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Civil and Environmental Research www.iiste.org 
ISSN 2224-5790 (Paper) ISSN 2225-0514 (Online) 
Vol.6, No.8, 2014 
The Effect of Hydraulic Structure on Aeration Performance 
Case Study: Stepped Cascade with End Sill 
Prof.Dr. Dheyaa Wajid Abbood1 Hanan Hussien Abood2 , 
Al-Mustansiriya University , Civil Engineering Department,P.O.14150,Baghdad , Iraq 
*Email:Dr.Dheyaa@gmail.com, hananhu_2006@yahoo.com 
ABSTRACT 
Cascade aeration has been utilized as a hydraulic structure for years which has proven to be the least costly 
aeration system in replenishing dissolved oxygen. The aeration performance of the cascade structure with end 
sill has been investigated in a large laboratory cascade structure which has been designed and constructed at Al- 
Mustansiriya university in environmental hydraulic .An empirical equation to predicting the oxygen transfer 
efficiency for different models of cascade structure with end sill was correlated. The results indicated that l/h 
and s/h were a significant effect on the aeration efficiency of cascade structure. 
Keywords: Hydraulic structure, Stepped cascade , End sill ,Aeration, Oxygen transfer 
1-Introduction 
Aeration or re-aeration is the physical process of oxygen transfer or oxygen absorption from the atmosphere acts 
to replenish the used oxygen. Aeration is one of the fundamental parameters required to maintain dissolved 
oxygen for the aerobic bacteria that feed on organics whether in treatment facilities or in streams and rivers (A. 
Baylar, 2010). (Metcalf & Eddy, 2003).Hydraulic structures increase the amount of dissolved oxygen in a river 
system, even though the water is in contact with the structure for only a short time . The same quantity of 
oxygen transfer that normally would occur over several kilometers in a river can occur at a single hydraulic 
structure (A. Baylar, 2010). 
Aeration efficiency (E20) of hydraulic structures has been studied by many investigators.. Within the last few 
years there has been a growing interest in the air entrainment by water jets plunging into pools(A. Baylar, 2010). 
Tebbutt et al. (1977) presented some aeration data for stepped cascades with nappe and skimming flows. Since 
they conducted the experiments in small-size facilities, reduced free-surface aeration was present of Essery et al. 
(1978) studied nappe flow in pooled stepped cascades. Novak (1994) compared a cascade as investigated by 
Essery et al. (1978) with a cascade of pools and a single jet/pool configuration. Toombes and Chanson (2000) 
and Chanson and Toombes (2000) considered aeration in small-slope stepped cascades. Chanson and Toombes 
(2002) conducted gas–liquid interface measurements in stepped cascade. Recently, Baylar et al. ( 2007a, b,2009 
), Baylar and Emiroglu (2003b, 2005,2006), Emiroglu and Baylar (2003a,), have conducted many studies to 
investigate air/water flow ratio (Qa/Qw) and aeration efficiency (E20) in cascade structure . Gulliver and 
Wilhelms (1992) have stated that an upstream DO deficit of greater than 2.5 mg/l is normally required for 
accuracy in an oxygen-transfer efficiency measurement. Wormleaton and Soufiani (1998) found that the oxygen 
transfer efficiency, E, is sensibly independent of the upstream DO deficit. 
Y. B. M. Heza et al (2008) investigated the feasibility of using aeration weir systems in agricultural drains 
receiving domestic sewage to increase its quality by increasing the dissolved oxygen content (DO). 
Stepped chutes have become popular in recent years mainly due to the intrinsic low cost and the speed of 
construction. In a stepped chute, the provision of steps can produce significant energy dissipation . The flow on 
stepped chutes can be in either nappe or skimming flow regimes (Emiroglu, M. E., & Baylar, A. 2003a). 
Rajaratnam (1990), Chamani and Rajaratnam (1994), Chanson (1994a,b; 1996), and Chamani and Rajaratnam 
(1999a,b) have focused mainly on characteristics of nappe flow and skimming flow over stepped chutes. There 
are not found any published analytical or physical studies of the dissolved oxygen levels produced in cascade 
structure with end sill. The basic goal of this study is to characterize the cascade efficiency for different cascade 
geometries, and the effect of varying l/h and s/h. 
2- Aeration Process 
Oxygen transfer and dispersion into water essentially is governed by the processes of molecular diffusion, 
turbulent mixing, or both. At the water surface it requires a difference in active partial pressures between the air 
and water. Lewis and Whitman (1924) suggested that two laminar films or layers lie on either side of the air-water 
interface. Both films offer resistance to the passage of oxygen molecules into the water. However, for a 
slightly soluble gas, such as oxygen in water, the resistance of the waterside is very much the greater of the two, 
effectively controlling the transfer process. The mass transfer rate (dm/dt) of gas molecules across an interface is 
known to be proportional to the concentration gradient across the interface, and this can be expressed as: 
11 
= =KL (CS-C) (1)
Civil and Environmental Research www.iiste.org 
ISSN 2224-5790 (Paper) ISSN 2225-0514 (Online) 
Vol.6, No.8, 2014 
where C is DO concentration(ML-3), KL is liquid film coefficient for oxygen (LT-1),A (L2) is surface area 
associated with the volume, V(L3), over which transfer occurs, Cs is saturation concentration (ML-3), and t is 
time (T). The term A/V is often called the specific surface area, a, or surface area per unit volume (L-1). 
The predictive relations described herein all assume that Cs is constant and determined by the water-atmosphere 
partitioning. If that assumption is made, Cs is constant with respect to time, and the oxygen transfer efficiency 
(aeration performance), E, may be defined as (Gulliver et al. 1990): 
E = 1- = (2) 
where u and d are subscripts indicating upstream and downstream 
locations, respectively, and r is the oxygen deficit ratio [(Cs – Cu)/(Cs – Cd)]. 
The saturation concentration in distilled, deionized water may be obtained from charts or equations. This is an 
approximation because the saturation DO concentration for natural waters is often different from that of distilled, 
deionized water due to the salinity effects. In this study, the saturation concentrations were determined by the 
chart of McGhee (1991). 
3-Experimental Arrangement and Experiments 
The lab-scale model consist of inlet PVR tank , inlet pump, transparent methacrylate cascade structure , 
recycling tank , recycling pump and outlet PVR tank connected to each other by galvanized cast iron pipes , 
fittings and flow meter .The schematic representation of lab- scale unit is shown in figure ( 1) and plate (1). 
Figure (1): Schematic representation of lab-scale unit 
The primary PVR tank of 5000 liter capacity connected to a pump which is of 600 l/min pump flow rate . The 
pump has been connected to flow meter by control valve for flow control . The cascade structure was constructed 
from three parts . The first part is a settling transparent methacrylate tank of dimension (0.8m*0.6m*1.25m),the 
second part is transparent methacrylate cascade steps of dimension (2.44m* 0.23m* 1.25m ) , the third part is a 
recycling transparent methacrylate tank of dimension (2.44m*0.3m *0.25m). Each part was made from a frame 
of iron angle connected to each other by welding and transparent methacrylate. 
In the settling tank a weir of 0.3 meter length and 0.23 m width was constructed and calibrated to measure the 
discharge . The laboratory model is depicted in plate (1). The recycling tank is connected to the outlet tank by a 
recycling pump of discharge= 600 l/min. 
12
Civil and Environmental Research www.iiste.org 
ISSN 2224-5790 (Paper) ISSN 2225-0514 (Online) 
Vol.6, No.8, 2014 
Plate (1): General arrangement of laboratory unit 
During the experiments, a digital thermometer was used to measure water temperature. Since the saturation 
concentration of oxygen is a strong function of temperature, the aeration efficiency is also temperature 
dependent. To provide a uniform basis for comparison of different systems ,the aeration efficiency is often 
normalized to a 20°C standard. Gulliver et al. (1990) proposed the following equation to describe the influence 
of temperature: 
E20=1-(1-ET)1/1.0+0.02103(T-20)+8.26*10-5(T-20)2 (3) 
where ET is oxygen transfer efficiency at the water temperature of measurement and E20 is oxygen transfer 
efficiency at 20°C. In this study, the aeration efficiency was normalized to 20°C using equation 3. Two cases of 
cascade were experimented 
1- For Case 1 the stepped cascade weirs are designed and constructed from three steps each step of dimension 
0.6m*0.23 m and of height 0.2 m The end sill of variable height (35,60,80,100 mm) have been tested . 
2- For Case 2 The cascade step of dimension (0.4m *0.23m) and of 0.1 m height. The end sill of variable height 
(40,50 mm) have been tested. 
The discharge was measured by means of a rotometer which has been installed in the supply line. The slope of 
the stepped chute, defined as l/h was equal to 3.0 for case 1 (α = 18.43°), 4.0 for case 2 (α = 14.036°). All 
experimental runs were carried out with discharges ranging between 1 and 4 l/s in 7 steps. 
Each experiment was started by filling the storage tank with marginal 
water and the characteristics of the marginal water as shown in Table was measured.The salt content of marginal 
water used for all of the experiments reported in this paper was low and was monitored constantly during the 
experiments to ensure there was no buildup of residues caused by the deoxygenation chemicals added to the 
water. Therefore, the results were not affected by the presence of any chemicals or pollutants. 
DO measurements at the upstream and downstream of the stepped chute were taken using calibrated portable 
HANNA Model HI 9142 oxygen meters at the locations identified. Measurements were made by submersing the 
probe to a depth of approximately 0.20 m at sampling points. The DO meters were calibrated daily according to 
local atmospheric pressure, prior to use, by the air calibration method. Calibration procedures followed those 
recommended by the manufacturer. The calibration was performed in humid air under ambient conditions. From 
equation 2 it can be seen that the measurement of transfer efficiency becomes quite sensitive to measurement 
errors with a low upstream DO deficit. 
4- Results and Analysis 
The aeration efficiency of stepped cascade were obtained depending on cascade inclination angle (α), sill height 
(s), 
discharge (Q) and chemical oxygen demand of aeration performance of experiments COD . Aeration efficiency 
results (E20).Tables 1-6 shows the results of experiments for cases 1,2 
13 
Settling tank 
Cascade structure 
Flow meter 
Pump 
Weir 
Valve
Civil and Environmental Research www.iiste.org 
ISSN 2224-5790 (Paper) ISSN 2225-0514 (Online) 
Vol.6, No.8, 2014 
Table (1): Results of experiments of Table (2): Results of experiments of 
Case 1 with end sill =35 mm Case 1 with end sill =60 mm 
Disch 
arge 
14 
PH 
U/S 
PH 
D/S 
EC 
U/S 
EC 
D/S 
TDS 
U/S 
TDS 
D/S 
1 7.66 7.77 1038 1047 527 516 
1.5 7.49 7.47 1040 1041 528 520 
2 7.32 7.37 1042 1035 521 516 
2.5 7.31 7.37 1055 1048 535 523 
3 7.3 7.36 1066 1062 555 531 
3.5 7.28 7.34 1064 1061 540 534 
4 7.27 7.32 1063 1061 537 531 
Table (3): Results of experiments of Table (4): Results of experiments of 
Case 1 with end sill =80 mm Case 1 with end sill =100 mm 
Disch 
arge 
PH 
U/S 
PH 
D/S 
EC 
U/S 
EC 
D/S 
TDS 
U/S 
TDS 
D/S 
1 7.01 7.1 1037 1034 516 510 
1.5 7.04 7.08 1030 1027 515 510 
2 7.06 7.06 1026 1021 513 508 
2.5 7.11 7.09 1024 1024 513 508 
3 7.13 7.20 1023 1028 513 507 
3.5 7.1 7.22 1031 1029 518 514 
4 7.08 7.34 1039 1030 524 515 
Table (5): Results of experiments of Table (6): Results of experiments of 
Case 2 with end sill =40 mm Case 2 with end sill =50 mm 
Disch 
arge 
PH 
U/S 
PH 
D/S 
EC 
U/S 
EC 
D/S 
TDS 
U/S 
TDS 
D/S 
1 7.36 7.56 1085 1055 542 524 
1.5 7.28 7.42 1086 1075 542 535 
2 7.22 7.28 1087 1095 543 546 
2.5 7.23 7.27 1087 1090 542 545 
3 7.24 7.26 1087 1084 542 543 
3.5 7.2 7.25 1091 1088 543 545 
4 7.18 7.24 1095 1092 545 546 
The COD range (32-50) mg/l. 
Figures (2-7) represent aeration efficiency E20 for Case 1,2 for different models 
Figure (2 ): Relation between discharge and aeration efficiency for case No.1 model No.1 
Disch 
arge 
PH 
U/S 
PH 
D/S 
EC 
U/S 
EC 
D/S 
TDS 
U/S 
TDS 
D/S 
1 6.82 6.85 1034 1023 515 509 
1.5 6.83 6.86 1027 1017 512 508 
6.824 66.83 6.9 1020 1011 509 506 
2.5 6.94 7.07 1006 999 502 499 
3 7.06 7.24 993 990 496 493 
3.5 7.04 7.06 998 995 498 496 
4 7.03 7.09 1002 999 500 497 
Disch 
arge 
PH 
U/S 
PH 
D/S 
EC 
U/S 
EC 
D/S 
TDS 
U/S 
TDS 
D/S 
1 7.41 7.53 1025 1084 566 544 
1.5 7.41 7.47 966 1074 538 509 
2 7.4 7.42 907 1064 453 533 
2.5 7.3 7.38 967 1046 584 523 
3 7.22 7.33 1028 1028 525 514 
3.5 7.40 7.47 1067 1048 551 524 
4 7.62 7.78 1106 1066 587 534 
Disch 
arge 
PH 
U/S 
PH 
D/S 
EC 
U/S 
EC 
D/S 
TDS 
U/S 
TDS 
D/S 
1 7.36 7.32 978 925 475 460 
1.5 7.27 7.32 953 922 469 460 
2 7.19 7.32 929 920 463 461 
2.5 7.23 7.28 930 924 464 462 
3 7.24 7.26 931 929 465 463 
3.5 7.26 7.27 926 922 462 462 
4 7.28 7.28 922 918 460 460
Civil and Environmental Research www.iiste.org 
ISSN 2224-5790 (Paper) ISSN 2225-0514 (Online) 
Vol.6, No.8, 2014 
Figure (3): Relation between discharge and aeration efficiency for case No.1 model No.2 
Figure (4): Relation between discharge and aeration efficiency for case No.1 model No.3 
Figure (5): Relation between discharge and aeration efficiency for case No.1 model No.4 
15
Civil and Environmental Research www.iiste.org 
ISSN 2224-5790 (Paper) ISSN 2225-0514 (Online) 
Vol.6, No.8, 2014 
Figure (6): Relation between discharge and aeration efficiency for case No.2 model No.1 
Figure (7): Relation between aeration efficiency - discharge for case No.2 model No.2 
Figure 8 represent a comparison between Aeration efficiency E20 for case 1,2 for s/h=0.4, and figure 9 represent 
a comparison between Aeration efficiency E20 for case 1,2 for s/h=0.5. 
From figures it is clear that case 1 is most efficient than case 2 and case 1 model 4 is most efficient than the other 
models. 
Figure (8): Aeration efficiency- discharge relationship for s/h=0.4 for case No.1 model No.3 and case No.2 
model No.1 
16
Civil and Environmental Research www.iiste.org 
ISSN 2224-5790 (Paper) ISSN 2225-0514 (Online) 
Vol.6, No.8, 2014 
Figure (9 ): Aeration efficiency - discharge relationship for s/h=0.5 for case No.1 model No.4 and case No.2 
model No.2 
An empirical correlation predicting oxygen transfer efficiency was 
developed for stepped cascade. The resulting correlation is given in equation 4: 
E20=(0.108+2.499*(s/l)1.329/2.69*10-11*(l/h)-22.053*(F* )0.701) (4); correlation coefficient=85% 
where h is the step height (m), l is the step length (m), and F is Froude number , s end sill height (m). 
The measured oxygen transfer efficiencies were compared to those 
predicted with equation 4. Good agreement between the measured oxygen 
transfer efficiencies and the values computed from the predictive 
equation was obtained. 
5-Conclusions 
Set of laboratory experiments have been carried out continuously on stepped cascade with end sill in order to 
determine aeration performance. An empirical correlation has been developed that predicted the oxygen transfer 
efficiency for stepped cascade. Based on the findings of this study, the following conclusions can be drawn: 
• Nappe flow was observed for all cases and the aeration efficiency 
of stepped chute with end sill increased with discharge 
• For stepped cascade with end sill, the aeration efficiency increased as chute inclination angle increased. 
• Additional testing is necessary to assess the effect of aeration efficiency for stepped cascade with end sill 
when discharge is higher than the largest discharge tested, 4 l/s. 
• The COD is an effective factor in aeration efficiency and as COD increases , the aeration efficiency decreased 
because of pollutant effect of marginal water (COD) 
References 
A. Baylar . (2010)" Hydraulic Structures in Water Aeration Processes " Water Air Soil Pollut 210:87–100 
Baylar, A., & Emiroglu, M. E. (2003b). Study of aeration efficiency at stepped channels. Proceedings of the 
Institution of Civil Engineers—Water & Maritime Engineering, 156(WM3), 257–263. 
Baylar, A., & Emiroglu, M. E. (2005). Closure of 'Study of aeration efficiency at stepped channels. Proceedings 
of the Institution of Civil Engineers—Water Management, 158 (WM2), 89–90. 
Baylar, A., Bagatur, T., & Emiroglu, M. E. (2007a). Aeration efficiency with nappe flow over stepped cascades. 
Proceedings of the Institution of Civil Engineers—Water Management, 160(1), 43–50. 
Baylar, A., Bagatur, T., & Emiroglu, M. E. (2007b). Prediction of oxygen content of nappe, transition and 
skimming flow regimes in stepped channel chutes. Journal of Environmental Engineering and Science, 
6(2), 201–208. 
Chamani MR, Rajaratnam N. 1994. Jet flow on stepped spillways. J. Hydraul. Eng. 120(2):254–259. 
Chamani MR, Rajaratnam N. 1999a. Characteristics of skimming flow over stepped spillways. J. Hydraul. Eng. 
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125(4):361–368. 
Chamani MR, Rajaratnam N. 1999b. Onset of skimming flow on stepped spillways. J. Hydraul. Eng. 
125(9):969–971. 
Chanson H. 1994a. Comparison of energy dissipation between nappe and skimming flow regimes on stepped 
chutes. J. Hydraul. Res. 32(2):213–218.
Civil and Environmental Research www.iiste.org 
ISSN 2224-5790 (Paper) ISSN 2225-0514 (Online) 
Vol.6, No.8, 2014 
Chanson H. 1994b. Hydraulics of skimming flows over stepped channel and spillways. J. Hydraul. Res. 
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32(3):445–460. 
Chanson H. 1996. Prediction of the transition nappe/skimming flow on a stepped channel. J. Hydraul. Res. 
34(3):421–429. 
Chanson, H., & Toombes, L. (2000). Discussion of Stream reaeration in nonuniform flow: Macroroughness 
enhancement. Journal of Hydraulic Engineering ASCE, 126(3), 222–224. 
Chanson, H., & Toombes, L. (2002). Experimental study of gas−liquid interfacial properties in a stepped cascade 
flow. Environmental Fluid Mechanics, 2(3), 241–263. 
Emiroglu, M. E., & Baylar, A. (2003a). An investigation of effect of stepped chutes with end sill on aeration 
performance. Water Quality Research Journal of Canada, 38(3), 527–539. 
Essery, I. T. S., Tebbutt, T. H. Y., & Rasaratnam, S. K. (1978). Design of spillways for reaeration of polluted 
waters, Rep. 72. London: CIRIA. 
Gulliver JS, Thene JR, Rindels AJ. 1990. Indexing gas transfer in self-aerated flows. J. Environ. Eng. 
116(3):503–523. 
Gulliver JS, Wilhelms SC. 1992. Discussion of ‘Aeration at Ohio River basin navigation dams’, by Railsback 
SF, Bownds JM, Sak MJ, Stevens MM, Taylor GH. J. Environ. Eng. 108(3):444–446. 
Lewis WK, Whitman WG. 1924. Principles of gas absorption. Ind. Eng. Chem. 16(12):1215–1220. 
McGhee TJ. 1991. Water supply and sewerage. McGraw-Hill International Editions, 6th ed 
Metcalf and Eddy, Inc. (2003). "Wastewater Engineering Treatment and Reuse." International ed. McGraw Hill, 
New York. 
Novak, P. (1994). Improvement of water quality in rivers by aeration at hydraulic structure. In M. Hino (Ed.), 
Water quality and its control. Madrid: International Association of Hydraulic Research. 
Rajaratnam N. 1990. Skimming flow in stepped spillways. J. Hydraul. Eng. 116(4): 587–591. 
Tebbutt, T. H. Y., Essery, I. T. S., & Rasaratnam, S. K. (1977). Reaeration performance of stepped cascades. 
Journalof the Institution of Water Engineering Science, 31(4), 285–297. 
Toombes, L., & Chanson, H. (2000). Air−water flow and gas transfer at aeration cascades: a comparative study 
of smooth and stepped chutes (pp. 77–84). Zurich, Switzerland: Proceedings of the International 
Workshop on Hydraulics of Stepped Spillways. 
Wormleaton PR, Soufiani E. 1998. Aeration performance of triangular platform labyrinth weirs. J. Environ. Eng. 
124(8):709–719. 
Y. B. M. Heza1, M. El-din , N. S. Donia and A. M. Refaat "Water Quality Improvement of Drains Polluted by 
Wastewaters Using Conventional Weir" Twelfth International Water Technology Conference , IWTC12 
2008, Alexandria, Egypt.
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The effect of hydraulic structure on aeration performance

  • 1. Civil and Environmental Research www.iiste.org ISSN 2224-5790 (Paper) ISSN 2225-0514 (Online) Vol.6, No.8, 2014 The Effect of Hydraulic Structure on Aeration Performance Case Study: Stepped Cascade with End Sill Prof.Dr. Dheyaa Wajid Abbood1 Hanan Hussien Abood2 , Al-Mustansiriya University , Civil Engineering Department,P.O.14150,Baghdad , Iraq *Email:Dr.Dheyaa@gmail.com, hananhu_2006@yahoo.com ABSTRACT Cascade aeration has been utilized as a hydraulic structure for years which has proven to be the least costly aeration system in replenishing dissolved oxygen. The aeration performance of the cascade structure with end sill has been investigated in a large laboratory cascade structure which has been designed and constructed at Al- Mustansiriya university in environmental hydraulic .An empirical equation to predicting the oxygen transfer efficiency for different models of cascade structure with end sill was correlated. The results indicated that l/h and s/h were a significant effect on the aeration efficiency of cascade structure. Keywords: Hydraulic structure, Stepped cascade , End sill ,Aeration, Oxygen transfer 1-Introduction Aeration or re-aeration is the physical process of oxygen transfer or oxygen absorption from the atmosphere acts to replenish the used oxygen. Aeration is one of the fundamental parameters required to maintain dissolved oxygen for the aerobic bacteria that feed on organics whether in treatment facilities or in streams and rivers (A. Baylar, 2010). (Metcalf & Eddy, 2003).Hydraulic structures increase the amount of dissolved oxygen in a river system, even though the water is in contact with the structure for only a short time . The same quantity of oxygen transfer that normally would occur over several kilometers in a river can occur at a single hydraulic structure (A. Baylar, 2010). Aeration efficiency (E20) of hydraulic structures has been studied by many investigators.. Within the last few years there has been a growing interest in the air entrainment by water jets plunging into pools(A. Baylar, 2010). Tebbutt et al. (1977) presented some aeration data for stepped cascades with nappe and skimming flows. Since they conducted the experiments in small-size facilities, reduced free-surface aeration was present of Essery et al. (1978) studied nappe flow in pooled stepped cascades. Novak (1994) compared a cascade as investigated by Essery et al. (1978) with a cascade of pools and a single jet/pool configuration. Toombes and Chanson (2000) and Chanson and Toombes (2000) considered aeration in small-slope stepped cascades. Chanson and Toombes (2002) conducted gas–liquid interface measurements in stepped cascade. Recently, Baylar et al. ( 2007a, b,2009 ), Baylar and Emiroglu (2003b, 2005,2006), Emiroglu and Baylar (2003a,), have conducted many studies to investigate air/water flow ratio (Qa/Qw) and aeration efficiency (E20) in cascade structure . Gulliver and Wilhelms (1992) have stated that an upstream DO deficit of greater than 2.5 mg/l is normally required for accuracy in an oxygen-transfer efficiency measurement. Wormleaton and Soufiani (1998) found that the oxygen transfer efficiency, E, is sensibly independent of the upstream DO deficit. Y. B. M. Heza et al (2008) investigated the feasibility of using aeration weir systems in agricultural drains receiving domestic sewage to increase its quality by increasing the dissolved oxygen content (DO). Stepped chutes have become popular in recent years mainly due to the intrinsic low cost and the speed of construction. In a stepped chute, the provision of steps can produce significant energy dissipation . The flow on stepped chutes can be in either nappe or skimming flow regimes (Emiroglu, M. E., & Baylar, A. 2003a). Rajaratnam (1990), Chamani and Rajaratnam (1994), Chanson (1994a,b; 1996), and Chamani and Rajaratnam (1999a,b) have focused mainly on characteristics of nappe flow and skimming flow over stepped chutes. There are not found any published analytical or physical studies of the dissolved oxygen levels produced in cascade structure with end sill. The basic goal of this study is to characterize the cascade efficiency for different cascade geometries, and the effect of varying l/h and s/h. 2- Aeration Process Oxygen transfer and dispersion into water essentially is governed by the processes of molecular diffusion, turbulent mixing, or both. At the water surface it requires a difference in active partial pressures between the air and water. Lewis and Whitman (1924) suggested that two laminar films or layers lie on either side of the air-water interface. Both films offer resistance to the passage of oxygen molecules into the water. However, for a slightly soluble gas, such as oxygen in water, the resistance of the waterside is very much the greater of the two, effectively controlling the transfer process. The mass transfer rate (dm/dt) of gas molecules across an interface is known to be proportional to the concentration gradient across the interface, and this can be expressed as: 11 = =KL (CS-C) (1)
  • 2. Civil and Environmental Research www.iiste.org ISSN 2224-5790 (Paper) ISSN 2225-0514 (Online) Vol.6, No.8, 2014 where C is DO concentration(ML-3), KL is liquid film coefficient for oxygen (LT-1),A (L2) is surface area associated with the volume, V(L3), over which transfer occurs, Cs is saturation concentration (ML-3), and t is time (T). The term A/V is often called the specific surface area, a, or surface area per unit volume (L-1). The predictive relations described herein all assume that Cs is constant and determined by the water-atmosphere partitioning. If that assumption is made, Cs is constant with respect to time, and the oxygen transfer efficiency (aeration performance), E, may be defined as (Gulliver et al. 1990): E = 1- = (2) where u and d are subscripts indicating upstream and downstream locations, respectively, and r is the oxygen deficit ratio [(Cs – Cu)/(Cs – Cd)]. The saturation concentration in distilled, deionized water may be obtained from charts or equations. This is an approximation because the saturation DO concentration for natural waters is often different from that of distilled, deionized water due to the salinity effects. In this study, the saturation concentrations were determined by the chart of McGhee (1991). 3-Experimental Arrangement and Experiments The lab-scale model consist of inlet PVR tank , inlet pump, transparent methacrylate cascade structure , recycling tank , recycling pump and outlet PVR tank connected to each other by galvanized cast iron pipes , fittings and flow meter .The schematic representation of lab- scale unit is shown in figure ( 1) and plate (1). Figure (1): Schematic representation of lab-scale unit The primary PVR tank of 5000 liter capacity connected to a pump which is of 600 l/min pump flow rate . The pump has been connected to flow meter by control valve for flow control . The cascade structure was constructed from three parts . The first part is a settling transparent methacrylate tank of dimension (0.8m*0.6m*1.25m),the second part is transparent methacrylate cascade steps of dimension (2.44m* 0.23m* 1.25m ) , the third part is a recycling transparent methacrylate tank of dimension (2.44m*0.3m *0.25m). Each part was made from a frame of iron angle connected to each other by welding and transparent methacrylate. In the settling tank a weir of 0.3 meter length and 0.23 m width was constructed and calibrated to measure the discharge . The laboratory model is depicted in plate (1). The recycling tank is connected to the outlet tank by a recycling pump of discharge= 600 l/min. 12
  • 3. Civil and Environmental Research www.iiste.org ISSN 2224-5790 (Paper) ISSN 2225-0514 (Online) Vol.6, No.8, 2014 Plate (1): General arrangement of laboratory unit During the experiments, a digital thermometer was used to measure water temperature. Since the saturation concentration of oxygen is a strong function of temperature, the aeration efficiency is also temperature dependent. To provide a uniform basis for comparison of different systems ,the aeration efficiency is often normalized to a 20°C standard. Gulliver et al. (1990) proposed the following equation to describe the influence of temperature: E20=1-(1-ET)1/1.0+0.02103(T-20)+8.26*10-5(T-20)2 (3) where ET is oxygen transfer efficiency at the water temperature of measurement and E20 is oxygen transfer efficiency at 20°C. In this study, the aeration efficiency was normalized to 20°C using equation 3. Two cases of cascade were experimented 1- For Case 1 the stepped cascade weirs are designed and constructed from three steps each step of dimension 0.6m*0.23 m and of height 0.2 m The end sill of variable height (35,60,80,100 mm) have been tested . 2- For Case 2 The cascade step of dimension (0.4m *0.23m) and of 0.1 m height. The end sill of variable height (40,50 mm) have been tested. The discharge was measured by means of a rotometer which has been installed in the supply line. The slope of the stepped chute, defined as l/h was equal to 3.0 for case 1 (α = 18.43°), 4.0 for case 2 (α = 14.036°). All experimental runs were carried out with discharges ranging between 1 and 4 l/s in 7 steps. Each experiment was started by filling the storage tank with marginal water and the characteristics of the marginal water as shown in Table was measured.The salt content of marginal water used for all of the experiments reported in this paper was low and was monitored constantly during the experiments to ensure there was no buildup of residues caused by the deoxygenation chemicals added to the water. Therefore, the results were not affected by the presence of any chemicals or pollutants. DO measurements at the upstream and downstream of the stepped chute were taken using calibrated portable HANNA Model HI 9142 oxygen meters at the locations identified. Measurements were made by submersing the probe to a depth of approximately 0.20 m at sampling points. The DO meters were calibrated daily according to local atmospheric pressure, prior to use, by the air calibration method. Calibration procedures followed those recommended by the manufacturer. The calibration was performed in humid air under ambient conditions. From equation 2 it can be seen that the measurement of transfer efficiency becomes quite sensitive to measurement errors with a low upstream DO deficit. 4- Results and Analysis The aeration efficiency of stepped cascade were obtained depending on cascade inclination angle (α), sill height (s), discharge (Q) and chemical oxygen demand of aeration performance of experiments COD . Aeration efficiency results (E20).Tables 1-6 shows the results of experiments for cases 1,2 13 Settling tank Cascade structure Flow meter Pump Weir Valve
  • 4. Civil and Environmental Research www.iiste.org ISSN 2224-5790 (Paper) ISSN 2225-0514 (Online) Vol.6, No.8, 2014 Table (1): Results of experiments of Table (2): Results of experiments of Case 1 with end sill =35 mm Case 1 with end sill =60 mm Disch arge 14 PH U/S PH D/S EC U/S EC D/S TDS U/S TDS D/S 1 7.66 7.77 1038 1047 527 516 1.5 7.49 7.47 1040 1041 528 520 2 7.32 7.37 1042 1035 521 516 2.5 7.31 7.37 1055 1048 535 523 3 7.3 7.36 1066 1062 555 531 3.5 7.28 7.34 1064 1061 540 534 4 7.27 7.32 1063 1061 537 531 Table (3): Results of experiments of Table (4): Results of experiments of Case 1 with end sill =80 mm Case 1 with end sill =100 mm Disch arge PH U/S PH D/S EC U/S EC D/S TDS U/S TDS D/S 1 7.01 7.1 1037 1034 516 510 1.5 7.04 7.08 1030 1027 515 510 2 7.06 7.06 1026 1021 513 508 2.5 7.11 7.09 1024 1024 513 508 3 7.13 7.20 1023 1028 513 507 3.5 7.1 7.22 1031 1029 518 514 4 7.08 7.34 1039 1030 524 515 Table (5): Results of experiments of Table (6): Results of experiments of Case 2 with end sill =40 mm Case 2 with end sill =50 mm Disch arge PH U/S PH D/S EC U/S EC D/S TDS U/S TDS D/S 1 7.36 7.56 1085 1055 542 524 1.5 7.28 7.42 1086 1075 542 535 2 7.22 7.28 1087 1095 543 546 2.5 7.23 7.27 1087 1090 542 545 3 7.24 7.26 1087 1084 542 543 3.5 7.2 7.25 1091 1088 543 545 4 7.18 7.24 1095 1092 545 546 The COD range (32-50) mg/l. Figures (2-7) represent aeration efficiency E20 for Case 1,2 for different models Figure (2 ): Relation between discharge and aeration efficiency for case No.1 model No.1 Disch arge PH U/S PH D/S EC U/S EC D/S TDS U/S TDS D/S 1 6.82 6.85 1034 1023 515 509 1.5 6.83 6.86 1027 1017 512 508 6.824 66.83 6.9 1020 1011 509 506 2.5 6.94 7.07 1006 999 502 499 3 7.06 7.24 993 990 496 493 3.5 7.04 7.06 998 995 498 496 4 7.03 7.09 1002 999 500 497 Disch arge PH U/S PH D/S EC U/S EC D/S TDS U/S TDS D/S 1 7.41 7.53 1025 1084 566 544 1.5 7.41 7.47 966 1074 538 509 2 7.4 7.42 907 1064 453 533 2.5 7.3 7.38 967 1046 584 523 3 7.22 7.33 1028 1028 525 514 3.5 7.40 7.47 1067 1048 551 524 4 7.62 7.78 1106 1066 587 534 Disch arge PH U/S PH D/S EC U/S EC D/S TDS U/S TDS D/S 1 7.36 7.32 978 925 475 460 1.5 7.27 7.32 953 922 469 460 2 7.19 7.32 929 920 463 461 2.5 7.23 7.28 930 924 464 462 3 7.24 7.26 931 929 465 463 3.5 7.26 7.27 926 922 462 462 4 7.28 7.28 922 918 460 460
  • 5. Civil and Environmental Research www.iiste.org ISSN 2224-5790 (Paper) ISSN 2225-0514 (Online) Vol.6, No.8, 2014 Figure (3): Relation between discharge and aeration efficiency for case No.1 model No.2 Figure (4): Relation between discharge and aeration efficiency for case No.1 model No.3 Figure (5): Relation between discharge and aeration efficiency for case No.1 model No.4 15
  • 6. Civil and Environmental Research www.iiste.org ISSN 2224-5790 (Paper) ISSN 2225-0514 (Online) Vol.6, No.8, 2014 Figure (6): Relation between discharge and aeration efficiency for case No.2 model No.1 Figure (7): Relation between aeration efficiency - discharge for case No.2 model No.2 Figure 8 represent a comparison between Aeration efficiency E20 for case 1,2 for s/h=0.4, and figure 9 represent a comparison between Aeration efficiency E20 for case 1,2 for s/h=0.5. From figures it is clear that case 1 is most efficient than case 2 and case 1 model 4 is most efficient than the other models. Figure (8): Aeration efficiency- discharge relationship for s/h=0.4 for case No.1 model No.3 and case No.2 model No.1 16
  • 7. Civil and Environmental Research www.iiste.org ISSN 2224-5790 (Paper) ISSN 2225-0514 (Online) Vol.6, No.8, 2014 Figure (9 ): Aeration efficiency - discharge relationship for s/h=0.5 for case No.1 model No.4 and case No.2 model No.2 An empirical correlation predicting oxygen transfer efficiency was developed for stepped cascade. The resulting correlation is given in equation 4: E20=(0.108+2.499*(s/l)1.329/2.69*10-11*(l/h)-22.053*(F* )0.701) (4); correlation coefficient=85% where h is the step height (m), l is the step length (m), and F is Froude number , s end sill height (m). The measured oxygen transfer efficiencies were compared to those predicted with equation 4. Good agreement between the measured oxygen transfer efficiencies and the values computed from the predictive equation was obtained. 5-Conclusions Set of laboratory experiments have been carried out continuously on stepped cascade with end sill in order to determine aeration performance. An empirical correlation has been developed that predicted the oxygen transfer efficiency for stepped cascade. Based on the findings of this study, the following conclusions can be drawn: • Nappe flow was observed for all cases and the aeration efficiency of stepped chute with end sill increased with discharge • For stepped cascade with end sill, the aeration efficiency increased as chute inclination angle increased. • Additional testing is necessary to assess the effect of aeration efficiency for stepped cascade with end sill when discharge is higher than the largest discharge tested, 4 l/s. • The COD is an effective factor in aeration efficiency and as COD increases , the aeration efficiency decreased because of pollutant effect of marginal water (COD) References A. Baylar . (2010)" Hydraulic Structures in Water Aeration Processes " Water Air Soil Pollut 210:87–100 Baylar, A., & Emiroglu, M. E. (2003b). Study of aeration efficiency at stepped channels. Proceedings of the Institution of Civil Engineers—Water & Maritime Engineering, 156(WM3), 257–263. Baylar, A., & Emiroglu, M. E. (2005). Closure of 'Study of aeration efficiency at stepped channels. Proceedings of the Institution of Civil Engineers—Water Management, 158 (WM2), 89–90. Baylar, A., Bagatur, T., & Emiroglu, M. E. (2007a). Aeration efficiency with nappe flow over stepped cascades. Proceedings of the Institution of Civil Engineers—Water Management, 160(1), 43–50. Baylar, A., Bagatur, T., & Emiroglu, M. E. (2007b). Prediction of oxygen content of nappe, transition and skimming flow regimes in stepped channel chutes. Journal of Environmental Engineering and Science, 6(2), 201–208. Chamani MR, Rajaratnam N. 1994. Jet flow on stepped spillways. J. Hydraul. Eng. 120(2):254–259. Chamani MR, Rajaratnam N. 1999a. Characteristics of skimming flow over stepped spillways. J. Hydraul. Eng. 17 125(4):361–368. Chamani MR, Rajaratnam N. 1999b. Onset of skimming flow on stepped spillways. J. Hydraul. Eng. 125(9):969–971. Chanson H. 1994a. Comparison of energy dissipation between nappe and skimming flow regimes on stepped chutes. J. Hydraul. Res. 32(2):213–218.
  • 8. Civil and Environmental Research www.iiste.org ISSN 2224-5790 (Paper) ISSN 2225-0514 (Online) Vol.6, No.8, 2014 Chanson H. 1994b. Hydraulics of skimming flows over stepped channel and spillways. J. Hydraul. Res. 18 32(3):445–460. Chanson H. 1996. Prediction of the transition nappe/skimming flow on a stepped channel. J. Hydraul. Res. 34(3):421–429. Chanson, H., & Toombes, L. (2000). Discussion of Stream reaeration in nonuniform flow: Macroroughness enhancement. Journal of Hydraulic Engineering ASCE, 126(3), 222–224. Chanson, H., & Toombes, L. (2002). Experimental study of gas−liquid interfacial properties in a stepped cascade flow. Environmental Fluid Mechanics, 2(3), 241–263. Emiroglu, M. E., & Baylar, A. (2003a). An investigation of effect of stepped chutes with end sill on aeration performance. Water Quality Research Journal of Canada, 38(3), 527–539. Essery, I. T. S., Tebbutt, T. H. Y., & Rasaratnam, S. K. (1978). Design of spillways for reaeration of polluted waters, Rep. 72. London: CIRIA. Gulliver JS, Thene JR, Rindels AJ. 1990. Indexing gas transfer in self-aerated flows. J. Environ. Eng. 116(3):503–523. Gulliver JS, Wilhelms SC. 1992. Discussion of ‘Aeration at Ohio River basin navigation dams’, by Railsback SF, Bownds JM, Sak MJ, Stevens MM, Taylor GH. J. Environ. Eng. 108(3):444–446. Lewis WK, Whitman WG. 1924. Principles of gas absorption. Ind. Eng. Chem. 16(12):1215–1220. McGhee TJ. 1991. Water supply and sewerage. McGraw-Hill International Editions, 6th ed Metcalf and Eddy, Inc. (2003). "Wastewater Engineering Treatment and Reuse." International ed. McGraw Hill, New York. Novak, P. (1994). Improvement of water quality in rivers by aeration at hydraulic structure. In M. Hino (Ed.), Water quality and its control. Madrid: International Association of Hydraulic Research. Rajaratnam N. 1990. Skimming flow in stepped spillways. J. Hydraul. Eng. 116(4): 587–591. Tebbutt, T. H. Y., Essery, I. T. S., & Rasaratnam, S. K. (1977). Reaeration performance of stepped cascades. Journalof the Institution of Water Engineering Science, 31(4), 285–297. Toombes, L., & Chanson, H. (2000). Air−water flow and gas transfer at aeration cascades: a comparative study of smooth and stepped chutes (pp. 77–84). Zurich, Switzerland: Proceedings of the International Workshop on Hydraulics of Stepped Spillways. Wormleaton PR, Soufiani E. 1998. Aeration performance of triangular platform labyrinth weirs. J. Environ. Eng. 124(8):709–719. Y. B. M. Heza1, M. El-din , N. S. Donia and A. M. Refaat "Water Quality Improvement of Drains Polluted by Wastewaters Using Conventional Weir" Twelfth International Water Technology Conference , IWTC12 2008, Alexandria, Egypt.
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