Labyrinth weirs are complex hydraulic structures. They have been widely used as a water regulator and to increase discharge in channels and spillway dams. Labyrinth weirs are an economical and effective method to pass large floods. In addition, they are used to reduce the requirements of the structural footprint. These features make them an interesting and appropriate choice to increase the capacity of discharge. Several factors affect the discharge capacity and the hydraulic performance of labyrinth weirs, including water level to crest height ratio, angle of sidewalls, apex width, conveyance channel conditions, and vertical aspect ratio. The present paper aims to summarise the most relevant knowledge of the hydraulic characteristics of the labyrinth weirs reported in previous articles. The importance of the present study is to provide a better understanding of how these weirs operate, in addition to which future studies deserve further investigation. The results demonstrated that some parameters still need further investigation. Also, energy dissipation over the labyrinth weir needs further investigation with different weir geometry. Furthermore, the results showed that common design equations did not take into account all parameters affecting labyrinth weir performance, including geometries, flow conditions, site conditions, and scale effect. In addition, machine learning techniques need further study.

  • The highlights of this review article are as follows:

  • • The physical modelling was reviewed.

  • • The numerical modelling was reviewed.

  • • The design methods of labyrinth weirs were reviewed.

  • • Machine learning techniques were reviewed.

  • • The present review article provides a scope of future works of labyrinth weirs.

Graphical Abstract

Graphical Abstract

The following symbols are utilised in the present study:

A/w

length of apex geometry to the width of a single cycle/Apex ratio

A

Inside apex width

AI

artificial intelligent

ANFIS

Adaptive neuro-fuzzy inference system

ANN

Artificial neural networks

APE

Average percentage error

Aw

Sidewall area of the weir

B

Length of labyrinth weir

BNN

Bayesian neural network

BPNN

Back propagation neural network

Cd

Coefficient of discharge

CHAID

Chi-squared automatic interaction detector

D

Outside apex width

ELM

Extreme learning machine

Fr

Froude number

g

Gravity acceleration

GA-BPNN

Genetic algorithm and back propagation neural network

GEP

Gene expression programming

GP

Genetic programming

h

Flow depth over the weir crest

Ht /P

Headwater ratio

Ht

Total head over the weir crest

Lc/W

Magnification ratio

Lc

Total centerline length of labyrinth weir

LSSVM

Least square support vector machine

MAE

Mean absolute error

MAPE

Mean absolute percentage error

ME

Mean error

MLPNN

Multilayer perceptron neural network

MLR

Multiple linear regression

N

Number of labyrinth weir cycles

NLR

Nonlinear regression analysis

NN

Neural network

NSC

Nash–Sutcliffe efficiency coefficient

P

Weir height

Q

Discharge over the weir

PSO-BPNN

Particle swarm optimization and back propagation neural network

R2

Determination coefficient

Rcrest

Radius of crest shape

RF

Random forests

RMSE

Root mean square error

SAELM

Self-adaptive extreme learning machine

SVM

Support vector machine

TW

Sidewall thickness

tw

Thickness of weir wall

w/p

Aspect ratio

w

Single labyrinth weir cycle width

W

Channel width

α/θ

Angle ratio

α

Sidewall angle

θ

Vortex angle

Labyrinth weirs play a significant role in passing floods upstream with a low water level. Labyrinth weirs became widely used around the world because of their reduced structural costs. These types of weirs are often utilised to limit the width of the weir to decrease maximal upstream water depth. Generally, labyrinth weirs are described by no linear plan forms such as triangular, rectangular, or trapezoidal shapes (see Figure 1). This configuration increases the weir length. The flow over a labyrinth weir is higher than that of a linear weir of the same upstream head and weir width (Crookston 2010). The trapezoidal and triangular-shaped labyrinth weirs give better hydraulic performance than the rectangular shape of the labyrinth weirs, and these types of weirs can be applied in many various field applications. Thus, there is great interest in their design and construction. Enhancing weir hydraulic performance usually needs physical model experimentation because many dimensional parameters influence the capacity of discharge over the labyrinth weirs.
Figure 1

Shapes of labyrinth weirs: (a) rectangular, (b) triangular, and (c) trapezoidal (Crookston 2010).

Figure 1

Shapes of labyrinth weirs: (a) rectangular, (b) triangular, and (c) trapezoidal (Crookston 2010).

Close modal

Ghare et al. (2008) showed that as a result of the ingrained benefits of labyrinths regarding magnification of the flow and stability of the structure, it should remain to be utilised to a larger extent for future projects. Therefore, labyrinth weirs have a basic role in guaranteeing the security of human life. In addition, labyrinth weirs save developing regions and natural environment safety. Because of their high efficiency, labyrinth weirs have become increasingly popular in recent years., especially in weirs rehabilitation schemes with limited channel width or for weirs constructed near a populated area. The hydraulics of labyrinth weirs have drawn a great deal of interest. Also, several methods for hydraulic design of the labyrinth weirs have been developed (Paxson et al. 2011).

Paxson et al. (2011) diagnosticated hydraulic characteristics of labyrinth weirs to deliver higher discharge than linear weirs for the same water level. The labyrinth weir is suitable for sites where increasing water surface elevation in a reservoir and higher discharge capacities are required and the weir width would be restricted (Khode & Tembhurkar 2010). Houston (1982) showed that labyrinth weirs are suitable for the rehabilitation of spillway dams. Labyrinth weirs have become the preferred choice for engineers and designers (Paxson & Savage 2006). The hydraulic complexity of these weirs has resulted from the geometrics, approach conditions, tailwater, headwater and other performance features. Paxson et al. (2011) showed that labyrinth weirs need further investigation and existing doubts regarding their functionality and usefulness need to be addressed. Total head (Ht) and the discharge coefficient Cd are the main parameters that affect the discharge capacity of labyrinth weirs. Several variables of the geometry of labyrinth weirs affect the coefficient of discharge Cd, including the effective length of a crest (L), the width of the weir (W), the weir height (P), the shape of a crest in planform, the shape of the apex, sidewall angle (α), head over the crest (h), cycle number (N) and thickness of sidewall (t) of the labyrinth weir. Figure 2 shows labyrinth weir geometries.
Figure 2

The geometric labyrinth weir parameters. (a) Labyrinth weir plan, (b) types of crest shapes, (c) cross-section AA (Crookston 2010).

Figure 2

The geometric labyrinth weir parameters. (a) Labyrinth weir plan, (b) types of crest shapes, (c) cross-section AA (Crookston 2010).

Close modal

Labyrinth weirs were utilised as regular structures for flow and also help control aeration, drop structures, and energy dissipation. Emiroglu & Baylar (2005) showed that labyrinth weirs are utilised to improve air entrainment flow proficiency. While Emiroglu et al. (2010) found that the labyrinth weirs are a good choice as side weirs to increase the discharge. There are several types of studies for labyrinth weirs that contributed to providing knowledge regarding hydraulic behaviour and design methods for this type of weir, such as (Lux 1984; Wormleaton & Soufiani 1998; Wormleaton & Tsang 2000; Emiroglu & Baylar 2005; Tullis et al. 2005; Tullis et al. 2007; Crookston & Tullis 2011a, 2011b, 2012a, 2012b, 2012c; Khode et al. 2011; Kumar et al. 2011; Crookston et al. 2012a; Dabling et al. 2013; Gupta & Singh 2013; Akoz et al. 2014; Crookston et al. 2014; Bahrebar et al. 2016; Baeimani & Bajestan 2015; Kanyabujinja 2015; Idrees & Al-Ameri 2022). Table 1 shows a summary of some previous studies related to labyrinth weirs.

Table 1

Summary of some previous studies related to labyrinth weirs

StudyPurposeLimitationsPlace of experimentResults
Houston (1982)  They investigated the possibility of replacing the Ute dam spillway with the labyrinth weir to increase the discharge • A flume dimensions 0.76 m wide, 0.61 m deep, and 10.97 m long.
• α = 45°
• sharp crest weir
• Scale model = 1:80
• 2 ≤ l/w ≤ 5 
Experimental investigation They found that labyrinth weirs are a good choice for the rehabilitation of spillway structures 
Wormleaton & Soufiani (1998)  They investigated effect the of aeration on a triangular labyrinth weir performance • Half-round crest
• Triangular labyrinth weir shape with θ = 30°, 45°, 60°, 90°, 120°, and 180°
• Weir width W (83–320) mm
• Discharge Q varied between 1.0 and 4.0 L/s 
Experimental investigation They demonstrated that the labyrinth weirs were better at the efficiency of the aeration than the same length of the linear weirs 
Wormleaton & Tsang (2000)  They investigated increasing the aeration process using a rectangular labyrinth weir by creating turbulence downstream • Sharp-crested weirs
• Discharge Q varied between 1 and 4.3 L/s
• Rectangular labyrinth weir
• Length of weir Lc = 240 and 150 mm 
Experimental investigation They showed that the labyrinth weirs are significantly better at the efficiency of the aeration than a straight weir. Also, they found regression equations relating to aeration efficiency 
Emiroglu & Baylar (2005)  They investigated the effect of the sill slope and angle of a triangular labyrinth on the aeration rate • A flume dimension is 3.40 m long, 0.60 m wide, and 0.50 m deep
• Triangular labyrinth weir shape
• θ = 45°, 90°, 135°, 180°
• Weir width w = 11.48, 21.21, 27.72, and 30 cm
• Flow rate = 4 L/ s
• The slope of sill (ϕ) changes from 0° to 45° 
Experimental investigation The authors found that a triangular labyrinth weir has a better aeration rate than a straight weir. Also, they found regression equations relating the aeration rate to weir discharge and drop height 
Tullis et al. (2005)  They investigated the possibility of replacing the existing gated spillway with the labyrinth weir to increase the discharge • A flume size is 1.22 m wide, 0.91 m deep and 7.3 m long
• Sidewall angles (α) are 7°, 8°
• Crest shapes are ogee, quarter-round, half-round crest
• Trapezoidal labyrinth weir 
Experimental investigation They found that a sidewall angle of 8° for a labyrinth weir with an ogee-type crest was the more efficient design for a labyrinth weir spillway 
Paxson and Savage (2006)  They applied Lux and Tullis design methods and compared them with the software Flow-3D model to develop the Hyrum Dam spillway • Aspect ratio W/P < 2 Experimental and numerical tests The results proved that the effects of aspect ratios W/P were lower than the least values which were used by the Lux and Tullis design method 
Tullis et al. (2007)  They developed new relationships of head discharge for submerged labyrinth weirs • A flume size 7.3 m long, 1.22 m wide, and 0.91 m deep
• Sidewall angles (α) are 7°, 8°, and 20°
• H* = Hd where 3.5 ≤ Hd/Ho 
Experimental investigation The authors found that the relationship of the new submerged dimensionless (H* /Ho versus Hd /Ho) was more precise than that found in Villemonte's relationship 
Ghare et al. (2008)  They applied a mathematical model to find the optimal discharge coefficient of the labyrinth weir • α = 6°, 8°, 12°, 15°, 18°, 25°, 35°, and 90°
• w/P range between 2 and 4
• The thickness of the crest wall ranges from 1 t to 2 t 
Experimental investigation The results showed that the new proposed methodology was efficient for the hydraulic design of labyrinth weirs 
Khode and Tembhurkar (2010)  They evaluated Lux and Tullis methods for designing labyrinth weirs with different vertical aspect ratios w/p • w/p ≥ 2 for trapezoidal labyrinth weir
• w/p ≥ 2.5 for triangular labyrinth weir 
Experimental investigation Authors found that the vertical aspect ratio (w/p) should not be less than 2 for trapezoidal labyrinth weir and should not be less than 2.5 for triangular labyrinth weir 
Emiroglu et al. (2010)  They investigated increased the discharge capacity of labyrinth side weirs • The main channel is 0.50 m wide, 12 m long, and 0.50 m deep
• Bed slope = 0.001
• A triangular labyrinth side weir
• θ = 45°, 60°, 90°, 120°, and 150° 
Experimental investigation The results showed that the discharge coefficient of labyrinth side weirs produced a higher coefficient value than classical side weirs. Also, they found a reliable equation for the discharge coefficient. The discharge coefficient of the labyrinth side weir was 1.5–4.5 times bigger than the rectangular side weir 
Crookston & Tullis (2011a)  They investigated the effects of specific parameters such as flush, projecting, arced labyrinth weirs, and rounded inlets on hydraulic performance • Half-round crest shape,
• Dimensions test tank 7.3 m long, 6.7 m wide and 1.5 m deep
• Half-round crest
• α = 12°, θ = 10°
• Trapezoidal labyrinth weir 
Experimental investigation The outcomes presented that the discharge efficiency for the arced labyrinth weir was 5–11% more than an in-channel labyrinth weir 
Crookston & Tullis (2011b)  They developed a hydraulic analysis and design method of the labyrinth weirs • Flume size 1.0 m deep, 1.2 m wide, and 14.6 m long
• Quarter-round crest
• 6° ≤ α ≤ 35° 
Experimental investigation The results showed that discharge coefficient values obtained from their study could be replaced with the values obtained by the Tullis et al. (1995) design method 
Kumar et al. (2011)  They investigated the discharge capacity of the sharp-crested triangular weir • Flume size 12 m long, 0.28 m wide and 0.41 m deep
• θ = 30°, 60°, 90°, 120°, 150° and 180°
• Triangular labyrinth weir 
Experimental investigation The results showed that the triangular weir was more efficient than the normal weir. They found an equation to estimate discharge with an accuracy of ±5% of the observed data 
Khode et al. (2011)  They investigated the coefficient of discharge for a trapezoidal labyrinth weir with different side wall angles • Laboratory flume 0.5 m wide by 0.5 m deep by 3.4 m long
• 6° ≤ α ≤ 30°
• Quarter-round crest 
Experimental investigation The results found that the discharge coefficient was the minimum value for sidewall angle 6. Also, the accuracy of the crest coefficient value between the prototype dam and that estimated by the present study was ± 5% 
Crookston & Tullis (2012b)  They provided new information related to the hydraulic performance of trapezoidal labyrinth weir designs. This information pertains to nappe vibrations, nappe behaviour, nappe ventilation, and nappe instability • Flume size 1.0 m deep, 1.2 m wide, and 14.6 m long
• 6° ≤ α ≤ 35°
• Trapezoidal labyrinth weir
• Quarter-round and half-round crests 
Experimental investigation The results showed that the labyrinth weir was more efficient for a clinging nappe condition. For quarter-round crest shapes, the effect of artificial aeration on the capacity of discharge can be negligible compared with the non-vented. The hydraulic performance of the half-round crest labyrinth weir was similar to the quarter-round crest when artificial aerated is vented 
Crookston & Tullis (2012a)  They presented an analysis and design of trapezoidal labyrinth weirs • Flume size 1.0 m deep, 1.2 m wide, and 14.6 m long
• 6° ≤ α ≤ 35°
• Trapezoidal labyrinth weir
• Quarter-round and half-round crests 
Laboratory investigation The results demonstrated the procedure for the design and analysis of a labyrinth weir. They use cycle efficiency as a tool for testing discharge capacity 
Crookston & Tullis (2012c)  They investigated the effect of nappe interference on the capacity of discharge and identified flow characteristics, including local submergence • Flume size 1.0 m deep, 1.2 m wide, and 14.6 m long
• 6° ≤ α ≤ 35°
• Trapezoidal labyrinth weir
• Quarter-round and half-round crests 
Laboratory investigation The results presented the nappe interference region as a function of weir geometry 
Crookston et al. (2012a)  They tested the performance of hydraulics for labyrinth weirs when headwater ratios were greater than 1 • Flume size 1.0 m deep, 1.2 m wide, and 14.6 m long
• Quarter-round crests
• Trapezoidal labyrinth weir
• α = 15° 
Numerical and experimental tests The outcomes presented that a set of design curves obtained by Crookston in 2010 were suitable for headwater ratios up to 2.0 
Dabling et al. (2013)  They evaluated the characteristics of discharge for different-staged labyrinth weirs • Flume size 1.0 m deep, 1.2 m wide, and 14.6 m long
• Quarter-round crests
• Trapezoidal labyrinth weir
• α = 15° 
Experimental investigation The results found that predictive error was up to 20% for discharge over the lower stage (notch) 
Crookston et al. (2014)  They studied nappe vibration, including physical processes and applicable mitigation methods • The smaller weir model is 1.2 m high, 1.8 m wide, and 76 mm thick
• The larger prototype-scale model is 3.3 m high by 4.7 m wide with the crest 0.3 m thick 
Experimental investigation The results observed that nappe vibration was generated when nappe flow was fully vented. Also, nappe breakers were a less suitable mitigation option 
Bahrebar et al. (2016)  They investigated the hydraulic performance of the new shape of labyrinth weirs • Flume size 0.40 m deep, 8 m long, and 0.35 m wide
• Triangular labyrinth weir 
Experimental investigation The results showed that discharge coefficients are reduced when wing length increases Furthermore, the coefficient of discharge for triangular labyrinth weirs is greater than that of linear weirs 
Idrees & Al-Ameri (2022)  They investigated using artificial ventilation methods to improve the hydraulic performance of compound labyrinth weirs • Flume size 0.6 m deep, 0.5 m wide, and 7 m long
• Half-round crests
• Trapezoidal labyrinth weir
• α = 10° 
Experimental investigation The results demonstrated that the suction pump method was the better device for artificial ventilation compared to the vent pipe method. The suction and vent devices produced a higher compound discharge coefficient than without utilising the artificial ventilation devices by 10% and 4.5%, respectively. They provided an empirical equation for predicting the compound discharge coefficient 
StudyPurposeLimitationsPlace of experimentResults
Houston (1982)  They investigated the possibility of replacing the Ute dam spillway with the labyrinth weir to increase the discharge • A flume dimensions 0.76 m wide, 0.61 m deep, and 10.97 m long.
• α = 45°
• sharp crest weir
• Scale model = 1:80
• 2 ≤ l/w ≤ 5 
Experimental investigation They found that labyrinth weirs are a good choice for the rehabilitation of spillway structures 
Wormleaton & Soufiani (1998)  They investigated effect the of aeration on a triangular labyrinth weir performance • Half-round crest
• Triangular labyrinth weir shape with θ = 30°, 45°, 60°, 90°, 120°, and 180°
• Weir width W (83–320) mm
• Discharge Q varied between 1.0 and 4.0 L/s 
Experimental investigation They demonstrated that the labyrinth weirs were better at the efficiency of the aeration than the same length of the linear weirs 
Wormleaton & Tsang (2000)  They investigated increasing the aeration process using a rectangular labyrinth weir by creating turbulence downstream • Sharp-crested weirs
• Discharge Q varied between 1 and 4.3 L/s
• Rectangular labyrinth weir
• Length of weir Lc = 240 and 150 mm 
Experimental investigation They showed that the labyrinth weirs are significantly better at the efficiency of the aeration than a straight weir. Also, they found regression equations relating to aeration efficiency 
Emiroglu & Baylar (2005)  They investigated the effect of the sill slope and angle of a triangular labyrinth on the aeration rate • A flume dimension is 3.40 m long, 0.60 m wide, and 0.50 m deep
• Triangular labyrinth weir shape
• θ = 45°, 90°, 135°, 180°
• Weir width w = 11.48, 21.21, 27.72, and 30 cm
• Flow rate = 4 L/ s
• The slope of sill (ϕ) changes from 0° to 45° 
Experimental investigation The authors found that a triangular labyrinth weir has a better aeration rate than a straight weir. Also, they found regression equations relating the aeration rate to weir discharge and drop height 
Tullis et al. (2005)  They investigated the possibility of replacing the existing gated spillway with the labyrinth weir to increase the discharge • A flume size is 1.22 m wide, 0.91 m deep and 7.3 m long
• Sidewall angles (α) are 7°, 8°
• Crest shapes are ogee, quarter-round, half-round crest
• Trapezoidal labyrinth weir 
Experimental investigation They found that a sidewall angle of 8° for a labyrinth weir with an ogee-type crest was the more efficient design for a labyrinth weir spillway 
Paxson and Savage (2006)  They applied Lux and Tullis design methods and compared them with the software Flow-3D model to develop the Hyrum Dam spillway • Aspect ratio W/P < 2 Experimental and numerical tests The results proved that the effects of aspect ratios W/P were lower than the least values which were used by the Lux and Tullis design method 
Tullis et al. (2007)  They developed new relationships of head discharge for submerged labyrinth weirs • A flume size 7.3 m long, 1.22 m wide, and 0.91 m deep
• Sidewall angles (α) are 7°, 8°, and 20°
• H* = Hd where 3.5 ≤ Hd/Ho 
Experimental investigation The authors found that the relationship of the new submerged dimensionless (H* /Ho versus Hd /Ho) was more precise than that found in Villemonte's relationship 
Ghare et al. (2008)  They applied a mathematical model to find the optimal discharge coefficient of the labyrinth weir • α = 6°, 8°, 12°, 15°, 18°, 25°, 35°, and 90°
• w/P range between 2 and 4
• The thickness of the crest wall ranges from 1 t to 2 t 
Experimental investigation The results showed that the new proposed methodology was efficient for the hydraulic design of labyrinth weirs 
Khode and Tembhurkar (2010)  They evaluated Lux and Tullis methods for designing labyrinth weirs with different vertical aspect ratios w/p • w/p ≥ 2 for trapezoidal labyrinth weir
• w/p ≥ 2.5 for triangular labyrinth weir 
Experimental investigation Authors found that the vertical aspect ratio (w/p) should not be less than 2 for trapezoidal labyrinth weir and should not be less than 2.5 for triangular labyrinth weir 
Emiroglu et al. (2010)  They investigated increased the discharge capacity of labyrinth side weirs • The main channel is 0.50 m wide, 12 m long, and 0.50 m deep
• Bed slope = 0.001
• A triangular labyrinth side weir
• θ = 45°, 60°, 90°, 120°, and 150° 
Experimental investigation The results showed that the discharge coefficient of labyrinth side weirs produced a higher coefficient value than classical side weirs. Also, they found a reliable equation for the discharge coefficient. The discharge coefficient of the labyrinth side weir was 1.5–4.5 times bigger than the rectangular side weir 
Crookston & Tullis (2011a)  They investigated the effects of specific parameters such as flush, projecting, arced labyrinth weirs, and rounded inlets on hydraulic performance • Half-round crest shape,
• Dimensions test tank 7.3 m long, 6.7 m wide and 1.5 m deep
• Half-round crest
• α = 12°, θ = 10°
• Trapezoidal labyrinth weir 
Experimental investigation The outcomes presented that the discharge efficiency for the arced labyrinth weir was 5–11% more than an in-channel labyrinth weir 
Crookston & Tullis (2011b)  They developed a hydraulic analysis and design method of the labyrinth weirs • Flume size 1.0 m deep, 1.2 m wide, and 14.6 m long
• Quarter-round crest
• 6° ≤ α ≤ 35° 
Experimental investigation The results showed that discharge coefficient values obtained from their study could be replaced with the values obtained by the Tullis et al. (1995) design method 
Kumar et al. (2011)  They investigated the discharge capacity of the sharp-crested triangular weir • Flume size 12 m long, 0.28 m wide and 0.41 m deep
• θ = 30°, 60°, 90°, 120°, 150° and 180°
• Triangular labyrinth weir 
Experimental investigation The results showed that the triangular weir was more efficient than the normal weir. They found an equation to estimate discharge with an accuracy of ±5% of the observed data 
Khode et al. (2011)  They investigated the coefficient of discharge for a trapezoidal labyrinth weir with different side wall angles • Laboratory flume 0.5 m wide by 0.5 m deep by 3.4 m long
• 6° ≤ α ≤ 30°
• Quarter-round crest 
Experimental investigation The results found that the discharge coefficient was the minimum value for sidewall angle 6. Also, the accuracy of the crest coefficient value between the prototype dam and that estimated by the present study was ± 5% 
Crookston & Tullis (2012b)  They provided new information related to the hydraulic performance of trapezoidal labyrinth weir designs. This information pertains to nappe vibrations, nappe behaviour, nappe ventilation, and nappe instability • Flume size 1.0 m deep, 1.2 m wide, and 14.6 m long
• 6° ≤ α ≤ 35°
• Trapezoidal labyrinth weir
• Quarter-round and half-round crests 
Experimental investigation The results showed that the labyrinth weir was more efficient for a clinging nappe condition. For quarter-round crest shapes, the effect of artificial aeration on the capacity of discharge can be negligible compared with the non-vented. The hydraulic performance of the half-round crest labyrinth weir was similar to the quarter-round crest when artificial aerated is vented 
Crookston & Tullis (2012a)  They presented an analysis and design of trapezoidal labyrinth weirs • Flume size 1.0 m deep, 1.2 m wide, and 14.6 m long
• 6° ≤ α ≤ 35°
• Trapezoidal labyrinth weir
• Quarter-round and half-round crests 
Laboratory investigation The results demonstrated the procedure for the design and analysis of a labyrinth weir. They use cycle efficiency as a tool for testing discharge capacity 
Crookston & Tullis (2012c)  They investigated the effect of nappe interference on the capacity of discharge and identified flow characteristics, including local submergence • Flume size 1.0 m deep, 1.2 m wide, and 14.6 m long
• 6° ≤ α ≤ 35°
• Trapezoidal labyrinth weir
• Quarter-round and half-round crests 
Laboratory investigation The results presented the nappe interference region as a function of weir geometry 
Crookston et al. (2012a)  They tested the performance of hydraulics for labyrinth weirs when headwater ratios were greater than 1 • Flume size 1.0 m deep, 1.2 m wide, and 14.6 m long
• Quarter-round crests
• Trapezoidal labyrinth weir
• α = 15° 
Numerical and experimental tests The outcomes presented that a set of design curves obtained by Crookston in 2010 were suitable for headwater ratios up to 2.0 
Dabling et al. (2013)  They evaluated the characteristics of discharge for different-staged labyrinth weirs • Flume size 1.0 m deep, 1.2 m wide, and 14.6 m long
• Quarter-round crests
• Trapezoidal labyrinth weir
• α = 15° 
Experimental investigation The results found that predictive error was up to 20% for discharge over the lower stage (notch) 
Crookston et al. (2014)  They studied nappe vibration, including physical processes and applicable mitigation methods • The smaller weir model is 1.2 m high, 1.8 m wide, and 76 mm thick
• The larger prototype-scale model is 3.3 m high by 4.7 m wide with the crest 0.3 m thick 
Experimental investigation The results observed that nappe vibration was generated when nappe flow was fully vented. Also, nappe breakers were a less suitable mitigation option 
Bahrebar et al. (2016)  They investigated the hydraulic performance of the new shape of labyrinth weirs • Flume size 0.40 m deep, 8 m long, and 0.35 m wide
• Triangular labyrinth weir 
Experimental investigation The results showed that discharge coefficients are reduced when wing length increases Furthermore, the coefficient of discharge for triangular labyrinth weirs is greater than that of linear weirs 
Idrees & Al-Ameri (2022)  They investigated using artificial ventilation methods to improve the hydraulic performance of compound labyrinth weirs • Flume size 0.6 m deep, 0.5 m wide, and 7 m long
• Half-round crests
• Trapezoidal labyrinth weir
• α = 10° 
Experimental investigation The results demonstrated that the suction pump method was the better device for artificial ventilation compared to the vent pipe method. The suction and vent devices produced a higher compound discharge coefficient than without utilising the artificial ventilation devices by 10% and 4.5%, respectively. They provided an empirical equation for predicting the compound discharge coefficient 

Labyrinth weirs seem a complex structure. This structure consists of a large set of parameters. Many studies relating to labyrinth weir geometry have described the impact of various parameters on rates of flow and discharge efficiency when passing over these types of weirs. Cassidy et al. (1985) used a physical model to investigate discharge capacity. Their results demonstrated that labyrinth weirs were less efficient than in models presented in the literature. Falvey (2003) reviewed previous studies on labyrinth weirs and revealed the most important variables of a labyrinth weir, such as the total head to the height of the weir ratio, sidewall angle, and magnification of length ratio. Ghare et al. (2008) adopted physical models and used regression analysis for the hydraulic design of a labyrinth weir. They found an empirical model to find the optimal value of the discharge coefficient for labyrinth weirs as shown in Figure 3. Equation (1) was proposed for calculating the flow rate over a labyrinth weir:
(1)
where Q is the flow capacity of the labyrinth weir, H is the total head over the labyrinth weir, P is the weir height, Lc is the weir length, and g is gravity. Ghodsian (2009) utilised the dimensional analysis method to estimate the flow rate of a triangular labyrinth weir given by Equation (2). Figure 4 shows the different dimensionless parameters of K/P against H/P for a triangular labyrinth weir:
(2)
where Q is the flow rate, L is the length of the crest for one cycle, H is the total head, w is one cycle width, P is the height of the labyrinth weir, and g is gravity. Crookston & Tullis (2010) included experimental outcomes for 8-degree sidewall angles, verifying the error in the original method, which was recommended by Tullis et al. (1995).
Figure 3

Optimal coefficient of discharge. Ghare et al. (2008).

Figure 3

Optimal coefficient of discharge. Ghare et al. (2008).

Close modal
Figure 4

Variations dimensionless parameter of K/P against H/P for a triangular labyrinth weir Ghodsian (2009).

Figure 4

Variations dimensionless parameter of K/P against H/P for a triangular labyrinth weir Ghodsian (2009).

Close modal
Khode et al. (2011) discussed the relevance between the discharge coefficient and H/P (total head to the height of the weir) of the labyrinth weir. A resulting chart showed the relationship between coefficients of discharge with H/P for various sidewall angles. The impact of three-dimensional flow caused a decrease in the discharge coefficient as the sidewall angle decreased. Figure 5 shows the discharge coefficient against Ht/P for different sidewall angles.
Figure 5

The discharge coefficient versus Ht/P for different sidewall angles of trapezoidal labyrinth weir (Khode et al. 2011).

Figure 5

The discharge coefficient versus Ht/P for different sidewall angles of trapezoidal labyrinth weir (Khode et al. 2011).

Close modal
Khode et al. (2012) investigated the flow characteristics of the labyrinth weirs. Different sidewall angles of 8° to 30° were used, and a chart with several design curves was plotted. The results represented the relationship between the discharge coefficient and H/P for sidewall angles of 8° to 30° as shown in Figure 6.
Figure 6

The discharge coefficient versus Ht/P for different sidewall angles of trapezoidal labyrinth weir Khode et al. (2012).

Figure 6

The discharge coefficient versus Ht/P for different sidewall angles of trapezoidal labyrinth weir Khode et al. (2012).

Close modal
Crookston et al. (2012b) examined sidewall angle α = 15°. They used trapezoidal labyrinth weirs for this purpose. The results showed that cycle efficiency decreased as the Ac/Lc ratio increased. The apex had the lowest impact on total discharge efficiency, as this was the larger impact on the total cycle length and caused decreases in sidewall length, thereby causing a decrease in total flow efficiency as shown in Figure 7. Also, as N increased (in the specified channel width) and remained constant, the overall crest length decreased. This also had a negative effect on the performance of labyrinth weirs hydraulically. Carollo et al. (2012) used five groups of physical models and adopted the empirical equation.
Figure 7

Cycle efficiency against HT/P for different sidewall angles of the labyrinth weirs Crookston et al. (2012b).

Figure 7

Cycle efficiency against HT/P for different sidewall angles of the labyrinth weirs Crookston et al. (2012b).

Close modal

Furthermore, Mirnaseri & Emadi (2014) tested physical models for rectangular labyrinth weirs and gates. They investigated the effect of the length and height of the labyrinth weir with different bed slopes of the flume on the discharge coefficient. The results demonstrated that the discharge coefficient of the combined model increased with increasing weir height. Data analysis demonstrated that increasing the effective length of the labyrinth weir when Ht/L was less than 0.03 led to an increase in the coefficient of discharge, while an Ht/L ratio of more than 0.03 led to a reduced coefficient of discharge in a combined model. Experimental outcomes for various flume slopes demonstrated that the coefficients of discharge of models increased with increasing flume slopes. The shape of the crest is the basic parameter that influences the hydraulic performance of the labyrinth weirs. Paxson & Savage (2006) showed that a rounded crest weir generally has a coefficient of discharge that is measurably higher than those of sharp and flat crest weirs. Amanian (1987) showed that the quarter-round crest was the more efficient shape. Also, Khode & Tembhurkar (2010) recommended the quarter-round crest. Labyrinth weirs with a half-round crest were more efficient for increasing discharge capacity.

Moreover, the choice of different geometric parameters, orientation, and position of the labyrinth weir affect the capacity of the discharge. Paxson et al. (2011) showed that flow conditions downstream of the labyrinth weir could also influence discharge capacity. The width of the inside apex defines whether the labyrinth weir is trapezoidal or triangular. Kumar et.al. (2012) investigated discharge capacity by using the sharp-crested curve under free-flow conditions. They proposed equations to estimate coefficients of discharge for curve labyrinth weirs. The results showed that discharge capacity was a gain of 40% for a curved weir compared to a normal weir. Kabiri & Javaheri (2012) investigated the flow coefficient for a rectangular labyrinth weir. The analytical method was based on the combination of the equations of a vertical and a lateral weir. This method is based on the determination of the contribution of each cited section (upstream b, downstream a, and lateral L). Gupta et al. (2013) studied the flow characteristics of a sharp-crested triangular labyrinth weir. The discharge efficiency across the triangular labyrinth weir was larger than the normal weir. The equation of flow was suggested for the given range of data and was within ±5% of the observed data. Ouamane & Lempèrière (2013) studied the rectangular labyrinth weir and found the rectangular shape more efficient than the trapezoidal shape. Gupta et al. (2014) studied W-planform weirs to determine discharge characteristics under free-flow conditions. The discharge efficiency of W-planform labyrinth weirs was higher than that of normal weirs. The equation of flow was suggested for the given range of data and was within ±5% of the observed data. Gupta et al. (2015) used 24 sharp crests of a labyrinth weir. A rectangular labyrinth weir was used to examine the effect of crest height on the discharge capacity for different crest lengths. The discharge efficiency of the rectangular labyrinth weir was higher than that of the normal weir. Idrees et al. (2016) discussed the effect of a range sidewall angle of 6° to 35° on the discharge coefficient for one cycle of a labyrinth weir. They developed a set of curves for estimating the discharge coefficient. Idrees et al. (2017) examined the hydraulic performance of compound labyrinth weirs. The compound labyrinth weir was located in normal and inverse orientations according to the flow direction. The outcomes demonstrated that the discharge coefficient values do not vary significantly when compared with the labyrinth weir orientations. Idrees et al. (2018) investigated the hydraulic characteristics of compound labyrinth weirs. They found empirical equations with a range of sidewall angles of 6° to 90° for estimating discharge coefficients.

Numerical modelling

Computational fluid dynamics (CFD) is a program that uses numerical methods for analysing and simulation (Institute for Water & Environmental Engineering 2012). Currently, CFD modelling has been widely utilised in water resources engineering applications by combining it with physical modelling. Versteeg & Malalasekera (1995) explained that CFD modelling is essential to the simulation of the problem rather than providing a final result. The CFD model can analyse hydraulic structures more cheaply than a physical model. Studies have investigated using CFD for verifying and refining the design of the labyrinth weir. Savage et al. (2004) compared physical models carried out by the USBR. They showed that current design approaches were deficient for different values of weir height (P). This resulted from using the design methods of Tullis et al. (1995) that depend on the HT/P ratio for finding the rating curve, which is influenced by the various P values. Savage et al. (2004) also observed that physical models were useful for verifying discharge and suggested using modelling of the CFD as an alternative method for reducing cost and time. They found good agreement with the physical model. Bhuiyan & Hey (2007) simulated experimental results for U-, V- and W-weir shapes. A positive correlation resulted from the calculated patterns of flow and the characteristics of the flow. Paxson et al. (2008) used CFD modelling to simulate the spillway for the Lake Townsend Dam. The results showed that the labyrinth weir was a suitable choice as a replacement gate for the spillway. A modified Tullis et al. (1995) method was applied to develop a discharge relationship for this proposed weir geometry, and the discharge coefficient estimated by this method was shown to be underestimated for low H/P ratios (less than 0.3).

Furthermore, to maintain safety at the Lake Holiday Dam in the State of Virginia, Ackers et al. (2011) utilised the hydraulic design equation that was recommended by Tullis et al. (1995) and examined the flow behaviour by utilising the CFD program. Holmquist-Johnson (2011) simulated the effect of alternative solutions for U-weir. The results explained that using U-weir geometry and flow patterns including stress, velocity distributions, bed shear and upstream flow depth, significant variations could be made. In addition, the author developed stage–discharge relationships by using results from the numerical model simulations. To compare with physical models, Torres et al. (2018) used two numerical models, including the ANSYS Fluent program and OpenFOAM. The results showed that the prediction data generated by the fluent model were more closely related to the physical model than those obtained by OpenFOAM. Carrillo et al. (2019) compared three different turbulence models through experimental work and CFD modelling. There was a positive correlation between the capacity of discharge in the cases of free discharge and submerged conditions. Idrees et al. (2022) simulated the flow behaviour of the compound labyrinth weir within three regions of flow depth. They used the CFD program for this purpose. The results showed that the streamlines were divided into two parts. Also, negative pressure behind the nappe flow was produced by air bubbles.

Machine learning methods

Recently, machine learning methods have been used to predict the discharge coefficient of weirs. These methods have also been used in modelling complex problems of hydraulic structures (Emiroglu & Kisi 2013). Machine learning techniques were investigated by several researchers, e.g. Roushangar et al. (2017) used gene expression programming (GEP) and adaptive neuro-fuzzy inference system (ANFIS) methods to predict the coefficient of discharge for labyrinth weirs. The results demonstrated that the ANFIS method was the best model for predicting the discharge coefficient. Roushangar et al. (2018) built a model to predict the coefficients of discharge for inverted and normal direction labyrinth weirs. They utilise support vector machine (SVM)-based models for this purpose. The results demonstrated that discharge coefficient prediction by the SVM-based model of arced labyrinth weir (ALW) was better solution when dimensionless parameters, e.g., angle ratio (α/θ), headwater ratio (HT/P), and magnification ratio (Lc/W) were used as input parameters. Furthermore, sensitivity analysis demonstrated that both parameters of the Froude number and headwater ratio were the most effective on the coefficient of discharge for normal labyrinth weirs, while for arced labyrinth weirs, both parameters of the angle ratio (α/θ) and headwater ratio were the most effective on coefficients of discharge. Karami et al. (2018) applied three models of intelligence techniques, including genetic programming (GP), extreme learning machine (ELM), and artificial neural networks (ANN) to predict the coefficient of discharge. The ELM model showed the best results for predicting discharge coefficients in comparison with the GP and ANN models. Salazar & Crookston (2019) applied the machine learning method to the analysis of arced labyrinth weirs geometrically. They used random forests (RF) and neural networks (NN) to estimate the coefficient of discharge. They demonstrated that RF and NN can be utilised as a unique representation for curve fitting. Norouzi et al. (2019) applied three models of the radial basis function networks, multilayer perceptron (MLP) networks, and support vector machines with various kernel functions to predict the coefficient of discharge (Cd) of labyrinth weirs. Moreover, the MLP model was more appropriate to predict the discharge coefficient. Dutta et al. (2020) built predictive models to compute the capacity of discharge for circular arc weirs and a multi-cycle labyrinth weir. They used an artificial neural network (ANN), multiple linear regression (MLR), and SVM. The results confirmed that the prediction made by the SVM regression model was more accurate than the ANN and MLR approaches. Norouzi et al. (2020) used the self-adaptive extreme learning machine (SAELM) artificial intelligence model to simulate the coefficient of discharge for a labyrinth weir. The results identified that dimensionless parameters such as (A/w) and (HT/P) were the most effective as input parameters. Wang et al. (2022) applied four methods of nonlinear regression analysis (NLR), the back propagation neural network (BPNN), the genetic algorithm (GA) BPNN (GA-BPNN), and the particle swarm optimization (PSO) BPNN (PSO-BPNN) to estimate the discharge coefficient of labyrinth weirs. The results showed that the predictions by the GA-BPNN and PSO-BPNN were better than the BPNN. The maximum error values with the discharge coefficient prediction by PSO-BPNN and GA-BPNN were 2.6% and 4.4%, respectively. They compared the results of discharge prediction to previous studies and showed that the mean absolute percentage errors (MAPE) for predicting the discharge coefficients by PSO-BPNN and GA-BPNN were 1.225% and 1.504%, respectively. Table 2 shows a summary of some previous studies related to machine learning techniques for predicting discharge coefficients (Cd).

Table 2

Summary of some previous studies related to machine learning techniques for predicting discharge coefficient

StudyPurpose of studyResultsInput parametersTechniquesPerformance indices
Roushangar et al. (2017)  They predicted the coefficient of discharge The results demonstrated that the ANFIS model was a more accurate and reliable model to predict the coefficient of discharge • Headwater ratio HT/P
• Cycle width ratio
• Upstream Froude number Fr
• Apex ratio A/w
• Sidewall angle
• Magnification ratio Lc/W 
• Adaptive neuro-fuzzy inference system ANFIS
• Gene expression programming GEP and 
• RMSE
• R2 
Roushangar et al. (2018)  They predicted the coefficients of discharge of arced labyrinth weirs in a reservoir and labyrinth weirs in a flume The results demonstrated that discharge coefficient prediction by the SVM-based model of arced labyrinth weir was a more accurate model when dimensionless parameters, e.g., angle ratio (α/θ), headwater ratio (HT/P), and magnification ratio (Lc/W) were used as input parameters. Furthermore, sensitivity analysis presented that the parameters of headwater ratio and Froude number were the most effective on coefficients of discharge for normal labyrinth weirs, while the most effective parameters on arced labyrinth weirs were headwater ratio and angle ratio (α/θ• Angle ratio α/θ
• Headwater ratio HT/P
• Magnification ratio Lc/W
• aspect ratio w/p
• A/w 
• Support vector machine (SVM)-based models • RMSE
• R2 
Karami et al. (2018)  They predicted the coefficient of discharge for the labyrinth side weirs The results showed that the model of extreme learning machine (ELM) was the best model for predicting discharge coefficients in comparison with the GP and ANN models • Froude number Fr
• Channel width B
• Weir crest length L
• Crest height P
• Vortex angle θ
• Hydraulic head over the weir crest H
• Hydraulic head behind the weir y=(h+w) 
• Artificial neural networks ANN
• Genetic programming GP
• Extreme learning machine ELM 
• R2
• RMSE
• MAPE 
Salazar & Crookston (2019)  They analysed the geometrically arced labyrinth weirs using a new tool of machine learning techniques The results showed that the random forests RF model and neural networks NN model can be utilised as a unique representation for curve fitting • Headwater ratio (HT/P)
• Cycle arc angle θ
• Approach configuration (Flush, arc projecting, projecting)
• Cycle sidewall angle α 
• Random forests RF
• Neural networks NN 
• RMSE
• MAPE
• ME
• MAE 
Zounemat-Kermani et al. (2019)  They predicted the coefficient of discharge over arced labyrinth weirs The outcomes found that the MLPNN was the highest precision in predicting the discharge coefficient over the labyrinth weir among these models • Labyrinth weir height P
• Total head HT
• Crest length Lc
• Number of cycle N
• Sidewall thickness TW
• Sidewall angle α
• Vortex angle θ
• Labyrinth weir width W 
• Bayesian neural network BNN
• Chi-squared automatic interaction detector CHAID
• Gene expression programming GEP
• Least square support vector machine LSSVM
• Multiple linear regression MLR
• Multilayer perceptron neural network MLPNN 
• R2
• RMSE
• MAPE 
Norouzi et al. (2019)  They predicted the discharge coefficient over labyrinth weirs The results showed that the multilayer perceptron MLP model was more appropriate to predict the discharge coefficient • Sidewall angle α
• Magnification ratio Lc/W
• Aspect ratio W/P
• Headwater ratio HT/P 
• Networks
• Multilayer perceptron MLP
• Support vector machines
• Radial basis function networks 
• RMSE
• R2 
Norouzi et al. (2020)  They estimated the discharge coefficient of the labyrinth weir using means of a new self-adaptive extreme learning machine SAELM artificial intelligent AI model The results showed that the ratio of the length of apex geometry to the width of a single cycle (A/w) and the ratio of the total head to the weir height (HT/P) were more effective as input parameters • Froude number Fr
• Sidewall angle α
• Magnification ratio Lc/W
• Length of apex geometry to the width of a single cycle A/w
• Headwater ratio HT/P
• w/P 
• Self-adaptive extreme learning machine SAELM artificial intelligent AI model • RMSE
• R2
• Scatter index
• NSC
• MAE 
Dutta et al. (2020)  They built models to predict the capacity of discharge for circular arc weir and a multi-cycle of labyrinth weir The results showed that the prediction by the SVM regression model was more accurate than the ANN and MLR approach • Head over labyrinth weir h
• Sidewall angle α
• Crest length Lc
• Labyrinth weir height P
• Number of cycle N 
• Support vector machine SVM
• Artificial neural network ANN
• Multiple linear regression MLR 
• R2
• CE
• APE 
Wang et al. (2022)  They predicted the coefficient of discharge for labyrinth weirs using intelligent methods The results showed that the predictions by the PSO-BPNN and the GA-BPNN were more accurate than the BPNN. The maximum error values with the coefficient of discharge prediction by PSO-BPNN and GA-BPNN were 2.6% and 4.4%, respectively. The prediction values of the discharge coefficient were compared with previous studies and found that MAPE values for the discharge coefficient predicted by PSO-BPNN and GA-BPNN were 1.225% and 1.504%, respectively • Channel width B
• Froude number Fr
• Crest length Lc
• Vortex angle θ
• Crest height W
• Head behind the weir y = (h + w)
• Head over the crest of the weir h 
• Nonlinear regression analysis NLR
• BP neural network (BPNN),
• Genetic algorithm (GA) and BP neural network (BPNN) (GA-BPNN)
• Particle swarm optimization PSO and BP neural network (PNN (PSO-BPNN
• RMSE
• R2
• MAE 
StudyPurpose of studyResultsInput parametersTechniquesPerformance indices
Roushangar et al. (2017)  They predicted the coefficient of discharge The results demonstrated that the ANFIS model was a more accurate and reliable model to predict the coefficient of discharge • Headwater ratio HT/P
• Cycle width ratio
• Upstream Froude number Fr
• Apex ratio A/w
• Sidewall angle
• Magnification ratio Lc/W 
• Adaptive neuro-fuzzy inference system ANFIS
• Gene expression programming GEP and 
• RMSE
• R2 
Roushangar et al. (2018)  They predicted the coefficients of discharge of arced labyrinth weirs in a reservoir and labyrinth weirs in a flume The results demonstrated that discharge coefficient prediction by the SVM-based model of arced labyrinth weir was a more accurate model when dimensionless parameters, e.g., angle ratio (α/θ), headwater ratio (HT/P), and magnification ratio (Lc/W) were used as input parameters. Furthermore, sensitivity analysis presented that the parameters of headwater ratio and Froude number were the most effective on coefficients of discharge for normal labyrinth weirs, while the most effective parameters on arced labyrinth weirs were headwater ratio and angle ratio (α/θ• Angle ratio α/θ
• Headwater ratio HT/P
• Magnification ratio Lc/W
• aspect ratio w/p
• A/w 
• Support vector machine (SVM)-based models • RMSE
• R2 
Karami et al. (2018)  They predicted the coefficient of discharge for the labyrinth side weirs The results showed that the model of extreme learning machine (ELM) was the best model for predicting discharge coefficients in comparison with the GP and ANN models • Froude number Fr
• Channel width B
• Weir crest length L
• Crest height P
• Vortex angle θ
• Hydraulic head over the weir crest H
• Hydraulic head behind the weir y=(h+w) 
• Artificial neural networks ANN
• Genetic programming GP
• Extreme learning machine ELM 
• R2
• RMSE
• MAPE 
Salazar & Crookston (2019)  They analysed the geometrically arced labyrinth weirs using a new tool of machine learning techniques The results showed that the random forests RF model and neural networks NN model can be utilised as a unique representation for curve fitting • Headwater ratio (HT/P)
• Cycle arc angle θ
• Approach configuration (Flush, arc projecting, projecting)
• Cycle sidewall angle α 
• Random forests RF
• Neural networks NN 
• RMSE
• MAPE
• ME
• MAE 
Zounemat-Kermani et al. (2019)  They predicted the coefficient of discharge over arced labyrinth weirs The outcomes found that the MLPNN was the highest precision in predicting the discharge coefficient over the labyrinth weir among these models • Labyrinth weir height P
• Total head HT
• Crest length Lc
• Number of cycle N
• Sidewall thickness TW
• Sidewall angle α
• Vortex angle θ
• Labyrinth weir width W 
• Bayesian neural network BNN
• Chi-squared automatic interaction detector CHAID
• Gene expression programming GEP
• Least square support vector machine LSSVM
• Multiple linear regression MLR
• Multilayer perceptron neural network MLPNN 
• R2
• RMSE
• MAPE 
Norouzi et al. (2019)  They predicted the discharge coefficient over labyrinth weirs The results showed that the multilayer perceptron MLP model was more appropriate to predict the discharge coefficient • Sidewall angle α
• Magnification ratio Lc/W
• Aspect ratio W/P
• Headwater ratio HT/P 
• Networks
• Multilayer perceptron MLP
• Support vector machines
• Radial basis function networks 
• RMSE
• R2 
Norouzi et al. (2020)  They estimated the discharge coefficient of the labyrinth weir using means of a new self-adaptive extreme learning machine SAELM artificial intelligent AI model The results showed that the ratio of the length of apex geometry to the width of a single cycle (A/w) and the ratio of the total head to the weir height (HT/P) were more effective as input parameters • Froude number Fr
• Sidewall angle α
• Magnification ratio Lc/W
• Length of apex geometry to the width of a single cycle A/w
• Headwater ratio HT/P
• w/P 
• Self-adaptive extreme learning machine SAELM artificial intelligent AI model • RMSE
• R2
• Scatter index
• NSC
• MAE 
Dutta et al. (2020)  They built models to predict the capacity of discharge for circular arc weir and a multi-cycle of labyrinth weir The results showed that the prediction by the SVM regression model was more accurate than the ANN and MLR approach • Head over labyrinth weir h
• Sidewall angle α
• Crest length Lc
• Labyrinth weir height P
• Number of cycle N 
• Support vector machine SVM
• Artificial neural network ANN
• Multiple linear regression MLR 
• R2
• CE
• APE 
Wang et al. (2022)  They predicted the coefficient of discharge for labyrinth weirs using intelligent methods The results showed that the predictions by the PSO-BPNN and the GA-BPNN were more accurate than the BPNN. The maximum error values with the coefficient of discharge prediction by PSO-BPNN and GA-BPNN were 2.6% and 4.4%, respectively. The prediction values of the discharge coefficient were compared with previous studies and found that MAPE values for the discharge coefficient predicted by PSO-BPNN and GA-BPNN were 1.225% and 1.504%, respectively • Channel width B
• Froude number Fr
• Crest length Lc
• Vortex angle θ
• Crest height W
• Head behind the weir y = (h + w)
• Head over the crest of the weir h 
• Nonlinear regression analysis NLR
• BP neural network (BPNN),
• Genetic algorithm (GA) and BP neural network (BPNN) (GA-BPNN)
• Particle swarm optimization PSO and BP neural network (PNN (PSO-BPNN
• RMSE
• R2
• MAE 

Design methods of the labyrinth weir

The labyrinth weir is a complex structure and the flows over labyrinth weirs are three-dimensional. The labyrinth weir has many parameters affecting discharge capacity. Paxson et al. (2011) showed that the success of a project will depend on factors that influence its design. Ghare et al. (2008) explained that a design should be sought that has a sound hydraulic operation and is economically viable. Although the labyrinth weirs are a favoured design option, they still face difficulties in reaching the optimal design for given sites and location conditions.

Since the innovation of labyrinth weirs, systematic and comprehensive model experiment series have been carried out in many laboratories (Schleiss 2011). These tests provided a large amount of information to evaluate the effect of geometric parameters. Hay & Taylor (1970) found two design charts for trapezoidal and triangular weirs, in which curve diagrams were used to show the relationship between the flow magnification ratio (Q/Qn) and the length magnification ratio (l/w) and dimensionless parameter (h/p). These diagrams explain a set of curves with a range of dimensionless parameters of w/p ≥ 2.5 and 3 ≤ l/w ≤ 8. They used the maximum possible value for sidewall angle (α). The effectiveness (E) was utilised to verify the benefits gained from an increase in the crest length as shown in Equation (3):
(3)
where (L) is the length of the crest, and (w) is the width of one labyrinth weir cycle.
Darvas (1971) introduced a set of design charts and an empirical discharge equation (Equation (4)). This approach used HT and introduced Cd−Darvas, which is a dimensional coefficient of discharge for the labyrinth weir:
(4)
Results were presented as Cd−Darvas against Lc−cycle/w, and a set of design curves (0.2 ≤ HT/P ≤ 0.6) was included for trapezoidal labyrinth weirs, and w/P ≥ 2. They found differences in the results, and the differences between the results were caused by variations in descriptions of the upstream head. Hay & Taylor (1970) used head (h) over a crest, while the USBR used total head over crest (HT). Lux & Hinchliff (1985) found that the coefficient of discharge (Cd−Lux) is a determining factor for the discharge over one labyrinth cycle (Qcycle). This study included a dimensionless parameters of the vertical aspect ratio (w/p) and an apex shape constant (k), as shown in Equation (5):
(5)
where Q is the flow rate over one cycle of the labyrinth weir, Cd− Lux is the coefficient of discharge, w is the width of one cycle, Ht is the total head over a weir, P is the weir height, K is the constant, and g is gravity. This method has a limited design factor of (w/p) ≥ 2.0. Magalhães & Lorena (1989) found a set of curves similar to those obtained by Darvas (1971) for labyrinth weir and found a dimensionless coefficient of discharge, Cd−M&L, as shown in Equation (6):
(6)
The outcomes of estimating discharge coefficients were less than those recommended by Darvas (1971). Magalhães & Lorena (1989) estimated Cd−M&L from six other hydraulic models carried out at the Laboratory of National Civil Engineering (LNEC), Lisbon, Portugal. Tullis et al. (1995) used Equation (7) which was developed for linear weirs:
(7)

The set of curves developed by Tullis et al. (1995) for a trapezoidal labyrinth weir. The angle of the crest was an effective parameter on the curves. Falvey (2003) showed that a set of curves obtained by Tullis et al. (1995) are beneficial for calculating discharge coefficients for both trapezoidal and triangular labyrinth weirs. Empirical equations for different sidewall angles, α, were developed by Tullis et al. (1995) to assist engineers in labyrinth weir design.

Melo et al. (2002) improved the design method Magalhães & Lorena (1989). They modified the parameter, k θ−CW, as shown in Equation (8). This design method showed k θ−CW as a function of θ-CW with sidewall angles between 0° and 90°. They considered the effect of converging channel walls (1.0 ≤ k θ−CW ≤ 1.4):
(8)
Crookston (2010) developed a labyrinth weir design method. Crookston (2010) applied different orientations of the labyrinth weir including rounded, projecting, flush, and inlet. It represents an improvement in the methodology of hydraulic and geometric designs. The results were obtained for half-round and quarter-round crests. Crookston (2010) tested the weir under inverse and normal orientation in the channel. The discharge was computed by the traditional weir equation but has been used the centreline length of the labyrinth weir (Lc) instead of the effect length (Le) which was used by previous design methods. Results were obtained for half-round and quarter-round crest of labyrinth weirs with a range of sidewall angles including 6° ≤ α ≤ 35°. Crookston (2010) developed design equations for labyrinth weirs and linear weirs as shown in Equations (9) and (10):
(9)
(10)
where Cd is the discharge coefficient, HT is the total head, P is the weir height and A, B, C, D are curve fit coefficients.

There are numerous types of studies on labyrinth weirs that have been accomplished through numerous experimental works and the construction of labyrinth weirs all over the world. However, a more in-depth understanding of some of the subjects is still required to adequately address the problems associated with them. Experiments with modifying the geometry and planform of the labyrinth weirs are being conducted in order to increase the discharge capacity and are being investigated. Although few authors have studied the floating debris risk, it needs further investigation. The construction methods require further investigation, and the produced reinforcement concrete can be an interesting solution. The main issues that are influencing a project, such as costs and delays, Therefore, we can seek new methods for the rapid construction of labyrinth weirs. These methods depend on hydrologic data and a minimum number of parameters that could be further taken up for research. The structural properties, as well as the materials used in the construction of the labyrinth weirs as composite structures, can be an area of further research. Also, relating labyrinth weirs to other kinds of spillways with the lowest cost is an area of further investigation. The use of numerical modelling to conduct research rather than physical models, which are frequently more time-consuming and expensive, can be an inspection. The energy dissipation downstream of the labyrinth weirs is one of the interesting issues in labyrinth weirs that needs further study. Different energy dissipators can be further investigated for effective energy dissipation with minimum cost. Machine learning methods need more study to provide significant and reliable equations to assist the designers in predicting discharge over labyrinth weirs.

The labyrinth weirs play an essential role in guaranteeing the security of human life, in addition to protecting developing areas. In recent years, labyrinth weirs have been widely used because of their high efficiency. Although labyrinth weirs have complex hydraulic behaviour, there have been studied by researchers for a long time. Many studies demonstrated that labyrinth weirs are not applicable, particularly under high relative overflow depth, high submergence, and poor plan geometry. The labyrinth weir is a complex structure. Therefore, it needs a large number of experimental tests to find empirically the impact of the different parameters on the capacity of discharge. Therefore, some parameters still need to be further investigated. Ideally, the hydraulically most efficient design needs to be considered during the design and construction of a labyrinth weir, but this is not always possible because many parameters affect the weir design. In addition, many factors may affect discharge capacities, such as increasing construction costs and the nature of the site regarding geological, topographic, and facility limitations. In addition, common design equations do not take into account all parameters affecting labyrinth weir performance, such as labyrinth weir geometries, flow conditions, site conditions, and scale effect. The design of labyrinth weir methods depends mainly on empirical equations derived from experimental work and generalised performance curves. Physical models still need more investigation. A labyrinth weir has a complex geometry. Therefore, it is a fascinating challenge for future numerical and experimental research. Also, labyrinth weir development may be enhanced with this historical outlook for further improvement both in economic and hydraulic features.

The authors would like to express their special thanks to the technician staff in the laboratory of the school of engineering at Deakin University, who supported them to complete this work.

All relevant data are included in the paper or its Supplementary Information.

The authors declare there is no conflict.

Ackers
J.
,
Bennet
F.
&
Zamesky
G.
2011
Upgrading Lake Holiday spillway using a labyrinth weir
. In:
Proceedings of the 31st Annual USSD Conference
,
San Diego, California
, pp.
1683
1696
.
Akoz
M. S.
,
Gumus
V.
&
Kirkgoz
M. S.
2014
Numerical simulation of flow over a semicylinder weir
.
Journal of Irrigation and Drainage Engineering
140
(
6
),
04014016
.
https://doi.org/10.1061/(asce)ir.1943-4774.0000717
.
Amanian
N.
1987
Performance and Design of Labyrinth Spillway
.
M.S. Thesis
,
Utah State University
,
Logan
,
Utah
.
Baeimani
M.
&
Bajestan
M. S.
2015
Numerical modeling of hydraulic performance of piano keys overflows with different geometry
.
Cumhuriyet Science Journal
36
,
2136
2148
.
Bahrebar
A.
,
Azarpayvand
H., asl
,
Momni Asl
M.
&
Barati
F.
2016
Laboratory investigation of the effect of a new labyrinth with different length and width in the wing length of a triangular-shaped labyrinth weir
.
International Journal of Advanced Biotechnology and Research
7
,
338
342
.
Bhuiyan
F. A. B. M.
&
Hey
R.
2007
Computation of three-dimensional flow field created by weir-type structures
.
Engineering Applications of Computational Fluid Mechanics
1
(
4
),
350
360
.
https://doi.org/10.1080/19942060.2007.11015205
.
Carollo
F. G.
,
Ferro
V.
&
Pampalone
V.
2012
Experimental investigation of the outflow process over a triangular labyrinth-weir
.
Journal of Irrigation and Drainage Engineering, ASCE
138
(
1
),
73
79
.
https://doi.org/10.1061/(asce)ir.1943-4774.0000366
.
Carrillo
J. M.
,
Matos
J.
&
Lopes
R.
2019
Numerical modeling of free and submerged labyrinth weir flow for a large sidewall angle
.
Environmental Fluid Mechanics
,
1
18
.
https://doi.org/10.1007/s10652-019-09701-0
.
Cassidy
J. J.
,
Gardner
C. A.
&
Peacock
R. T.
1985
Boardman labyrinth crest spillway
.
Journal of Hydraulic Engineering
111
(
3
),
398
416
.
https://doi.org/10.1061/(asce)0733-9429(1985)111:3(398)
.
Crookston
B.
,
Tullis
B. P.
,
2010
Hydraulic performance of labyrinth weirs
. In:
Proceedings of the 3rd International Junior Researcher and Engineer Workshop on Hydraulic Structures, Edinburgh
(
Janssen
R.
&
Chanson
H.
, eds).
Hydraulic model report CH80/10, University of Queensland
,
Brisbane
, pp.
39
46
.
Crookston
B. M.
2010
Labyrinth Weirs
.
Doctor of Philosophy (PhD) Dissertation
,
Utah State University
.
Crookston
B. M.
&
Tullis
B. P.
2011a
Discharge efficiency of reservoir-application-specific labyrinth weirs
.
Journal of Irrigation and Drainage Engineering
138
(
6
),
564
568
.
https://doi.org/10.1061/(asce)ir.1943-4774.0000451
.
Crookston
B. M.
&
Tullis
B. P.
2011b
Hydraulic characteristics of labyrinth weirs
. In:
Proceedings of the International Conference Labyrinth and Piano Key Weirs–PKW
. pp.
25
32
.
https://doi.org/10.1201/b12349-5
.
Crookston
B. M.
&
Tullis
B. P.
2012a
Hydraulic design and analysis of labyrinth weirs. I: discharge relationships
.
Journal of Irrigation and Drainage Engineering
139
(
5
),
363
370
.
https://doi.org/10.1061/(asce)ir.1943-4774.0000558
.
Crookston
B. M.
&
Tullis
B. P.
2012b
Hydraulic design and analysis of labyrinth weirs. II: nappe aeration, instability, and vibration
.
Journal of Irrigation and Drainage Engineering
139
(
5
),
371
377
.
https://doi.org/10.1061/(asce)ir.1943-4774.0000553
.
Crookston
B. M.
&
Tullis
B. P.
2012c
Labyrinth weirs: nappe interference and local submergence
.
Journal of Irrigation and Drainage Engineering
138
(
8
),
757
765
.
https://doi.org/10.1061/(asce)ir.1943-4774.0000466
.
Crookston
B. M.
,
Paxson
G. S.
&
Savage
B. M.
2012a
Hydraulic performance of labyrinth weirs for high headwater ratios
. In:
The 4th IAHR International Symposium on Hydraulic Structures
,
In: Erpicum, S., Laugier, F., Boillat, J. L., Pirotton, M., Reverchon, B. & Schleiss, A. J. Labyrinth and piano key weirs II-PKW, CRC Press
,
Porto
,
Portugal
, pp.
1
8
.
Crookston
B. M.
,
Paxson
G. S.
&
Savage
B. M.
2012b
It can be done! Labyrinth weir design guidance for high headwater and low cycle width ratios
. In:
Proc., Dam Safety 2012
,
ASDSO
,
Denver, CO
.
Crookston
B. M.
,
Anderson
A.
,
Shearin-Feimster
L.
&
Tullis
B. P.
2014
Mitigation investigation of flow-induced vibrations at a rehabilitated spillway
. In:
11th National Conference on Hydraulics in Civil Engineering & 5th International Symposium on Hydraulic Structures: Hydraulic Structures and Society-Engineering Challenges and Extremes
,
Engineers Australia
, p.
149
.
https://doi.org/10.14264/uql.2014.30
.
Dabling
M. R.
,
Tullis
B. P.
&
Crookston
B. M.
2013
Staged labyrinth weir hydraulics
.
Journal of Irrigation and Drainage Engineering
139
(
11
),
955
960
.
https://doi.org/10.1061/(asce)ir.1943-4774.0000636
.
Darvas
L. A.
1971
Discussion of performance and design of labyrinth weirs
.
Journal of the Hydraulics Division
97
,
1246
1251
.
https://doi.org/10.1061/jyceaj.0003056
.
Dutta
D.
,
Mandal
A.
&
Afzal
M. S.
2020
Discharge performance of plan view of multi-cycle W-form and circular arc labyrinth weir using machine learning
.
Flow Measurement and Instrumentation
73
,
101740
.
https://doi.org/10.1016/j.flowmeasinst.2020.101740
.
Emiroglu
M. E.
&
Baylar
A.
2005
Influence of included angle and sill slope on air entrainment of triangular planform labyrinth weirs
.
Journal of Hydraulic Engineering
131
(
3
),
184
189
.
https://doi.org/10.1061/(asce)0733-429(2005)131:3(184)
.
Emiroglu
M. E.
&
Kisi
O.
2013
Prediction of discharge coefficient for trapezoidal labyrinth side weir using a neuro-fuzzy approach
.
Water Resources Management
27
(
5
),
1473
1488
.
https://doi.org/10.1007/s11269-012-0249-0
.
Emiroglu
M. E.
,
Kaya
N.
&
Agaccioglu
H.
2010
Discharge capacity of labyrinth side weir located on a straight channel
.
Journal of Irrigation and Drainage Engineering
136
(
1
),
37
46
.
https://doi.org/10.1061/(asce)ir.1943-4774.0000112
.
Falvey
H. T.
2003
Hydraulic Design of Labyrinth Weirs
.
ASCE Press (American Society of Civil Engineers)
,
Reston, VA
.
Ghare
A. D.
,
Mhaisalkar
V. A.
&
Porey
P. D.
2008
An approach to optimal design of trapezoidal labyrinth weirs
.
World Applied Sciences Journal
3
(
6
),
934
938
.
Ghodsian
M.
2009
Stage–discharge relationship for a triangular labyrinth spillway
. In:
Proceedings of the Institution of Civil Engineers-Water Management
, Vol.
162
, No.
3
, pp.
173
178
,
Thomas Telford Ltd
.
https://doi.org/10.1680/wama.2009.00033
.
Gupta
S. K.
&
Singh
V. P.
2013
Discussion of experimental studies on flow over labyrinth weir by BV Khode, AR Tembhurkar, PD Porey, and RN Ingle
.
Journal of Irrigation and Drainage Engineering
139
(
12
),
1048
1051
.
https://doi.org/10.1061/(asce)ir.1943-4774.0000581
.
Gupta
K. K.
,
Kumar
S.
&
Kumar
K.
2013
Flow characteristics of sharp-crested triangular plan form contracted weirs
.
International Journal of Engineering Research & Technology (IJERT)
2
(
12
),
1252
1258
.
Gupta
K. K.
,
Kumar
S.
&
Ahmad
Z.
2014
Flow characteristics of sharp-crested W-planform weirs
.
International Journal of Advanced Technology & Engineering Research (IJATER)
4
,
176
180
.
Gupta
K. K.
,
Kumar
S.
&
Ahmad
Z.
2015
Effect of weir height on flow performance of sharp crested rectangular – planform weir
.
World Applied Sciences Journal
33
(
1
),
168
175
.
Hay
N.
&
Taylor
G.
1970
Performance and design of labyrinth weirs
.
Journal of the Hydraulics Engineering, ASCE
96
(
11
),
2337
2357
.
Holmquist-Johnson
C. L.
2011
Numerical Analysis of River Spanning Rock U-Weirs: Evaluating Effects of Structure Geometry on Local Hydraulics
.
Doctoral Dissertation
,
Colorado State University
.
https://doi.org/10.1061/41036(342)328
.
Houston
K. L.
1982
Hydraulic Model Study of Ute Dam Labyrinth Spillway
.
Bureau of Reclamation Division of Research Hydraulics Branch
,
Denver
.
Idrees
A. K.
&
Al-Ameri
R.
2022
Improving the performance of the compound labyrinth weirs using an artificial ventilation approach
.
Water Supply
22
(
8
),
6585
6602
.
https://doi.org/10.2166/ws.2022.260
.
Idrees
A. K.
,
Al-Ameri
R.
&
Das
S.
2016
Determination of discharge coefficient for flow over one cycle compound trapezoidal plan form labyrinth weir
.
International Journal of Civil Engineering and Technology
7
(
4
),
314
328
.
Idrees
A. K.
,
Al-Ameri
R.
,
Chua
L.
&
Das
S.
2017
Experimental study on the hydraulic performance of trapezoidal planform compound labyrinth weir
. In:
First MOHESR and HCED Iraqi Scholars Conference in Australasia 2017
. p.
51
.
Idrees
A. K.
,
Al-Ameri
R.
,
Chua
L.
&
Das
S.
2018
Discharge characteristics for trapezoidal compound labyrinth
. In:
IAHRAPD 2018: Multi-Perspective Water for Sustainable Development: Proceedings of the 21st Congress of International Association for Hydro-Environment Engineering and Research (IAHR), Asia Pacific Division (APD), in Conjunction with 6th Regional Conference on Natural Disaster (RCND)
.
International Association for Hydro-Environment Engineering and Research
, pp.
305
311
.
Idrees
A. K.
,
Al-Ameri
R.
&
Das
S.
2022
Using CFD modelling to study hydraulic flow over labyrinth weirs
.
Water Supply
22
(
3
),
3125
3142
.
https://doi.org/10.2166/ws.2021.424
.
Institute for Water and Environmental Engineering
2012
Investigation of Unsteady Flow Conditions at Dam Bottom Outlet Works Due to Air Entrainment During Gate Closure. Volume II: Computational Modelling
.
Water Research Commission
,
Gezina
.
Kabiri-Samani
A.
&
Javaheri
A.
2012
Discharge coefficients for free and submerged flow over Piano Key weirs
.
Journal of Hydraulic Research
50
(
1
),
114
120
.
https://doi.org/10.1080/00221686.2011.647888
.
Kanyabujinja
N. P.
2015
CFD Modelling of Ogee Spillway Hydraulics and Comparison with Physical Model Tests
.
Doctoral Dissertation
,
Stellenbosch University
,
Stellenbosch
.
Karami
H.
,
Karimi
S.
,
Bonakdari
H.
&
Shamshirband
S.
2018
Predicting discharge coefficient of triangular labyrinth weir using extreme learning machine, artificial neural network and genetic programming
.
Neural Computing and Applications
29
(
11
),
983
989
.
https://doi.org/10.1007/s00521-016-2588-x
.
Keramati
R. A.
,
Azarpayvand
H.
,
Bahrebar
A.
,
Momni Asl
M.
&
Barati
F.
2014
Laboratory investigation of the effect of a new labyrinth with different length and width in the wing length of a triangular-shaped labyrinth weir
.
Journal of Middle East Applied Science and Technology (JMEAST)
,
561
566
.
Khode
B. V.
&
Tembhurkar
A. R.
2010
Evaluation and analysis of crest coefficient for labyrinth weir
.
World Applied Sciences Journal
11
,
835
839
.
Khode
B. V.
,
Tembhurkar
A. R.
,
Porey
P. D.
&
Ingle
R. N.
2011
Determination of crest coefficient for flow over trapezoidal labyrinth weir
.
World Applied Sciences Journal
12
(
3
),
324
329
.
Khode
B. V.
,
Tembhurkar
A. R.
,
Porey
P. D.
&
Ingle
R. N.
2012
Experimental studies on flow over labyrinth weir
.
Journal of Irrigation and Drainage Engineering
138
(
6
),
548
552
.
https://doi.org/10.1061/(asce)ir.1943-4774.0000336
.
Kumar
S.
,
Ahmad
Z.
&
Mansoor
T.
2011
A new approach to improve the discharging capacity of sharp-crested triangular plan form weirs
.
Flow Measurement and Instrumentation
22
,
175
180
.
https://doi.org/10.1016/j.flowmeasinst.2011.01.006
.
Kumar
S.
,
Ahmad
Z.
,
Mansoor
T.
&
Himanshu
S. K.
2012
Discharge characteristics of sharp crested weir of curved plan-form
.
Research Journal of Engineering Sciences
2278
,
9472
.
Lux
F.
III
1984
Discharge characteristics of labyrinth weirs
. In:
Proceedings of Conference on Water for Resource Development, American Society of Civil Engineering, Coeur d'Alene, Idaho
. pp.
385
389
.
Lux
F.
&
Hinchliff
D.
1985
Design and construction of labyrinth spillways
. In:
15th Congress International Commission on Large Dams ICOLD
, Vol.
IV
,
Q59-R15, Lausanne, Switzerland
, pp.
249
274
.
Magalhães
A. P.
&
Lorena
M.
1989
Hydraulic Design of Labyrinth Weirs. Memoir No. 736
.
National Laboratory of Civil Engineering (LNEC)
,
Portugal
(in Portuguese)
.
Melo
J. F.
,
Ramos
C. M.
&
Magalhães
A. P.
2002
Descarregadores com soleira em labirinto de um ciclo em canais convergentes. Determinação da capacidade de vazão
. In:
Proc. 6° Congresso da Água
.
Mirnaseri
M.
&
Emadi
A.
2014
Hydraulic performance of combined flow labyrinth weir-gate
.
Advance in Agriculture and Biology
2
,
54
60
.
https://doi.org/10.15192/pscp.aab.2014.1.1.article1
.
Norouzi
R.
,
Daneshfaraz
R.
&
Ghaderi
A.
2019
Investigation of discharge coefficient of trapezoidal labyrinth weirs using artificial neural networks and support vector machines
.
Applied Water Science
9
(
7
),
1
10
.
https://doi.org/10.1007/s13201-019-1026-5
.
Norouzi
P.
,
Rajabi
A.
,
Izadbakhsh
M. A.
,
Shabanlou
S.
,
Yosefvand
F.
&
Yaghoubi
B.
2020
A new non-tuned self-adaptive machine-learning approach for simulating the discharge coefficient of labyrinth weirs
.
Irrigation and Drainage
69
(
3
),
398
416
.
https://doi.org/10.1002/ird.2423
.
Ouamane
A.
&
Lempérière
F.
2013
Improvement of labyrinth weirs shape
. In:
International Workshop on Labyrinth and Piano Key Weirs – PKW 2013
.
CRC Press
,
London
, pp.
15
22
.
https://doi.org/10.1201/b15985-4
.
Paxson
G.
&
Savage
B.
2006
Labyrinth Spillways: Comparison of two Popular USA Design Methods and Consideration of non-Standard Approach Conditions and Geometries
.
Division of Civil Engineering
,
Brisbane
, pp.
37
46
.
Paxson
G.
,
Crookston
B.
,
Savage
B.
,
Tullis
B. P.
&
Lux
F.
2008
The Hydraulic Design Toolbox: Theory and Modeling for the Lake Townsend Spillway Replacement Project
.
Association of State Dam Safety Officials (ASDSO)
.
Paxson
G.
,
Campbell
D.
&
Monroe
J.
2011
Evolving Design Approaches and Considerations for Labyrinth Spillways
.
U.S. Society on Dams
,
San Diego
, pp.
1645
1666
.
Roushangar
K.
,
Alami
M. T.
,
Majedi Asl
M.
&
Shiri
J.
2017
Modeling discharge coefficient of Normal and inverted orientation labyrinth weirs using machine learning techniques
.
ISH Journal of Hydraulic Engineering
23
(
3
),
331
340
.
https://doi.org/10.1080/09715010.2017.1327333
.
Roushangar
K.
,
Alami
M. T.
,
Shiri
J.
&
Asl
M. M.
2018
Determining discharge coefficient of labyrinth and arced labyrinth weirs using support vector machine
.
Hydrology Research
49
(
3
),
924
938
.
https://doi.org/10.2166/nh.2017.214
.
Salazar
F.
&
Crookston
B. M.
2019
A performance comparison of machine learning algorithms for arced labyrinth spillways
.
Water
11
(
3
),
544
.
https://doi.org/10.3390/w11030544
.
Savage
B.
,
Frizell
K.
&
Crowder
J.
2004
Brains versus brawn: the changing world of hydraulic model studies
. In:
Proceedings of the 2004 Annual Conference
.
Association of State Dam Safety Officials (ASDSO)
,
Phoenix
,
USA
.
Schleiss
A. J.
2011
From labyrinth to piano key weirs: A historical review
. In:
Labyrinth and Piano key Weirs –PKW 2011
.
CRC Press
,
London
, pp.
3
15
.
https://doi.org/10.1201/b12349-3
.
Torres
C.
,
Borman
D.
,
Sleigh
A.
&
Neeve
D.
2018
Determination of scale effects for a scaled physical model of a Labyrinth weir using CFD
. In:
7th IAHR International Symposium on Hydraulic Structures
,
15-18 May
,
Aachen, Germany
.
doi:10.15142/T38W7F (978-0-692-13277-7)
.
Tullis
J. P.
,
Amanian
N.
&
Waldron
D.
1995
Design of labyrinth spillways
.
Journal of Hydraulic Engineering
121
(
3
),
247
255
.
https://doi.org/10.1061/(asce)0733-9429(1995)121:3(247)
.
Tullis
B. P.
,
Willmore
C. M.
&
Wolfhope
J. S.
2005
Improving performance of low-head labyrinth weirs
. In:
Proceedings of the 2005 World Water and Environmental Resources Congress, May 2005, 15–19. In: Impacts of Global Climate Change
. pp.
1
9
.
https://doi.org/10.1061/40792(173)418
.
Tullis
B. P.
,
Young
J. C.
&
Chandler
M. A.
2007
Head-discharge relationships for submerged labyrinth weirs
.
Journal of Hydraulic Engineering
133
(
3
),
248
254
.
https://doi.org/10.1061/(asce)0733-9429(2007)133:3(248)
.
Versteeg
H.
&
Malalasekera
W.
1995
An Introduction to Computational Fluid Dynamics
.
Longman Scientific and Technical
,
Harlow
.
https://doi.org/10.1002/9780470172643.ch18
.
Wang
F.
,
Zheng
S.
,
Ren
Y.
,
Liu
W.
&
Wu
C.
2022
Application of hybrid neural network in discharge coefficient prediction of triangular labyrinth weir
.
Flow Measurement and Instrumentation
83
,
102108
.
https://doi.org/10.1016/j.flowmeasinst.2021.102108
.
Wormleaton
P. R.
&
Soufiani
E.
1998
Aeration performance of triangular planform labyrinth weirs
.
Journal of Environmental Engineering
124
(
8
),
709
719
.
https://doi.org/10.1061/(asce)0733-9372(1998)124:8(709)
.
Wormleaton
P. R.
&
Tsang
C. C.
2000
Aeration performance of rectangular planform labyrinth weirs
.
Journal of Environmental Engineering
126
(
5
),
456
465
.
https://doi.org/10.1061/(asce)0733-9372(2000)126:5(456)
.
Zounemat-Kermani
M.
,
Kermani
S. G.
,
Kiyaninejad
M.
&
Kisi
O.
2019
Evaluating the application of data-driven intelligent methods to estimate discharge over triangular arced labyrinth weir
.
Flow Measurement and Instrumentation
68
,
101573
.
https://doi.org/10.1016/j.flowmeasinst.2019.101573
.
This is an Open Access article distributed under the terms of the Creative Commons Attribution Licence (CC BY 4.0), which permits copying, adaptation and redistribution, provided the original work is properly cited (http://creativecommons.org/licenses/by/4.0/).