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<strong>SCIENCE</strong> <strong>CITATION</strong> <strong>INDEX</strong> <strong>EXPANDED</strong> <strong>JOURNAL</strong> <strong>LIST</strong><br />

<strong>Search</strong> terms: 1432-7643<br />

Total journals found: 1<br />

1. SOFT COMPUTING<br />

Bimonthly<br />

ISSN: 1432-7643<br />

SPRINGER, 233 SPRING ST, NEW YORK, USA, NY, 10013<br />

1. Science Citation Index Expanded<br />

2. Current Contents - Engineering, Computing & Technology<br />

Abstracted/Indexed in:<br />

Compendex,<br />

Computer Science Index,<br />

Ei Page One,<br />

Inspec,<br />

Journal Citation Reports/Science Edition,<br />

Science Citation Index Expanded (Sci<strong>Search</strong>),<br />

SCOPUS,<br />

Zentralblatt Math


Soft Comput (2009) 13:701–707<br />

DOI 10.1007/s00500-008-0343-7<br />

ORIGINAL PAPER<br />

Predicting flow conditions over stepped chutes based on ANFIS<br />

Davut Hanbay · Ahmet Baylar · Emrah Ozpolat<br />

Published online: 15 July 2008<br />

© Springer-Verlag 2008<br />

Abstract Chute flow may be either smooth or stepped. The<br />

flow conditions in stepped chutes have been classified into<br />

nappe, transition and skimming flows. In this paper, characteristics<br />

of flow conditions are presented systematically<br />

under a wide range of critical flow depth, step height and<br />

chute slope. The Adaptive Network Based Fuzzy Inference<br />

System (ANFIS) is used to predict flow conditions in stepped<br />

chutes using critical flow depth, step height and chute slope<br />

information. The proposed model performance is determined<br />

by threefold cross validation method. The evaluated classification<br />

accuracy of ANFIS model is 99.01%. The test results<br />

showed that the proposed ANFIS model can be used successfully<br />

for complex process control in hydraulic systems.<br />

Keywords ANFIS · Fuzzy membership function · Stepped<br />

chute · Flow conditions · Cross validation<br />

1 Introduction<br />

In a stepped chute, the chute face is provided with a series of<br />

steps, from near the crest to the toe. The provision of steps<br />

can produce significant energy dissipation. Stepped chutes<br />

are commonly used for gabion weirs, river training, irrigation<br />

channels, and storm waterways. Stepped chutes are used<br />

also for in-stream re-aeration and in water treatment plants<br />

to enhance the air–water transfer of atmospheric gases (e.g.<br />

oxygen, nitrogen) and of volatile organic components.<br />

D. Hanbay<br />

Electronic and Computer Science Department, Firat University,<br />

Elazig, Turkey<br />

A. Baylar (B) · E. Ozpolat<br />

Civil Engineering Department, Firat University, Elazig, Turkey<br />

e-mail: abaylar@firat.edu.tr<br />

Three distinct flow conditions are found on stepped chutes,<br />

so-called nappe flow, transition flow, and skimming flow<br />

(Fig. 1). Rajaratnam (1990), Chamani and Rajaratnam (1994),<br />

Chamani and Rajaratnam (1999a), Chamani and Rajaratnam<br />

(1999b), Chanson (1994a,b, 1996) and Hewlett et al. (1997)<br />

have focused mainly on the hydraulic design of stepped chute,<br />

and in particular, characteristics of nappe flow, transition<br />

flow, and skimming flow over stepped chutes. Recently,<br />

Baylar and Emiroglu (2003), Emiroglu and Baylar (2003,<br />

2006) and Baylar et al. (2006, 2007a,b,c) did some detailed<br />

experiments on the aeration efficiency of stepped chutes.<br />

In recent years the developments in intelligent methods<br />

make them possible to use in complex systems modeling.<br />

One of these intelligent methods is artificial neural network.<br />

Artificial neural network performance depends on the size<br />

and quality of training samples. When the number of training<br />

data is small, not representative of the possibility space,<br />

standard neural network results are poor. The other intelligent<br />

method is fuzzy theory, which has been used successfully in<br />

many applications (Frayman and Wang 1998; Kecman 2001;<br />

Held et al. 2006; Wang and Fu 2005; Hanbay et al. 2006a,b).<br />

Fuzzy methods provide linguistic labels for complex system<br />

modeling. There are many advantages of fuzziness, one of<br />

which is the ability to handle blur data. Both artificial neural<br />

network and fuzzy logic advantages are used in ANFIS’s<br />

architecture. ANFIS uses a hybrid learning algorithm to identify<br />

parameters of Sugeno-type fuzzy inference systems. It<br />

applies a combination of the least-squares method and the<br />

backpropagation gradient descent method for training membership<br />

function parameters to emulate a given training data<br />

set.<br />

ANFIS is widely used in complex system studies for<br />

modeling, control or parameter estimating. However, its<br />

application to the hydraulic systems related studies are very<br />

limited (Hanbay et al. 2007). In this study, the flow conditions<br />

123


702 D. Hanbay et al.<br />

Fig. 1 Flow conditions on a stepped chute. a Skimming flow, b transition<br />

flow, c nappe flow<br />

in stepped chutes are predicted based on the ANFIS. The<br />

paper is organized as follows. In Sect. 2, wereviewsome<br />

basic properties of stepped chute flow and the ANFIS. In<br />

Sect. 3, experimental data are given and the effectiveness<br />

of the proposed structure is demonstrated. Finally, Sect. 4<br />

presents conclusion.<br />

2 Preliminaries<br />

The theoretical foundations of the presented study are given<br />

in the following subsections.<br />

2.1 Flow conditions over stepped chutes<br />

2.1.1 Skimming flow condition<br />

For large discharges, the waters flow down a stepped chute<br />

as a coherent stream “skimming” over the steps. The external<br />

edges of the steps form a pseudo-bottom over which<br />

the flow skims. Beneath the pseudo-bottom, recirculating<br />

vortices develop and recirculation is maintained through the<br />

transmission of shear stress from the main stream (Fig. 1a).<br />

Small-scale vorticity is also generated at the corner of the<br />

steps. The aerated flow region follows a region where the<br />

free-surface is smooth and glassy. Next to the boundary however,<br />

turbulence is generated and the boundary layer grows<br />

until the outer edge of the boundary layer reaches the surface.<br />

When the outer edge of the boundary layer reaches the<br />

free surface, the turbulence can initiate natural free surface<br />

aeration. The location of the start of air entrainment is called<br />

the point of inception. Downstream of the inception point of<br />

123<br />

free-surface aeration, the flow becomes rapidly aerated and<br />

the free-surface appears white. Air and water are fully mixed<br />

forming a homogeneous two-phase flow (Chanson 2002).<br />

2.1.2 Transition flow condition<br />

Ohtsu and Yasuda (1997) were probably the first to introduce<br />

the concept of a “transition flow” condition, although they<br />

did not elaborate on its flow properties. For a given stepped<br />

chute geometry, a range of flow rates gives an intermediary<br />

flow condition between nappe flows at low discharges and<br />

skimming flows at large flow rates. In the transition flow<br />

condition, air bubble entrainment takes place along the jet<br />

upper nappe and in the spray region downstream of the stagnation<br />

point. The flow highly turbulent, air and water are<br />

continuously mixed (Fig. 1b). The air entrainment process in<br />

transition flow is not yet fully understood (Chanson 2002).<br />

2.1.3 Nappe flow condition<br />

For a given flat step geometry, low flows behave as a series<br />

of free-falling jets with nappe impact onto the downstream<br />

step: i.e. nappe flow condition. At the upstream end of each<br />

step, the flow is characterized by a free-falling nappe, an air<br />

cavity and a pool of recirculating fluid (Fig. 1c). In a nappe<br />

flow, air is entrained at the jet interfaces and by a plunging<br />

jet mechanism at the intersection of the lower nappe with<br />

the recirculating pool, while de-aeration is often observed<br />

downstream. In the free-falling nappe, interfacial aeration<br />

takes place at both the upper and lower nappes. At the lower<br />

nappe, the developing shear layer is characterized by a high<br />

level of turbulence and significant interfacial air entrainment<br />

is observed (Chanson 2002).<br />

2.2 Adaptive network based fuzzy inference system<br />

(ANFIS)<br />

The architecture and learning rule of ANFIS have been<br />

described in detail in (Jang 1993). ANFIS is a multilayer<br />

feed forward network where each node performs a particular<br />

function on incoming signals. Both square and circle<br />

node symbols are used to represents different properties of<br />

adaptive learning. To perform desired input-output characteristics,<br />

adaptive learning parameters are updated based on<br />

gradient learning rules (Jang 1993). ANFIS model is one of<br />

the implementation of a first order Sugeno fuzzy inference<br />

system (Kulkarni 2001). The rules are of the form in Eq. (1).<br />

In this system<br />

If x1 is A1, x2 is A2, then y = px1 + qx2 + r (1)<br />

where x1 and x2 inputs A1 and A2 corresponding term set,<br />

y is output, p, q, r are constant. An ANFIS model is shown<br />

in Fig. 2. It is a multi-input, one-output model; a multi-output


Predicting flow conditions over stepped chutes based on ANFIS 703<br />

X1<br />

X 2<br />

L1<br />

A1<br />

A2<br />

A3<br />

B1<br />

B2<br />

B3<br />

L2<br />

π<br />

π<br />

π<br />

W1<br />

W n<br />

Fig. 2 ANFIS model structure<br />

L3<br />

N<br />

N<br />

N<br />

W11<br />

W 1n<br />

model can be designed by connecting few single output<br />

models. The node functions in the same layer are similar<br />

and described as below<br />

Layer-1 Every node i in this layer is a square node with<br />

a node function. Nodes in layer 1 implement fuzzy membership<br />

functions, mapping input variables to corresponding<br />

fuzzy membership values. Outputs of this layer can be<br />

described as Eq. (2)<br />

O 1<br />

i<br />

= µAi (x) (2)<br />

where x is input to node i, and Aiis linguistic label associated<br />

with this node function. O1 i is the membership function of<br />

Ai, the fuzzy membership functions can take any form, such<br />

as triangular, Gaussian but usually µAi (x) is chosen bellshaped<br />

with maximum equal to 1 and minimum equal to 0.<br />

Detail information on the types of membership functions was<br />

described by Bhattacharya and Vasant (2007), Vasant and<br />

Bhattacharya (2007), Vasant et al. (2007) and Bhattacharya<br />

et al. (2008).<br />

Layer-2 Every node in this layer is a circle node labeled <br />

which multiplies the incoming signals and sends the product<br />

out. For instance,<br />

wi = µA1 (x)µA2 (y)... i = 1, 2, 3,...,N (3)<br />

Each node output represents the firing strength of a rule.<br />

Layer-3 Every node in this layer is a circle node labeled<br />

N. Theith node calculates the ratio of the ith rules firing<br />

strength to the sum of all rule’s firing strengths. Where ¯w is<br />

the normalized firing strength of rules.<br />

¯w =<br />

wi<br />

w1 + w2 ···wN<br />

L4<br />

L5<br />

i = 1, 2, 3,...,N (4)<br />

Layer-4 Every nodei in this layer is a square node with a<br />

node function,<br />

O 4 i = ¯wi fi = ¯wi(px + qy + ...+ r)<br />

i = 1, 2, 3,...,N (5)<br />

Σ<br />

Y<br />

where ¯wi is the output of layer 3 and {p, q, r} is the parameter<br />

set. Parameters in this layer will be referred to as consequent<br />

parameters.<br />

Layer-5 The single node in this layer is a circle node<br />

labeled that computes the overall output of ANFIS as the<br />

summation of all incoming signals.<br />

<br />

wi fi<br />

<br />

i<br />

= overall output = ¯wi fi = <br />

(6)<br />

O 5 i<br />

3 Application<br />

3.1 Experiments<br />

i<br />

The data used in this study were taken from studies conducted<br />

by Baylar and Emiroglu (2003) and Baylar et al. (2006)ona<br />

large model of a stepped chute. A schematic representation<br />

of the experimental set-up is shown on Fig. 3 that shows a<br />

prismatic rectangular chute, 0.30 m wide and 0.50 m deep,<br />

in which the steps were installed. The side walls were made<br />

of transparent methacrylate to follow flow condition. Water<br />

was pumped from the storage tank to stilling tank, from which<br />

water entered the chute through an approach channel, with<br />

its bed 1.25 and 2.50 m above the laboratory floor. Downstream<br />

channel used in this study was 3.0 m long, 0.35 m<br />

wide and 0.45 m deep. The experiments reported here were<br />

carried out, with unit discharges ranging between 16.67 ×<br />

10 −3 and 166.67 × 10 −3 m 2 /s. The discharge was measured<br />

by means of a flow meter installed in the supply line. Chute<br />

slopes were equal to 14.48 ◦ , 18.74 ◦ , 22.55 ◦ ,30 ◦ ,40 ◦ , and<br />

50 ◦ and for all slopes tested, steps with h equal to 5, 10, and<br />

15 cm were used.<br />

3.2 Experimental results<br />

The experimental results indicated that the type of flow condition<br />

is a function of the flow rate, step height and chute slope.<br />

Three different flow conditions, namely the nappe, transition<br />

and skimming flow conditions occur on stepped chutes.<br />

A tendency towards the nappe flow condition is observed<br />

with increasing step height and decreasing unit discharge<br />

and chute slope. However, the results show a tendency<br />

towards the transition and skimming flow conditions as<br />

unit discharge and chute slope increase and as step height<br />

decreases. Figure 4 shows classification of flow conditions<br />

on stepped chutes.<br />

3.3 ANFIS modeling results<br />

All program code was written in MATLAB. The parameters<br />

considered in the study are the ratio between the critical<br />

i<br />

wi<br />

123


704 D. Hanbay et al.<br />

Fig. 3 Laboratory stepped<br />

chute apparatus<br />

hc/ h<br />

3.0<br />

2.5<br />

2.0<br />

1.5<br />

1.0<br />

0.5<br />

0.0<br />

0<br />

Skimming<br />

flow<br />

Transition<br />

flow<br />

Nappe<br />

flow<br />

10<br />

20<br />

30<br />

Tank<br />

α (degrees)<br />

40<br />

Water<br />

pump<br />

Water<br />

flowmeter<br />

Fig. 4 Flow conditions on stepped chutes (Baylar et al. 2006)<br />

flow depth and step height (hc/h), chute slope (α) and flow<br />

condition. The parameters (hc/h) and α are used as inputs to<br />

the ANFIS for the prediction of flow condition. Three flow<br />

conditions, nappe, transition and skimming, are denoted as<br />

the numbers 1, 2 and 3, respectively. Total 126 experimental<br />

data sets were used in this study. Threefold cross validation<br />

method was used for proposed model validation. The training<br />

performance of ANFIS model is shown in Fig. 5. InFig.5<br />

error is the array of root mean square training errors.<br />

The test results are represented in Table 1 and graphically<br />

showed in Fig. 6. In the fourth column of Table 1, the numbers<br />

1, 2 and 3 indicate the flow conditions, nappe, transition<br />

and skimming, respectively. In the fifth column, the ANFIS<br />

predictions are presented. In the sixth column, the classifica-<br />

123<br />

50<br />

Water feed line<br />

Flow<br />

control valve<br />

60<br />

Error<br />

0.194<br />

0.192<br />

0.190<br />

0.188<br />

0.186<br />

0.184<br />

0.182<br />

Grid<br />

Upstream<br />

channel<br />

Stilling<br />

tank<br />

Stepped chute<br />

α<br />

Downstream<br />

channel<br />

0.180<br />

0 20 40 60<br />

Epochs<br />

80 100<br />

Fig. 5 Training performance of ANFIS model<br />

tion result of ANFIS model is presented. It can be obviously<br />

seen from Table 1 that the ANFIS predicts observed flow<br />

conditions at high accuracy. The correct classification<br />

success rate was found as 99.01%.<br />

The ANFIS structure is described in Table 2 for gbellmf<br />

membership function. Different types of membership functions<br />

were used. The best performance is obtained with<br />

gbellmf as seen from Table 3. Each input has three membership<br />

function. The training epoch for all membership is<br />

100.<br />

4 Conclusions<br />

Stepped chute flows are characterized by a high level of turbulence<br />

and large amounts of entrained air. The mechanisms<br />

by which air is entrained into water because of a stepped chute<br />

are several and complex. Basic air entrainment mechanisms<br />

occur in nappe, transition and skimming flow conditions. For<br />

the hydraulic design of a stepped channel, it is important to


Predicting flow conditions over stepped chutes based on ANFIS 705<br />

Table 1 The test data and ANFIS outputs for predicted flow condition<br />

hc/h α Flow condition Flow condition Flow condition Flow condition Prediction<br />

(deg.) observed observed predicted by ANFIS classified by ANFIS error (%)<br />

0.960 14.48 Transition 2 2.2585 2 12.9250<br />

2.020 14.48 Skimming 3 2.9928 3 0.2400<br />

0.600 18.74 Nappe 1 1.0670 1 6.7000<br />

1.540 18.74 Skimming 3 3.0122 3 0.4067<br />

2.820 18.74 Skimming 3 3.1594 3 5.3133<br />

1.260 22.55 Skimming 3 2.8854 3 3.8200<br />

2.440 22.55 Skimming 3 2.9654 3 1.1533<br />

0.960 30.00 Skimming 3 2.8511 3 4.9633<br />

2.020 30.00 Skimming 3 3.0531 3 1.7700<br />

0.600 40.00 Transition 2 1.4657 1 46.5700<br />

1.540 40.00 Skimming 3 3.0196 3 0.6533<br />

2.820 40.00 Skimming 3 2.9737 3 0.8767<br />

1.260 50.00 Skimming 3 3.0539 3 1.7967<br />

2.440 50.00 Skimming 3 2.9654 3 1.1533<br />

0.480 14.48 Nappe 1 1.0142 1 1.4200<br />

1.010 14.48 Transition 2 2.4281 2 21.4050<br />

0.300 18.74 Nappe 1 0.9513 1 4.8700<br />

0.770 18.74 Transition 2 1.4971 1 49.7100<br />

1.410 18.74 Skimming 3 2.9742 3 0.8600<br />

0.630 22.55 Nappe 1 1.1473 1 14.7300<br />

1.220 22.55 Skimming 3 2.8626 3 4.5800<br />

0.480 30.00 Nappe 1 0.9100 1 9.0000<br />

1.010 30.00 Skimming 3 2.9849 3 0.5033<br />

0.300 40.00 Nappe 1 1.0433 1 4.3300<br />

0.770 40.00 Transition 2 2.1442 2 7.2100<br />

1.410 40.00 Skimming 3 2.9828 3 0.5733<br />

0.630 50.00 Transition 2 2.0776 2 3.8800<br />

1.220 50.00 Skimming 3 3.0504 3 1.6800<br />

0.320 14.48 Nappe 1 0.9874 1 1.2600<br />

0.673 14.48 Nappe 1 1.2924 1 29.2400<br />

0.200 18.74 Nappe 1 1.0168 1 1.6800<br />

0.513 18.74 Nappe 1 0.9667 1 3.3300<br />

0.940 18.74 Transition 2 2.1103 2 5.5150<br />

0.420 22.55 Nappe 1 0.9218 1 7.8200<br />

0.813 22.55 Transition 2 1.8099 2 9.5050<br />

0.320 30.00 Nappe 1 0.9260 1 7.4000<br />

0.673 30.00 Nappe 1 1.3815 1 38.1500<br />

0.200 40.00 Nappe 1 0.9901 1 0.9900<br />

0.513 40.00 Nappe 1 1.2656 1 26.5600<br />

0.940 40.00 Skimming 3 2.8379 3 5.4033<br />

0.420 50.00 Nappe 1 1.4913 1 49.1300<br />

0.813 50.00 Skimming 3 2.5796 3 14.0133<br />

predict flow conditions. In this study, an ANFIS model was<br />

used in prediction of flow condition over stepped chutes. The<br />

most important aspect of the intelligent model is the ability<br />

of self-organization of the ANFIS without requirements of<br />

programming and the immediate response of a trained net<br />

during real-time applications. These features make the<br />

123


706 D. Hanbay et al.<br />

Flow regime<br />

3.5<br />

3<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

Measured Data<br />

ANFIS Output<br />

0 10 20 30 40 50<br />

Samples<br />

Fig. 6 Test performance of ANFIS model (The membership function<br />

number is 3 for each input)<br />

Table 2 The ANFIS structure for (gbellmf)<br />

Number of nodes 35<br />

Number of linear parameters 27<br />

Number of nonlinear parameters 18<br />

Total number of parameters 45<br />

Number of training data pairs 84<br />

Number of checking data pairs 42<br />

Number of fuzzy rules 9<br />

Table 3 The performance of different type membership functions<br />

Membership Classification accuracy (%) Average<br />

functions classification<br />

Test dataset-1 Test dataset-2 Test dataset-3 accuracy (%)<br />

Dsigmf 98.84 99.08 98.68 98.8667<br />

Gauss2mf 98.99 98.82 98.87 98.8933<br />

Gbellmf 98.97 99.16 98.91 99.0133<br />

Pimf 98.90 98.05 98.05 98.3333<br />

Psigmf 98.83 99.08 98.68 98.8633<br />

Trapmf 98.81 98.94 97.75 98.5000<br />

Trimf 98.63 99.07 99.03 98.9100<br />

intelligent model suitable for complex systems modeling.<br />

The modeling performance of this study shows the advantages<br />

of intelligent modeling. It is rapid and easy to operate.<br />

This model offers advantage in commercial application.<br />

Although our intelligent model was carried out on the hydraulic<br />

systems, similar results for the biomedical, biological and<br />

industrial systems can be expected.<br />

123<br />

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