| Literature DB >> 30443574 |
Armando Di Nardo1,2,3, Michele Di Natale1,2, Carlo Giudicianni1, Roberto Greco1,2, Giovanni Francesco Santonastaso1,2.
Abstract
In order to improve the management and to better locate water losses, Water Distribution Networks can be physically divided into District Meter Areas (DMAs), inserting hydraulic devices on proper pipes and thus simplifying the control of water budget and pressure regime. Traditionally, the water network division is based on empirical suggestions and on 'trial and error' approaches, checking results step by step through hydraulic simulation, and so making it very difficult to apply such approaches to large networks. Recently, some heuristic procedures, based on graph and network theory, have shown that it is possible to automatically identify optimal solutions in terms of number, shape and dimension of DMAs. In this paper, weighted spectral clustering methods have been used to define the optimal layout of districts in a real water distribution system, taking into account both geometric and hydraulic features, through weighted adjacency matrices. The obtained results confirm the feasibility of the use of spectral clustering to address the arduous problem of water supply network partitioning with an elegant mathematical approach compared to other heuristic procedures proposed in the literature. A comparison between different spectral clustering solutions has been carried out through topological and energy performance indices, in order to identify the optimal water network partitioning procedure.Entities:
Keywords: Laplacian spectrum; Spectral clustering; Water network partitioning; k-means
Year: 2017 PMID: 30443574 PMCID: PMC6214270 DOI: 10.1007/s41109-017-0033-4
Source DB: PubMed Journal: Appl Netw Sci ISSN: 2364-8228
Topological characteristics of the water distribution network of Parete
| m | n | q | K | APL | Dm | λ2 | Δλ |
|---|---|---|---|---|---|---|---|
| 282 | 184 | 0.017 | 3.05 | 8.80 | 20 | 0.021 | 0.062 |
Hydraulic characteristics of the water distribution network of Parete
| h* | hmin | hmean | hmax | PA |
|---|---|---|---|---|
| [m] | [m] | [m] | [m] | [kW] |
| 25.00 | 21.36 | 31.05 | 50.47 | 12122.11 |
h* = 25 m (the pressure head required to satisfy water demand at all nodes)
Fig. 1First 10-smallest eigenvalues of unweighted graph Laplacian matrix
Characteristics of the clusters obtained with the three tested algorithms and the five adopted pipe weights
| Laplacian Matrix | Weight | n° nodes DMA 1 | n° nodes DMA 2 | n° nodes DMA 3 | n° nodes DMA 4 | Ib | Nec |
|---|---|---|---|---|---|---|---|
| L | WA | 48 | 48 | 43 | 45 | 2.45 | 16 |
| WD | 53 | 46 | 43 | 42 | 4.97 | 17 | |
| W1/L | 59 | 56 | 40 | 29 | 14.07 | 20 | |
| WC | 84 | 65 | 19 | 16 | 33.83 | 26 | |
| WF | 76 | 64 | 42 | 2 | 32.54 | 15 | |
| Lrw | WA | 48 | 48 | 45 | 43 | 2.45 | 16 |
| WD | 49 | 47 | 45 | 43 | 2.58 | 17 | |
| W1/L | 54 | 45 | 44 | 41 | 5.60 | 19 | |
| WC | 82 | 40 | 33 | 29 | 24.43 | 21 | |
| WF | 78 | 43 | 36 | 27 | 22.32 | 24 | |
| Lsym | WA | 48 | 48 | 45 | 43 | 2.45 | 16 |
| WD | 49 | 47 | 45 | 43 | 2.58 | 17 | |
| W1/L | 55 | 47 | 42 | 40 | 6.68 | 19 | |
| WC | 126 | 32 | 15 | 11 | 54.10 | - | |
| WF | 86 | 46 | 28 | 24 | 28.33 | - |
Fig. 2Node coordinates in the eigenspace of the first 3-smallest eigenvectors of the diameter-weighted graph L Laplacian matrix
Characteristics of the edge-cut set obtained with the three tested algorithms and the five assumed pipe weights
| Laplacian Matrix | Weight | Nec | Multiplicity of pipe diameters D [mm] | ||||||
|---|---|---|---|---|---|---|---|---|---|
| 60 | 80 | 100 | 110 | 125 | 150 | 200 | |||
| L | WA | 16 | 5 | 1 | 4 | 1 | 1 | 2 | 2 |
| WD | 17 | 6 | 1 | 4 | 1 | 1 | 2 | 2 | |
| W1/L | 20 | 5 | 1 | 3 | 0 | 1 | 3 | 7 | |
| WC | 26 | 20 | 0 | 2 | 1 | 1 | 1 | 1 | |
| WF | 15 | 4 | 2 | 4 | 0 | 1 | 1 | 3 | |
| Lrw | WA | 16 | 5 | 1 | 4 | 1 | 1 | 2 | 2 |
| WD | 17 | 6 | 1 | 4 | 1 | 1 | 2 | 2 | |
| W1/L | 19 | 7 | 1 | 3 | 1 | 1 | 2 | 4 | |
| WC | 21 | 10 | 3 | 3 | 1 | 1 | 3 | 0 | |
| WF | 24 | 10 | 1 | 4 | 1 | 1 | 2 | 6 | |
| Lsym | WA | 16 | 5 | 1 | 4 | 1 | 1 | 2 | 2 |
| WD | 17 | 6 | 1 | 4 | 1 | 1 | 2 | 2 | |
| W1/L | 19 | 6 | 1 | 4 | 1 | 1 | 2 | 4 | |
| WC | - | - | - | - | - | - | - | - | |
| WF | - | - | - | - | - | - | - | - | |
Hydraulic performance indices after the dividing phase for the three tested algorithms and the five adopted pipe weights
| Laplacian Matrix | Weight | Nec | Nbv | Nfm | PD | PN | hmin | hmean | hmax |
|---|---|---|---|---|---|---|---|---|---|
| [-] | [-] | [-] | [kW] | [kW] | [m] | [m] | [m] | ||
| L | WA | 16 | 11 | 5 | 1831.64 | 10290.47 | 22.78 | 30.46 | 50.07 |
| WD | 17 | 12 | 5 | 1875.29 | 10246.82 | 22.09 | 29.82 | 50.16 | |
| W1/L | 20 | 15 | 5 | 1890.23 | 10231.88 | 22.23 | 29.93 | 49.87 | |
| WC | 26 | 21 | 5 | 1954.84 | 10167.27 | 14.04 | 28.68 | 50.03 | |
| WF | 15 | 10 | 5 | 1716.15 | 10405.96 | 21.58 | 30.99 | 50.41 | |
| Lrw | WA | 16 | 11 | 5 | 1831.64 | 10290.47 | 22.78 | 30.46 | 50.07 |
| WD | 17 | 12 | 5 | 1875.29 | 10246.82 | 22.09 | 29.82 | 50.16 | |
| W1/L | 19 | 14 | 5 | 1863.96 | 10258.15 | 22.49 | 30.24 | 49.98 | |
| WC | 21 | 16 | 5 | 1895.35 | 10226.76 | 20.81 | 29.13 | 50.61 | |
| WF | 24 | 19 | 5 | 1720.86 | 10401.25 | 20.79 | 30.81 | 50.50 | |
| Lsym | WA | 16 | 11 | 5 | 1831.64 | 10290.47 | 22.78 | 30.46 | 50.07 |
| WD | 17 | 12 | 5 | 1875.29 | 10246.82 | 22.09 | 29.82 | 50.16 | |
| W1/L | 19 | 14 | 5 | 1877.49 | 10244.62 | 22.36 | 30.09 | 50.11 | |
| WC | - | - | - | - | - | - | - | - | |
| WF | - | - | - | - | - | - | - | - |
Fig. 3Parete WSN partitioning in 4-DMA for the unweighted graph adjacency matrix: clustering phase (a) and dividing phase (b)
Fig. 4Parete WSN partitioning in 4-DMA for the conductance-weighted graph adjacency matrix and L Laplacian: clustering phase (a) and dividing phase (b). Flow meters are represented by rectangles while gate valves with the double triangle