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SCIENCE CITATION INDEX EXPANDED JOURNAL LIST<br />

Search terms: 1863-0650<br />

Total journals found: 1<br />

<strong>1.</strong> <strong>CLEAN</strong>-<strong>SOIL</strong> <strong>AIR</strong> <strong>WATER</strong><br />

<strong>Bimonthly</strong><br />

ISSN: 1863-0650<br />

WILEY-V C H VERLAG GMBH, PO BOX 10 11 61, WEINHEIM, GERMANY, D-69451<br />

<strong>1.</strong> Science Citation Index Expanded<br />

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Abstracting and Indexing Information<br />

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ISI)<br />

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Web of Science® (Thomson ISI)<br />

Zoological Record (Thomson ISI)


186 Clean 2007, 35 (2), 186 – 192<br />

Ahmet Baylar 1<br />

Davut Hanbay 2<br />

Emrah Ozpolat 1<br />

1 Firat University, Civil Engineering<br />

Department, Elazig, Turkey.<br />

2 Firat University, Electronic and<br />

Computer Science Department, Elazig,<br />

Turkey.<br />

1 Introduction<br />

Research Article<br />

Stepped cascade flows are characterized by the strong turbulent<br />

mixing, the large residence time, and the substantial air bubble<br />

entrainment. Stepped flows can be classified into skimming flow,<br />

transition flow, and nappe flow. For narrow steps or larger discharges<br />

such as the design discharge the water skims over the step<br />

corners and recirculating zones develop in triangular niches<br />

formed by the step faces and the pseudo-bottom, as shown in Fig. 1a.<br />

In skimming flow the water flows as a coherent stream over the<br />

pseudo-bottom formed by the step corners. For a range of intermediate<br />

discharges, a transition flow regime takes place. The dominant<br />

feature is stagnation on the horizontal step face associated with significant<br />

splashing and a chaotic appearance (see Fig. 1b). For nappe<br />

flow the steps act as a series of overfalls with the water plunging<br />

from one step to another (see Fig. 1c). Generally speaking, the nappe<br />

flow is found for low discharges and wide steps [1].<br />

Self-aeration on stepped cascades is now recognized for its substantial<br />

contribution to the air-water transfer of atmospheric gases<br />

such as oxygen and nitrogen. Stepped cascades are very efficient<br />

means of aeration because of the strong turbulent mixing, the large<br />

residence time, and the substantial air bubble entrainment.<br />

Stepped cascades are used in water treatment for re-oxygenation,<br />

denitrification, or VOC removals. In the treatment of drinking<br />

water, cascade aeration may be used to remove chlorine and to eliminate<br />

or reduce offensive taste and odor [2].<br />

Chanson and Toombes [3] conducted gas-liquid interface measurements<br />

in a stepped cascade. Local void fractions, bubble count<br />

rates, bubble size distributions, and gas-liquid interface areas were<br />

measured simultaneously in the air-water flow region using resistivity<br />

probes. However, they stated that future work is needed to compare<br />

aeration efficiencies estimated with detailed interfacial area<br />

data and based upon dissolved gas measurements. Recently, Baylar<br />

Correspondence: Prof. A. Baylar (abaylar@firat.edu.tr), Firat University,<br />

Civil Engineering Department, Elazig, Turkey.<br />

Modeling Aeration Efficiency of Stepped Cascades<br />

by Using ANFIS<br />

The physical process of oxygen transfer or oxygen absorption from the atmosphere<br />

acts to replenish the used oxygen, a process termed re-aeration or aeration. Aeration<br />

enhancement by macro-roughness is well-known in water treatment and one form is<br />

the aeration cascade. The macro-roughness of the steps significantly reduces the flow<br />

velocities and leads to flow aeration along the stepped cascade. In this paper, the aeration<br />

efficiency in stepped cascade aerators was modeled by using the Adaptive Network<br />

Based Fuzzy Inference System (ANFIS). The obtained model was tested with experimental<br />

data. Test results showed that ANFIS can be used to estimate the aeration<br />

efficiency in stepped cascade aerators.<br />

Keywords: ANFIS; Aeration efficiency; Modeling; Oxygen transfer;<br />

Received: February 14, 2007; revised: March 9, 2007; accepted: March 12, 2007<br />

DOI: 10.1002/clen.200700019<br />

Figure <strong>1.</strong> Flow regimes above stepped cascades: a) Skimming flow; b)<br />

Transition flow; c) Nappe flow [22].<br />

and Emiroglu [4], Emiroglu and Baylar [5], Baylar et al. [6], Emiroglu<br />

and Baylar [7], and Baylar et al. [8 – 10] did some detailed experiments<br />

on the aeration efficiency of stepped cascades. It was found<br />

that water can trap a lot of air when passing through the steps and<br />

that the oxygen content in the water body is increased. So stepped<br />

cascades can be used as highly effective aerators in streams, rivers,<br />

constructed channels, fish hatcheries, water treatment plants, etc.<br />

Intelligent techniques are used in various areas of water-related<br />

research [11 – 14]. Recently, Hanbay et al. [15,16] modeled the aeration<br />

efficiency of weirs by using the Adaptive Network Based Fuzzy<br />

Inference System (ANFIS) and by using wavelet and neural network.<br />

In this study, the aeration efficiency in stepped cascade aerators is<br />

modeled by using ANFIS. After reviewing some basic properties of<br />

i 2007 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim www.clean-journal.com


Clean 2007, 35 (2), 186 – 192 Modeling of Aeration Efficiency 187<br />

the oxygen transfer posses and the ANFIS, the effectiveness of the<br />

proposed intelligent system is demonstrated.<br />

2 Preliminaries<br />

The oxygen transfer process and the theoretical foundations for the<br />

intelligent system used in the presented study are given in the following<br />

subsections.<br />

2.1 Oxygen Transfer Process<br />

The rate of oxygen mass transfer, i. e., from the gas (air bubbles) to<br />

the liquid phase (water) is governed by the term described below:<br />

dC<br />

dt<br />

¼ KL<br />

A<br />

V ðCs CÞ ð1Þ<br />

Where C is the dissolved oxygen (DO) concentration, KL is the<br />

liquid film coefficient for oxygen, A is the surface area associated<br />

with the volume, V, over which the transfer occurs, Cs is the saturation<br />

concentration, and t is the time. The term A/V is often called the<br />

specific surface area, a, or surface area per unit volume.<br />

Eq. (1) does not consider sources and sinks of oxygen in the water<br />

body because their rates are relatively slow compared to the oxygen<br />

transfer that occurs at most hydraulic structures due to the increase<br />

in free-surface turbulence and the large quantity of air that is normally<br />

entrained into the flow.<br />

The predictive relations assume that Cs is constant and determined<br />

by the water-atmosphere partitioning. If that assumption is<br />

made, Cs is constant with respect to time, and the oxygen transfer<br />

efficiency (aeration efficiency), E, may be defined as [17]:<br />

E ¼ Cd Cu<br />

Cs Cu<br />

¼ 1<br />

1<br />

r<br />

where u and d are subscripts indicating upstream and downstream<br />

locations, respectively, and r is the oxygen deficit ratio:<br />

[(Cs – Cu)/(Cs –Cd)]<br />

A transfer efficiency value of <strong>1.</strong>0 means that the full transfer up to<br />

the saturation value has occurred at the structure surface. No transfer<br />

would correspond to E = 0.0. The saturation concentration in distilled,<br />

deionized water may be obtained from charts or equations<br />

what is an approximation as the saturation DO concentration for<br />

natural waters is often different from that of distilled, deionized<br />

water due to the salinity affects.<br />

Comparative evaluations of oxygen uptake at hydraulic structures<br />

require that the aeration efficiency is corrected to a reference<br />

temperature. To provide a uniform basis for comparison of measurement<br />

results, the aeration efficiency is often normalized to a 208C<br />

standard. Gulliver et al. [17] proposed the following equation to<br />

describe the influence of the temperature:<br />

1–E20 =(1–E) 1/f (3)<br />

Where E is the transfer efficiency at the actual water temperature,<br />

E20 is the transfer efficiency for 208C, and f is an exponent described<br />

by:<br />

f = <strong>1.</strong>0 + 2.1610 –2 (T –20) + 8.26610 –5 (T–20) 2 (4)<br />

ð2Þ<br />

In this study, the aeration efficiency was normalized to 208C<br />

using Eq. (3).<br />

2.2 Adaptive Network Based Fuzzy Inference System<br />

(ANFIS)<br />

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

detail in [18]. ANFIS is a Multilayer feed forward network where<br />

each node performs a particular function on incoming signals. Both<br />

square and circle node symbols are used to represents different<br />

properties of adaptive learning. To perform desired input-output<br />

characteristics, adaptive learning parameters are updated based on<br />

gradient learning rules [18 – 20]. The ANFIS architecture has six<br />

inputs and one output. This architecture is formed by using five<br />

layer and 64 if-then rules, a sample rule base is described in Eq. (5):<br />

If (x is A1, y is B1, …, zz is F1)<br />

then (f1 = p1x +q1y+… + pp1zz + ri) (5)<br />

Where, x, y, …, zz, are inputs and p, q, r, …, pp, u are linear output<br />

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

described as below:<br />

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

function.<br />

O 1 i ¼ lAiðxÞ ð6Þ<br />

Where, x1, x2, …, x5, x6 are inputs to node i, and Ai, Bi, Ci, …, Hi are<br />

linguistic labels associated with this node function. O1 i is the membership<br />

function of Ai. Usually lAi(x) is chosen as a bell-shaped function<br />

with a maximum value equal to 1 and a mininmum value equal<br />

to 0.<br />

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

multiplies the incoming signals and sends the product out. For<br />

instance:<br />

wi = lAi(x)*lBi(y)*lCi(z)*lDi(xx)*lEi(yy)*lEi(yy)<br />

i =1,2,3,…, 64 (7)<br />

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

Layer-3: Every node in this layer is a circle node labeled N. The i th<br />

node calculates the ratio of the i th rules firing strength to the sum of<br />

all rule's firing strengths.<br />

wi ¼<br />

wi<br />

w1 þ w2:::w64<br />

i ¼ 1; 2; 3; :::; 64 ð8Þ<br />

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

function:<br />

O 4 i ¼ wifi ¼ wiðpix þ qiy þ :::: þ riÞ i ¼ 1; 2; 3; :::; 64 ð9Þ<br />

Where, wi is the output of layer 3 and {pi, qi, ri, …, ppi, ui} is the<br />

parameter 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 labeled S that<br />

computes the overall output of ANFIS as the summation of all<br />

incoming signals.<br />

X<br />

O 5 i<br />

¼ overall output ¼ X<br />

i 2007 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim www.clean-journal.com<br />

i<br />

wifi ¼<br />

i<br />

X<br />

i<br />

wifi<br />

wi<br />

ð10Þ


188 A. Baylar et al. Clean 2007, 35 (2), 186 – 192<br />

Figure 2. Experimental arrangement for the stepped cascade model.<br />

Figure 3. ANFIS model structure.<br />

3 Experimental Results and Application<br />

3.1 Experimental Arrangement<br />

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

Baylar et al. [4, 6] on a large model of a stepped cascade. Schematic<br />

representation of the experimental setup used in these studies is<br />

shown in Fig. 2. All experiments were conducted in a prismatic rectangular<br />

channel with 0.30 m width and 0.50 m deepth. The side<br />

walls were made of transparent methacrylate to follow the flow<br />

regime. Water was pumped from the storage tank to the stilling<br />

tank, from which it entered the stepped channel through an<br />

approach channel.<br />

The discharge was measured by means of a flow meter installed<br />

in the supply line. All experimental runs were carried out in unit<br />

discharges ranging between 16.67 and 166.67 L/s m. For the stepped<br />

channel, the downstream channel was 3.0 m long, 0.35 m wide, and<br />

Figure 4. Training performance of the ANFIS model.<br />

Figure 5. Test performance of the ANFIS model.<br />

0.45 m deep. The slopes of the stepped channel were varied: 14.488,<br />

18.748, 22.558, 308, 408, and 508. For all slopes tested, steps with a<br />

height, h, of 5, 10, and 15 cm were used.<br />

i 2007 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim www.clean-journal.com


Clean 2007, 35 (2), 186 – 192 Modeling of Aeration Efficiency 189<br />

Table <strong>1.</strong> Data of stepped cascade for h = 0.05 m.<br />

q<br />

(m 2 /s610 –3 )<br />

h<br />

(m)<br />

a<br />

(deg.)<br />

L<br />

(m)<br />

Tap water was used throughout the present experiments. The<br />

water was changed for each experiment. The water in the tank was<br />

deoxygenated by the sodium sulfite method. Theoretically, 7.9 g/m 3<br />

of sodium sulfite is required to remove 1 g/m 3 of DO. Based on the<br />

DO of the test tap water, the approximate sodium sulfite requirements<br />

are estimated (a 10 – 20% excess is used). Usually, addition of<br />

cobalt(II) chloride is required at a dosage of 3.3 g/m 3 as a catalyst for<br />

the deoxygenation reaction. In this study, 70 g/m 3 of sodium sulfite<br />

and 3.3 g/m 3 of cobalt(II) chloride were added. The salt content of<br />

the tap water used for all of the experiments reported in this paper<br />

was low and monitored constantly during the experiments to<br />

ensure no significant buildup of residues caused by deoxygenation<br />

of the chemicals added to the water. Therefore, it is unlikely that<br />

N E20<br />

(–)<br />

Flow Regime<br />

16.67 0.05 14.48 5.00 25 0.60 Nappe<br />

33.33 0.05 14.48 5.00 25 0.58 Transition<br />

50.00 0.05 14.48 5.00 25 0.55 Skimming<br />

66.67 0.05 14.48 5.00 25 0.45 Skimming<br />

100.00 0.05 14.48 5.00 25 0.30 Skimming<br />

133.33 0.05 14.48 5.00 25 0.26 Skimming<br />

166.67 0.05 14.48 5.00 25 0.23 Skimming<br />

16.67 0.05 30.00 5.00 50 0.81 Nappe<br />

33.33 0.05 30.00 5.00 50 0.82 Skimming<br />

50.00 0.05 30.00 5.00 50 0.74 Skimming<br />

66.67 0.05 30.00 5.00 50 0.70 Skimming<br />

100.00 0.05 30.00 5.00 50 0.62 Skimming<br />

133.33 0.05 30.00 5.00 50 0.59 Skimming<br />

166.67 0.05 30.00 5.00 50 0.57 Skimming<br />

16.67 0.05 18.74 3.89 25 0.60 Nappe<br />

33.33 0.05 18.74 3.89 25 0.57 Transition<br />

50.00 0.05 18.74 3.89 25 0.52 Skimming<br />

66.67 0.05 18.74 3.89 25 0.44 Skimming<br />

100.00 0.05 18.74 3.89 25 0.28 Skimming<br />

133.33 0.05 18.74 3.89 25 0.22 Skimming<br />

166.67 0.05 18.74 3.89 25 0.16 Skimming<br />

16.67 0.05 40.00 3.89 50 0.74 Transition<br />

33.33 0.05 40.00 3.89 50 0.75 Skimming<br />

50.00 0.05 40.00 3.89 50 0.72 Skimming<br />

66.67 0.05 40.00 3.89 50 0.70 Skimming<br />

100.00 0.05 40.00 3.89 50 0.63 Skimming<br />

133.33 0.05 40.00 3.89 50 0.59 Skimming<br />

166.67 0.05 40.00 3.89 50 0.56 Skimming<br />

16.67 0.05 22.55 3.26 25 0.68 Nappe<br />

33.33 0.05 22.55 3.26 25 0.61 Transition<br />

50.00 0.05 22.55 3.26 25 0.53 Skimming<br />

66.67 0.05 22.55 3.26 25 0.42 Skimming<br />

100.00 0.05 22.55 3.26 25 0.32 Skimming<br />

133.33 0.05 22.55 3.26 25 0.29 Skimming<br />

166.67 0.05 22.55 3.26 25 0.24 Skimming<br />

16.67 0.05 50.00 3.26 50 0.79 Transition<br />

33.33 0.05 50.00 3.26 50 0.77 Skimming<br />

50.00 0.05 50.00 3.26 50 0.75 Skimming<br />

66.67 0.05 50.00 3.26 50 0.74 Skimming<br />

100.00 0.05 50.00 3.26 50 0.72 Skimming<br />

133.33 0.05 50.00 3.26 50 0.66 Skimming<br />

166.67 0.05 50.00 3.26 50 0.64 Skimming<br />

the results were measurably affected by the presence of chemicals<br />

or pollutants.<br />

Each experiment was started by filling the storage tank with<br />

water by adding Na2SO3 and CoCl2 for chemical deoxygenation. During<br />

the experiments, DO measurements upstream and downstream<br />

of the stepped cascade were taken using calibrated portable HANNA<br />

Model HI 9142 oxygen meters at the locations identified in Fig. 2.<br />

Measurements were made by submersing the probe to a depth of<br />

approximately 0.20 m at the sampling points. The DO meters were<br />

calibrated daily according to local atmospheric pressure, prior to<br />

use, by the air calibration method. Calibration procedures followed<br />

those recommended by the manufacturer. The calibration was performed<br />

in humid air under ambient conditions. In this study, the<br />

i 2007 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim www.clean-journal.com


190 A. Baylar et al. Clean 2007, 35 (2), 186 – 192<br />

Table 2. Data of stepped cascade for h = 0.10 m.<br />

q<br />

(m 2 /s610 –3 )<br />

saturation concentrations were determined by the chart of McGhee<br />

[21].<br />

3.2 Modeling<br />

h<br />

(m)<br />

a<br />

(deg.)<br />

L<br />

(m)<br />

The experimental results for the aeration efficiency in the stepped<br />

cascade aerators are given in Tabs. 1 – 3.<br />

The ANFIS model used in this study is shown in Fig. 3. The parameters<br />

considered in the study are unit discharge (q), step height (h),<br />

channel slope (a), channel length (L), total number of steps (N), flow<br />

regime information and aeration efficiency at 208C(E20). The parameters,<br />

q, h, a, L, N, and the flow regime information were used as<br />

inputs to the ANFIS model for the estimation of E20. In the seventh<br />

column, the numbers 1, 2, and 3 used to represent the flow regimes,<br />

nappe, transition, and skimming, respectively. 100 of 126 experimental<br />

data sets were used to train the ANFIS model and 26 experimental<br />

data sets were used for the validation test. The 26 test data<br />

were randomly selected among the whole data.<br />

Before training and testing, the training input and output values<br />

were normalized using Eq. (11):<br />

xi ¼ xi xmin<br />

xmax xmin<br />

N E20<br />

(–)<br />

Flow Regime<br />

16.67 0.10 14.48 5.00 12 0.55 Nappe<br />

33.33 0.10 14.48 5.00 12 0.54 Nappe<br />

50.00 0.10 14.48 5.00 12 0.54 Nappe<br />

66.67 0.10 14.48 5.00 12 0.52 Transition<br />

100.00 0.10 14.48 5.00 12 0.44 Transition<br />

133.33 0.10 14.48 5.00 12 0.41 Skimming<br />

166.67 0.10 14.48 5.00 12 0.34 Skimming<br />

16.67 0.10 30.00 5.00 25 0.80 Nappe<br />

33.33 0.10 30.00 5.00 25 0.79 Nappe<br />

50.00 0.10 30.00 5.00 25 0.77 Nappe<br />

66.67 0.10 30.00 5.00 25 0.75 Transition<br />

100.00 0.10 30.00 5.00 25 0.72 Skimming<br />

133.33 0.10 30.00 5.00 25 0.67 Skimming<br />

166.67 0.10 30.00 5.00 25 0.60 Skimming<br />

16.67 0.10 18.74 3.89 12 0.58 Nappe<br />

33.33 0.10 18.74 3.89 12 0.58 Nappe<br />

50.00 0.10 18.74 3.89 12 0.55 Nappe<br />

66.67 0.10 18.74 3.89 12 0.55 Transition<br />

100.00 0.10 18.74 3.89 12 0.47 Transition<br />

133.33 0.10 18.74 3.89 12 0.41 Skimming<br />

166.67 0.10 18.74 3.89 12 0.37 Skimming<br />

16.67 0.10 40.00 3.89 25 0.74 Nappe<br />

33.33 0.10 40.00 3.89 25 0.76 Nappe<br />

50.00 0.10 40.00 3.89 25 0.77 Transition<br />

66.67 0.10 40.00 3.89 25 0.76 Transition<br />

100.00 0.10 40.00 3.89 25 0.70 Skimming<br />

133.33 0.10 40.00 3.89 25 0.66 Skimming<br />

166.67 0.10 40.00 3.89 25 0.63 Skimming<br />

16.67 0.10 22.55 3.26 12 0.62 Nappe<br />

33.33 0.10 22.55 3.26 12 0.59 Nappe<br />

50.00 0.10 22.55 3.26 12 0.57 Nappe<br />

66.67 0.10 22.55 3.26 12 0.55 Transition<br />

100.00 0.10 22.55 3.26 12 0.46 Skimming<br />

133.33 0.10 22.55 3.26 12 0.39 Skimming<br />

166.67 0.10 22.55 3.26 12 0.30 Skimming<br />

16.67 0.10 50.00 3.26 25 0.77 Nappe<br />

33.33 0.10 50.00 3.26 25 0.74 Transition<br />

50.00 0.10 50.00 3.26 25 0.74 Transition<br />

66.67 0.10 50.00 3.26 25 0.73 Transition<br />

100.00 0.10 50.00 3.26 25 0.71 Skimming<br />

133.33 0.10 50.00 3.26 25 0.68 Skimming<br />

166.67 0.10 50.00 3.26 25 0.65 Skimming<br />

ð11Þ<br />

Where xmin and xmax denote the minimum and maximum of the<br />

stage and discharge data. Each input has two bell-shaped membership<br />

functions. The desired sum squared error value was selected as<br />

0.000<strong>1.</strong> The ANFIS model performed this value at 300 epochs.<br />

i 2007 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim www.clean-journal.com


Clean 2007, 35 (2), 186 – 192 Modeling of Aeration Efficiency 191<br />

Table 3. Data of stepped cascade for h = 0.15 m.<br />

q<br />

(m 2 /s610 –3 )<br />

h<br />

(m)<br />

The training performance of the ANFIS model is graphically<br />

showed in Fig. 4. Moreover, the test performance of the ANFIS model<br />

is graphically presented in Fig. 5. As it can be seen from Fig. 5, the<br />

ANFIS model estimates the measured values with a high accuracy.<br />

The regression coefficient (R 2 ) was calculated as R 2 = 0.999 for a training<br />

performance of the ANFIS model and R 2 = 0.985 for a test performance<br />

of the model.<br />

4 Conclusions<br />

a<br />

(deg.)<br />

L<br />

(m)<br />

Hydraulic structures can increase dissolved oxygen levels by creating<br />

turbulent conditions where small air bubbles are carried into<br />

the bulk of the flow. Stepped chute aeration is a particular instance<br />

of this. In this study, an ANFIS model was used in estimation of the<br />

aeration efficiency of stepped cascade aerators. There was a good<br />

agreement between the measured aeration efficiencies and the<br />

values computed from the ANFIS model. This is evidenced by a very<br />

high regression coefficient, R 2 = 0.985. Therefore, ANFIS can be used<br />

to estimate the aeration efficiency in stepped cascade aerators.<br />

References<br />

N E20<br />

(–)<br />

Flow Regime<br />

16.67 0.15 14.48 5.00 8 0.49 Nappe<br />

33.33 0.15 14.48 5.00 8 0.50 Nappe<br />

50.00 0.15 14.48 5.00 8 0.48 Nappe<br />

66.67 0.15 14.48 5.00 8 0.46 Nappe<br />

100.00 0.15 14.48 5.00 8 0.43 Nappe<br />

133.33 0.15 14.48 5.00 8 0.40 Transition<br />

166.67 0.15 14.48 5.00 8 0.40 Transition<br />

16.67 0.15 30.00 5.00 16 0.78 Nappe<br />

33.33 0.15 30.00 5.00 16 0.76 Nappe<br />

50.00 0.15 30.00 5.00 16 0.75 Nappe<br />

66.67 0.15 30.00 5.00 16 0.75 Nappe<br />

100.00 0.15 30.00 5.00 16 0.73 Nappe<br />

133.33 0.15 30.00 5.00 16 0.72 Transition<br />

166.67 0.15 30.00 5.00 16 0.71 Skimming<br />

16.67 0.15 18.74 3.89 8 0.57 Nappe<br />

33.33 0.15 18.74 3.89 8 0.58 Nappe<br />

50.00 0.15 18.74 3.89 8 0.53 Nappe<br />

66.67 0.15 18.74 3.89 8 0.52 Nappe<br />

100.00 0.15 18.74 3.89 8 0.47 Nappe<br />

133.33 0.15 18.74 3.89 8 0.43 Transition<br />

166.67 0.15 18.74 3.89 8 0.39 Transition<br />

16.67 0.15 40.00 3.89 16 0.76 Nappe<br />

33.33 0.15 40.00 3.89 16 0.76 Nappe<br />

50.00 0.15 40.00 3.89 16 0.77 Nappe<br />

66.67 0.15 40.00 3.89 16 0.76 Nappe<br />

100.00 0.15 40.00 3.89 16 0.71 Transition<br />

133.33 0.15 40.00 3.89 16 0.69 Transition<br />

166.67 0.15 40.00 3.89 16 0.68 Skimming<br />

16.67 0.15 22.55 3.26 8 0.56 Nappe<br />

33.33 0.15 22.55 3.26 8 0.56 Nappe<br />

50.00 0.15 22.55 3.26 8 0.53 Nappe<br />

66.67 0.15 22.55 3.26 8 0.52 Nappe<br />

100.00 0.15 22.55 3.26 8 0.51 Nappe<br />

133.33 0.15 22.55 3.26 8 0.47 Transition<br />

166.67 0.15 22.55 3.26 8 0.41 Transition<br />

16.67 0.15 50.00 3.26 16 0.77 Nappe<br />

33.33 0.15 50.00 3.26 16 0.75 Nappe<br />

50.00 0.15 50.00 3.26 16 0.74 Nappe<br />

66.67 0.15 50.00 3.26 16 0.74 Transition<br />

100.00 0.15 50.00 3.26 16 0.72 Transition<br />

133.33 0.15 50.00 3.26 16 0.70 Skimming<br />

166.67 0.15 50.00 3.26 16 0.69 Skimming<br />

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