect all the pipe bursts when the maximum *DP* with the pressure meters was 82%. As flow meters are vulnerable to false alarms, using pressure meters is likely to be more valuable for pipe burst detection in the modified Austin network.

The proposed sensor placement model employed the WEC rules which are the easiest to implement, as there are no parameters to be estimated. However, other SPC methods with higher detection effectiveness, such as CUSUM and EWMA can replace the WEC rules for improving detectability, although the system-specific parameters should be estimated by paying high computational costs.

This study has several limitations that future research must address. First, as in most sensor network designs, the layout is based on a limited set of conditions. Here, we have defined a set of bursts; the final design may be biased by this set, and some study should be conducted to determine how large a set is needed to converge to a consistent design. Multiple simultaneous bursts can be generated and provided for burst detection. Second, this study determined the optimal locations for pressure and flow meters independently. The optimal combinations of pressure and flow meters and their locations can be determined with a small extension of the posed model. Along this line, meter costs and a budget constraint can be included in the optimization model, instead of only limiting the number of meters. Third, as confirmed from this study, a trade-off exists between *DP* and *RF*. Multi-objective optimal meter placement problems can be formulated to minimize total meter cost and *RF* and maximize *DP*. This study and the previous studies focused on burst occurrence detection. However, since all the pressure meters detect the same set of bursts, they provide little information on where the burst is located. To provide a truly effective monitoring system, it is necessary to simultaneously consider the possibility of detecting and locating bursts, while minimizing false alarms and detection time. Finally, the proposed approach can be applied to detect real-life bursts by including additional preprocessing steps such as raw measurement filtering.

## ACKNOWLEDGEMENTS

This material is based in part upon the work supported by the National Science Foundation under Grant No. 0835930. The opinions, findings, and conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect the views of the National Science Foundation.