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Proceeding Paper

Artificial Neural Network for Daily Low Stream Flow Rate Prediction of Perigiali Stream, Kavala City, NE Greece †

by
Thomas Papalaskaris
1,* and
Theologos Panagiotidis
2
1
Department of Civil Engineering, Democritus University of Thrace, Kimmeria Campus, 67100 Xanthi, Greece
2
Department of Mechanical Engineering, Eastern Macedonia & Thrace Institute of Technology, 65404 Kavala, Greece
*
Author to whom correspondence should be addressed.
Presented at the 3rd EWaS International Conference on “Insights on the Water-Energy-Food Nexus”, Lefkada Island, Greece, 27–30 June 2018.
Proceedings 2018, 2(11), 578; https://doi.org/10.3390/proceedings2110578
Published: 20 August 2018
(This article belongs to the Proceedings of EWaS3 2018)

Abstract

:
Only a few scientific research studies with reference to extremely low stream flow conditions, have been conducted in Greece, so far. Forecasting future low stream flow rate values is a crucial and desicive task when conducting drought and watershed management plans, designing water reservoirs and general hydraulic works capacity, calculating hydrological and drought low flow indices, separating groundwater base flow and storm flow of storm hydrographs etc. Artificial Neural Network modeling simulation method generates artificial time series of simulated values of a random (hydrological in this specific case) variable. The present study produces artificial low stream flow time series of both a part of the past year (2016) as well as the present year (2017) considering the stream flow data observed during two different respecting interval period of the years 2016 and 2017. We compiled an Artificial Neural Network to simulate low stream flow rate data, acquired at a certain location of the partly regulated semi-urban stream which runs through the eastern exit of Kavala city, NE Greece, using a 3-inches U.S.G.S. modified portable Parshall flume, a 3-inches conventional portable Parshall flume, a 3-inches portable Montana (short Parshall) flume and a 90° V-notched triangular shaped sharp crested portable weir plate. The observed data were plotted against the predicted one and the results were demonstrated through interactive tables providing us the ability to effectively evaluate the ANN model simulation procedure performance. Finally, we plot the recorded against the simulated low stream flow rate data, compiling a log-log scale chart which provides a better visualization of the discrepancy ratio statistical performance metrics and calculate the derived model statistics featuring the comparison between the recorded and the forecasted low stream flow rate data.

1. Introduction

Low flow regimes in rivers and streams are of paramount importance to the ecological conditions of any land surface hydrological feature. Any shift in the flows pattern throughout any hydrological year, stemming, for instance, from either individual activities e.g., groundwater abstraction, precipitation shortage, riparian areas encroachment, stream channelizing due to urbanization etc., or a combination of them, may contribute to stream ecology changes that cannot be undone [1]. Low flow analysis and forecasting is also fundamental when building works along watercourses (e.g., dams, reservoirs, water deviation channels for irrigation purposes etc.) and for watercourse rehabilitation plans regarding which a knowledge of hydrological fluctuation is of fundamental importance in designing sustainable rehabilitation works.
Another type of low flow analysis, specifically probability distribution analysis, was performed in the past analyzing the observed data collected at the same gauging station between 14th of May 2016 and 31th of July 2016 revealing that Pearson type 6 (3P) demonstrated the highest final goodness of fit obtained score based, simultaneously, on all available (Anderson-Darling, Chi-Squared and Kolmogorov-Smirnov) goodness of fit criteria [2]. Furthermore, as far as the same gauging station, similar type of analysis was elaborated considering, this time, the observed data collected at the same gauging station both between 14th of May 2016 and 29th of August 2016 revealing that Wakeby type (5P) demonstrated the highest final goodness of fit obtained score based on the Kolmogorov-Smirnov goodness of fit criterion and employed to generate an artificial low flow time series for the same time interval [3,4].
Especially within the last decade, a great number of ANN models have been designed for stream flow and sediment transport rates simulation. In a scientific research article, an ANN model was employed to design a model for streamflow forecasting respecting San Juan River basin, Argentina, using meteorological data from Pachon meteorological station built at 1900 m of altitude and proved distinctively effective of fitting remarkably well the observed stream flow data [5]. In a scientific research article, an ANN model was developed and proved effective of simulating well the daily both high and low flows, in Mesochora catchment, (drained by the Acheloos River), central mountain region of Greece [6]. In another scientific research article, the performance of three different ANN Schemes (a–c) was tested in order to calculate bed load transport rate in gravel-bed rivers running within the Snake River Basin, USA [7]. In another scientific research article, an ANN model was developed and proved capable of stream flow modeling of Savitri catchment, India [8]. In another scientific research article, an ANN model was designed and performed adequately of stream flow modeling of Nestos River, NE Greece [9].
In the present scientific research study, ANNs have been employed to design a forecasting model for the daily low flows of Perigiali Stream (at the exit of the homonymous watershed), Kavala city, Eastern Macedonia & Thrace Prefecture, NE Greece. Their selection is founded on the fact that they perform remarkably well (together within other sectors of scientific interests) in the field of hydrology, although, in some occasions, there is not available adequate information respecting all the variables contributing to the watershed system driving forces.

2. Study Area

The stream flow rate gauging station established in Kavala city coastal area, is located at the north of the Aegean Sea, across the Thassos Island, and surrounded by the Lekani mountain series branches to the North and East and the Paggaion Mountain ramifications to the West, (established in the proximity of the city urban web center and at the eastern exit of the city as well), located at the specific co-ordinates 40°56′727″ N and 24°25′929″ E, Perigiali city area, and operated during specified time intervals, bridging a time interval period from 14 May 2016 to 7 October 2017, as illustrated in Figure 1. It should be noted that since it is located just a few decades of meters upstream the sea shore and simultaneously at the exit of the entire Perigiali area watershed, between the sea shore and the Old National Road connecting the eastern exit of the Kavala city to the Xanthi city, drained by the homonymous Perigiali area stream, the associated stream flow rate measurements provide profooundly valuable scientific information respecting the entire regime of the water resources, (incorporating headwaters and lower order streams to higher order streams and the main stream channel), of the Perigiali area watershed.

3. Materials and Methods

We considered the stream flow data observed during two different center interval period of the years 2016 and 2017, more precisely, during part of May (from the 14th of May 2016), June, July and part of August 2016 (until the 30th of August 2016), part of December 2016 (from the 24th of December 2016), part of January 2017 (until the 5th of January 2017) as well as part of May (from the 24th of May 2017), June, July, August, September and part of October 2017, until the 7th of October 2017, without filling the consecutive data gaps for the rest, ungauged gaps, of the years 2016 and 2017, (see supplementary materials).
The distinctively shallow waters, exacerbated by the extremely low water stream flow velocity occurring at the gauging station, make impossible to perform the area-velocity method in order to calculate the stream flow rate (discharge), using a current meter mounted on a wading rod, due to the fact that there isn’t adequate depth to submerge the current meter; Moreover, the pronounced low water stream flow velocity is not sufficient enough to trigger the operation of a current meter. Under those noticeable circumstances the only other remaining options, are the use of either a small-sized portable weir (all those its implementation brings difficulties due to the fact that weirs, in general, demand a relatively great head loss which is not available at areas in proximity to watersheds’ outlets, where, in most cases, the natural slope of the channel bed is extremely low if not zero) plate or/and a small-sized flume or/and a set of small-sized weir and flumes which, eventually, was our final selected option, more specifically, a “3-inch U.S.G.S. Modified Portable Parshall Flume”, “3-inch U.S.G.S. Conventional Portable Parshall Flume” and a “90° V-Notched Triangular-Shaped Sharp-Crested (Sharp-Edged) U.S.G.S. Portable Weir Plate” [10,11,12,13,14,15,16,17,18,19,20], made of sea plywood, covered with a sprayed thin smooth polyester coating, (identical to that usually the industry covers the outside surface of high-speed sea boats, in order to reduce the friction developing between the outside area of those sea boats and the sea water, thus securing that the friction developed between the bottom as well as the walls of the stream flow rate gauging apparatus is minimized/restricted to a minimum.
Meteorological data has been collected from Dexameni-Kavala city—Eastern Macedonia & Thrace Prefecture—Greece private meteorological station (located at 40°56′25″ N–E 24°24′01″ E, Altitude: 90 m).
Low stream flow rate values were forecasted employing MLFP that is an appropriate type of ANNs both for meteorological as well as for river stream flow rate predictions.

4. Results and Discussion

Employing MATLAB software, various different designs of MLFP were elaborated with different number of neurons within both the input as well as the hidden layers. The superb model for daily forecasting (in the present study, M13.10.1) is described within the first following subsection whilst the referenced statistical criteria are displayed within the second following one. The three important identification characteristics of the model are as following: the number of neurons in input (i), hidden (j) and output (k) layers respectively.

4.1. Structure of Artificial Neural Network (M13.10.1)

A custom neural network (abbreviated as M13.10.1) was employed in order to simulate all the 246 site-measured values of the observed stream flow rate, (as depicted within Table A1), with the following architecture: Network Type: Feed-forward back propagation, Training Function: TRAINGDX, Adaption Learning Function: LEARNGDM, Performance Function: MSE, Number of Layers: 2, Number of Neurons: 10, Transfer Function: LOGSIG. It should also be stressed that epochs was selected equal to 1000. The input data for 246 site measurements were arranged as a time series with length of 246 data.
The selected custom neural network’s architecture used for this simulation is depicted within Figure 2.
The input layer for this network consists of thirteen neurons representing total daily rainfall R, cumulative total daily rainfall RC, mean daily wind velocity UWave, maximum daily wind velocity UWmax, mean daily air temperature Tave, minimum daily air temperature Tmin, maximum daily air temperature Tmax, mean daily air humidity Have, minimum daily air humidity Hmin, maximum daily humidity Hmax, mean daily air pressure Pave, minimum daily air pressure Pmin and maximum daily pressure Pmax. For this network 10 neurons were selected for the hidden layer.
The validation performance of the ANN (M13.10.1) is illustrated within Figure 3.
The training regression performance of the ANN (M681) is illustrated within Figure 4.

4.2. Model Statistical Efficiency Criteria and Performance Metrics

The respective statistical criteria values concerning Perigiali Stream regarding the selected artificial neural network (M13.10.1) are depicted within Table 1 [21]. It is noted that the relative error value depicted within Table 1 represents the average value of the relative errors calculated for each pair of calculated and site measured low stream flow rate values.
The plot depicted within Figure 5 represents the discrepancy ratio concerning Perigiali Stream with reference to the selected artificial neural network, depicting graphically, more specifically, as far as the present study is concerned, the percentage of the computed low stream flow rate values lying between the double and the half of the corresponding recorded values. At this point, it should be noted that both coordinate axes are in logarithmic scale; therefore, the equations y = x, y = 0.5x and y = 2.0x are represented graphically by parallel straight lines [22].
In general, the obtained values of the statistical criteria RMSE, RE, EC for Perigiali Stream can be considered fairly satisfactory. Additionally, the degree of linear dependence between computed and observed low daily stream flow rate is very high.
The dates of all measurements as well as both the site measured as well as the calculated stream flow rates of Perigiali Stream are presented in Table A1.

5. Discussion-Conclusions-Further Research

Lots of models based on ANN procedure concept have been employed and proposed by researchers so far in order to model daily stream flow and sediment transport rate worldwide. In the present study, a custom neural network (abbreviated as M13.10.1) was employed in order to simulate all the 246 site-measured values of the observed low stream flow rate, (as depicted within Table A1), with the certain architecture, using as inputs several meteorological parameters, (exogenous variables of the runoff generating processes), prevailing around the study area, and turned out, among others, to be the most appropriate to simulate the recorded daily low stream flow rate data. The resulted statistical efficiency criteria proved a strong relationship between those meteorological parameters involved and the daily stream flow rate of Perigiali Stream, Kavala city, Greece, suggesting that that ANN modeling concept is able to efficiently simulate observed daily low stream flow rate data which is essential for water resources management at a watershed level in terms of drought forecasting and management, water reservoir and water deviation works design, agricultural schemes planning at a regional level, filling gaps within low stream flow rate time series, low-flow indices calculation for environmental purposes, model implementation in ungaged catchments in order to generate artificial low stream flow rate data etc. Furthermore, the fact that the observed data represents short time intervals instead of an adequately long continuous time series can be definitely considered as a limitation underlining the need of more collected low stream flow rate recorded data in order to prove that our model can be regarded as an undoubtedly reliable one. In future, provided that proper and adequate apparatus is available, we intend to monitor water quality parameters in order to perform statistical analysis and assessment [23,24] and apply stochastic models [25] to predict future respecting values which are essential towards the establishment of a holistic Perigiali watershed management scheme.

Supplementary Materials

The following are available online at https://www.youtube.com/watch?v=Wu8KBj3qqXg, Video S1: Watershed Stream Flow Measurement-Stream Perigiali-2016.06.18-Kavala City-Greece, https://www.youtube.com/watch?v=-HbPZLNGplY&feature=youtu.be, Video S2: Watershed Stream Flow Measurement-Stream Perigiali-2017.07.27(a)-Kavala City-Greece (08:16:49 a.m.).

Conflicts of Interest

The authors declare no conflict of interest.

Appendix A

The dates of all measurements as well as both the site measured as well as the calculated stream flow rates of Perigiali Stream are presented in Table A1.
Table A1. Stream flow rate measurements of Perigiali Stream.
Table A1. Stream flow rate measurements of Perigiali Stream.
No.DateStream Flow Rate (m3/s) Site-MeasuredStream Flow Rate (m3/s) Calculated (M13.10.1)
114-5-20160.43700.3151
215-5-20160.50800.5156
316-5-20160.40300.5368
417-5-20160.40300.3824
518-5-20160.47200.4206
619-5-20160.58300.3695
720-5-20160.50800.5401
821-5-20162.74602.7714
922-5-20161.01101.0422
1023-5-20160.83000.7277
1124-5-20160.87400.8777
1225-5-20160.66200.6884
1326-5-20160.66200.3522
1427-5-20160.37000.3328
1528-5-20160.24880.1621
1629-5-20160.37010.2290
1730-5-20160.27750.2464
1831-5-20160.33810.2399
191-6-20160.24880.1881
202-6-20160.17000.2775
213-6-20160.37010.4214
224-6-20160.54510.3349
235-6-20160.33810.2148
246-6-20160.54500.4573
257-6-20160.30720.3277
268-6-20160.19500.3244
279-6-20160.12380.5328
2810-6-20160.12380.2220
2911-6-20160.19500.1596
3012-6-20160.12380.2532
3113-6-20161.46501.4400
3214-6-20160.62200.5874
3315-6-20160.43710.6716
3416-6-20160.30720.3144
3517-6-20160.22130.2456
3618-6-20160.30720.1447
3719-6-20160.27750.0960
3820-6-20160.19500.1450
3921-6-20160.27750.1379
4022-6-20160.08320.1844
4123-6-20160.10280.0345
4224-6-20160.01150.0324
4325-6-20160.03440.1006
4426-6-20160.14620.0823
4527-6-20160.14620.2139
4628-6-20160.27750.3824
4729-6-20160.17000.2488
4830-6-20160.06520.1717
491-7-20160.17000.1751
502-7-20160.17000.1731
513-7-20160.37010.2599
524-7-20160.27750.1681
535-7-20160.27750.1840
546-7-20160.06520.1986
557-7-20160.22130.2425
568-7-20160.02180.2421
579-7-20160.08320.2085
5810-7-20160.10280.1696
5911-7-20160.10280.0924
6012-7-20160.10280.1883
6113-7-20160.04890.1802
6214-7-20160.12380.2023
6315-7-20160.06520.1956
6416-7-20160.22130.3563
6517-7-20160.14620.1511
6618-7-20160.03440.2032
6719-7-20160.19500.2087
6820-7-20160.10280.1845
6921-7-20160.03440.1792
7022-7-20160.33810.1551
7123-7-20160.22130.1385
7224-7-20160.19500.1859
7325-7-20160.12380.1675
7426-7-20160.03400.2132
7527-7-20160.10280.1404
7628-7-20160.04890.2120
7729-7-20160.08320.1716
7830-7-20160.12380.1539
7931-7-20160.37010.2470
801-8-20160.06520.1286
812-8-20160.19500.1875
823-8-20160.10280.2106
834-8-20160.14620.1703
845-8-20160.24880.1431
856-8-20160.33810.1404
867-8-20160.12380.1855
878-8-20160.19500.1470
889-8-20160.37010.3080
8910-8-20160.19500.0914
9011-8-20160.33810.1474
9112-8-20160.24880.1523
9213-8-20160.19500.1698
9314-8-20160.24880.1911
9415-8-20160.22190.2268
9516-8-20160.27750.2724
9617-8-20160.43710.3402
9718-8-20160.37010.3989
9819-8-20160.40310.3530
9920-8-20160.30720.3288
10021-8-20160.19500.1659
10122-8-20160.22130.1439
10223-8-20160.43710.1598
10324-8-20160.27750.1746
10425-8-20160.22130.1580
10526-8-20160.27750.3003
10627-8-20160.27750.4087
10728-8-20160.30720.2810
10829-8-20160.43710.1957
10930-8-20160.66160.1487
11024-5-20170.12100.0630
11125-5-20170.08200.2088
11226-5-20175.91505.8006
11327-5-20170.21300.3294
11428-5-20170.08200.0721
11529-5-20170.06500.1313
11630-5-20170.10100.0732
11731-5-20170.04900.0942
1181-6-20170.03400.0577
1192-6-20170.06500.0701
1203-6-20170.06500.0926
1214-6-20170.08200.1520
1225-6-20170.06500.1203
1236-6-20170.08200.1310
1247-6-20170.06500.0775
1258-6-20170.08200.0967
1269-6-20170.10100.2323
12710-6-20170.08200.0822
12811-6-20175.85605.7520
12912-6-20171.40100.1787
13013-6-20170.06500.1244
13114-6-20170.10100.0562
13215-6-20170.08200.0934
13316-6-20170.08200.1727
13417-6-20170.10100.0953
13518-6-20170.08200.2393
13619-6-20170.06500.1153
13720-6-20170.06500.2136
13821-6-20170.06500.0858
13922-6-20170.06500.1791
14023-6-20170.06500.0815
14124-6-20170.04900.0913
14225-6-20170.06500.0944
14326-6-20170.04900.1180
14427-6-20170.04900.1054
14528-6-20170.04900.0907
14629-6-20170.04900.0868
14730-6-20170.04900.0799
1481-7-20170.04900.0761
1492-7-20170.04900.0405
1503-7-20170.06450.0220
1514-7-20170.04860.0528
1525-7-20170.04860.0771
1536-7-20170.04860.1173
1547-7-20170.04860.0557
1558-7-20170.04860.0526
1569-7-20170.04860.0943
15710-7-20170.03440.0954
15811-7-20170.03440.1002
15912-7-20170.06450.1101
16013-7-20170.03440.0953
16114-7-20170.98720.0938
16215-7-20170.10070.1689
16316-7-20170.08190.0594
16417-7-20170.14210.1343
16518-7-20170.12080.0546
16619-7-20170.10070.1309
16720-7-20170.08190.1488
16821-7-20170.04860.1666
16922-7-20170.06450.0871
17023-7-20170.06450.0853
17124-7-20170.06450.0791
17225-7-20170.03440.0470
17326-7-20170.04860.0324
17427-7-20170.04860.1451
17528-7-20170.04860.0401
17629-7-20170.04860.0833
17730-7-20170.04860.0854
17831-7-20170.04860.0917
1791-8-20170.03440.1454
1802-8-20170.03440.1289
1813-8-20170.03440.0650
1824-8-20170.03440.0745
1835-8-20170.03440.0478
1846-8-20170.04860.0646
1857-8-20170.03440.0831
1868-8-20170.03440.0593
1879-8-20170.03440.0648
18810-8-20170.03440.0761
18911-8-20170.03440.0717
19012-8-20170.03440.0536
19113-8-20170.03440.0579
19214-8-20170.03440.0325
19315-8-20170.03440.0407
19416-8-20170.03440.0666
19517-8-20170.03440.0412
19618-8-20170.02210.0871
19719-8-20170.20600.0963
19820-8-20170.18900.0784
19921-8-20170.16700.0463
20022-8-20170.04860.1150
20123-8-20170.12100.0395
20224-8-20170.04860.0695
20325-8-20170.04860.0432
20426-8-20170.20700.0584
20527-8-20170.16900.0670
20628-8-20170.03440.0642
20729-8-20170.04860.0653
20830-8-20170.17700.1272
20931-8-20170.17100.0511
2101-9-20170.07300.0719
2112-9-20170.04700.0651
2123-9-20170.19300.0619
2134-9-20170.94390.0466
2145-9-20170.03440.0558
2156-9-20170.03600.0309
2167-9-20170.03200.0423
2178-9-20170.04300.1097
2189-9-20170.13900.1766
21910-9-20170.13700.1078
22011-9-20170.02200.0488
22112-9-20170.03440.0442
22213-9-20170.14500.0686
22314-9-20170.03440.1917
22415-9-20170.16100.1379
22516-9-20170.14900.0648
22617-9-20170.04860.0852
22718-9-20170.10800.0699
22819-9-20170.04860.0667
22920-9-20170.03440.0622
23021-9-20170.09900.0127
23122-9-20170.07140.0565
23223-9-20170.13800.0165
23324-9-20170.09960.0243
23425-9-20170.09340.1726
23526-9-20174.60034.6082
23627-9-20170.18700.0140
23728-9-20170.15100.0125
23829-9-20170.17900.0118
23930-9-20170.03300.0174
2401-10-20170.12800.1406
2412-10-20170.14200.0136
2423-10-20170.09100.0124
2434-10-20170.06500.0139
2445-10-20170.10500.0147
2456-10-20170.05900.0550
2467-10-20171.12451.1225

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Figure 1. Parshall flumes and V-Notched weir gauging station, Perigiali Stream area, Kavala city, Greece.
Figure 1. Parshall flumes and V-Notched weir gauging station, Perigiali Stream area, Kavala city, Greece.
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Figure 2. ANN (M13.10.1) architecture plot of Perigiali Stream.
Figure 2. ANN (M13.10.1) architecture plot of Perigiali Stream.
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Figure 3. ANN (M13.10.1) validation performance plot of Perigiali Stream.
Figure 3. ANN (M13.10.1) validation performance plot of Perigiali Stream.
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Figure 4. ANN (M13.10.1) training regression performance plots of Perigiali Stream.
Figure 4. ANN (M13.10.1) training regression performance plots of Perigiali Stream.
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Figure 5. Discrepancy ratio plot of Perigiali Stream (ANN M13.10.1).
Figure 5. Discrepancy ratio plot of Perigiali Stream (ANN M13.10.1).
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Table 1. Statistical criteria values of Perigiali Stream (ANN M13.10.1).
Table 1. Statistical criteria values of Perigiali Stream (ANN M13.10.1).
Number of Paired ValuesRMSE (ltrs/s)RE (%)ECrr2Discrepancy Ratio
2460.1479−0.40800.94680.97320.94720.6789
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Papalaskaris, T.; Panagiotidis, T. Artificial Neural Network for Daily Low Stream Flow Rate Prediction of Perigiali Stream, Kavala City, NE Greece. Proceedings 2018, 2, 578. https://doi.org/10.3390/proceedings2110578

AMA Style

Papalaskaris T, Panagiotidis T. Artificial Neural Network for Daily Low Stream Flow Rate Prediction of Perigiali Stream, Kavala City, NE Greece. Proceedings. 2018; 2(11):578. https://doi.org/10.3390/proceedings2110578

Chicago/Turabian Style

Papalaskaris, Thomas, and Theologos Panagiotidis. 2018. "Artificial Neural Network for Daily Low Stream Flow Rate Prediction of Perigiali Stream, Kavala City, NE Greece" Proceedings 2, no. 11: 578. https://doi.org/10.3390/proceedings2110578

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