Abstract
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.
HIGHLIGHTS
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
NOTATIONS
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
INTRODUCTION
Shapes of labyrinth weirs: (a) rectangular, (b) triangular, and (c) trapezoidal (Crookston 2010).
Shapes of labyrinth weirs: (a) rectangular, (b) triangular, and (c) trapezoidal (Crookston 2010).
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).
The geometric labyrinth weir parameters. (a) Labyrinth weir plan, (b) types of crest shapes, (c) cross-section AA (Crookston 2010).
The geometric labyrinth weir parameters. (a) Labyrinth weir plan, (b) types of crest shapes, (c) cross-section AA (Crookston 2010).
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.
Summary of some previous studies related to labyrinth weirs
Study . | Purpose . | Limitations . | Place of experiment . | Results . |
---|---|---|---|---|
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 |
Study . | Purpose . | Limitations . | Place of experiment . | Results . |
---|---|---|---|---|
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 |
PHYSICAL MODELLING
Variations dimensionless parameter of K/P against H/P for a triangular labyrinth weir Ghodsian (2009).
Variations dimensionless parameter of K/P against H/P for a triangular labyrinth weir Ghodsian (2009).
The discharge coefficient versus Ht/P for different sidewall angles of trapezoidal labyrinth weir (Khode et al. 2011).
The discharge coefficient versus Ht/P for different sidewall angles of trapezoidal labyrinth weir (Khode et al. 2011).
The discharge coefficient versus Ht/P for different sidewall angles of trapezoidal labyrinth weir Khode et al. (2012).
The discharge coefficient versus Ht/P for different sidewall angles of trapezoidal labyrinth weir Khode et al. (2012).
Cycle efficiency against HT/P for different sidewall angles of the labyrinth weirs Crookston et al. (2012b).
Cycle efficiency against HT/P for different sidewall angles of the labyrinth weirs Crookston et al. (2012b).
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).
Summary of some previous studies related to machine learning techniques for predicting discharge coefficient
Study . | Purpose of study . | Results . | Input parameters . | Techniques . | Performance 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 |
Study . | Purpose of study . | Results . | Input parameters . | Techniques . | Performance 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.
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.
SCOPE OF FUTURE WORK
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.
CONCLUSION
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.
ACKNOWLEDGEMENTS
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.
DATA AVAILABILITY STATEMENT
All relevant data are included in the paper or its Supplementary Information.
CONFLICT OF INTEREST
The authors declare there is no conflict.