# Optimized Vegetation Density to Dissipate Energy of Flood Flow in Open Canals

Authors: Mahdi Feizbahr; Navid Tonekaboni; Guang-Jun Jiang; Hong-Xia Chen
Journal: Mathematical Problems in Engineering
 (2021)

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## Abstract

Vegetation along the river increases the roughness and reduces the average flow velocity, reduces flow energy, and changes the flow velocity profile in the cross section of the river. Many canals and rivers in nature are covered with vegetation during the floods. Canal’s roughness is strongly affected by plants and therefore it has a great effect on flow resistance during flood. Roughness resistance against the flow due to the plants depends on the flow conditions and plant, so the model should simulate the current velocity by considering the effects of velocity, depth of flow, and type of vegetation along the canal. Total of 48 models have been simulated to investigate the effect of roughness in the canal. The results indicated that, by enhancing the velocity, the effect of vegetation in decreasing the bed velocity is negligible, while when the current has lower speed, the effect of vegetation on decreasing the bed velocity is obviously considerable.


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## Body

## 1. Introduction

Considering the impact of each variable is a very popular field within the analytical and statistical methods and intelligent systems [1–14]. This can help research for better modeling considering the relation of variables or interaction of them toward reaching a better condition for the objective function in control and engineering [15–27]. Consequently, it is necessary to study the effects of the passive factors on the active domain [28–36]. Because of the effect of vegetation on reducing the discharge capacity of rivers [37], pruning plants was necessary to improve the condition of rivers. One of the important effects of vegetation in river protection is the action of roots, which cause soil consolidation and soil structure improvement and, by enhancing the shear strength of soil, increase the resistance of canal walls against the erosive force of water. The outer limbs of the plant increase the roughness of the canal walls and reduce the flow velocity and deplete the flow energy in vicinity of the walls. Vegetation by reducing the shear stress of the canal bed reduces flood discharge and sedimentation in the intervals between vegetation and increases the stability of the walls [38–41].One of the main factors influencing the speed, depth, and extent of flood in this method is Manning’s roughness coefficient. On the other hand, soil cover [42], especially vegetation, is one of the most determining factors in Manning’s roughness coefficient. Therefore, it is expected that those seasonal changes in the vegetation of the region will play an important role in the calculated value of Manning’s roughness coefficient and ultimately in predicting the flood wave behavior [43–45]. The roughness caused by plants’ resistance to flood current depends on the flow and plant conditions. Flow conditions include depth and velocity of the plant, and plant conditions include plant type, hardness or flexibility, dimensions, density, and shape of the plant [46]. In general, the issue discussed in this research is the optimization of flood-induced flow in canals by considering the effect of vegetation-induced roughness. Therefore, the effect of plants on the roughness coefficient and canal transmission coefficient and in consequence the flow depth should be evaluated [47, 48].Current resistance is generally known by its roughness coefficient. The equation that is mainly used in this field is Manning equation. The ratio of shear velocity to average current velocityV∗/V is another form of current resistance. The reason for using the V∗/V ratio is that it is dimensionless and has a strong theoretical basis. The reason for using Manning roughness coefficient is its pervasiveness. According to Freeman et al. [49], the Manning roughness coefficient for plants was calculated according to the Kouwen and Unny [50] method for incremental resistance. This method involves increasing the roughness for various surface and plant irregularities. Manning’s roughness coefficient has all the factors affecting the resistance of the canal. Therefore, the appropriate way to more accurately estimate this coefficient is to know the factors affecting this coefficient [51].To calculate the flow rate, velocity, and depth of flow in canals as well as flood and sediment estimation, it is important to evaluate the flow resistance. To determine the flow resistance in open ducts, Manning, Chézy, and Darcy–Weisbach relations are used [52]. In these relations, there are parameters such as Manning’s roughness coefficient (n), Chézy roughness coefficient (C), and Darcy–Weisbach coefficient (f). All three of these coefficients are a kind of flow resistance coefficient that is widely used in the equations governing flow in rivers [53].The three relations that express the relationship between the average flow velocity (V) and the resistance and geometric and hydraulic coefficients of the canal are as follows:(1)V=KnnR2/3Sf1/2,Manning,(2)V=8gfRSf,Darcy−Weisbach,(3)V=CRSf,Chezy,where n, f, and c are Manning, Darcy–Weisbach, and Chézy coefficients, respectively. V = average flow velocity, R = hydraulic radius, Sf = slope of energy line, which in uniform flow is equal to the slope of the canal bed, g = gravitational acceleration, and Kn is a coefficient whose value is equal to 1 in the SI system and 1.486 in the English system. The coefficients of resistance in equations (1) to (3) are related as follows:(4)f8=nR1/6gKn=gC=gRSfV.Based on the boundary layer theory, the flow resistance for rough substrates is determined from the following general relation:(5)8f=2.5LnyKs+A,where f = Darcy–Weisbach coefficient of friction, y = flow depth, Ks = bed roughness size, and A = constant coefficient.On the other hand, the relationship between the Darcy–Weisbach coefficient of friction and the shear velocity of the flow is as follows:(6)8f=VU∗.By using equation (6), equation (5) is converted as follows:(7)8f=VU∗2.5LnyKs+A.Investigation on the effect of vegetation arrangement on shear velocity of flow in laboratory conditions showed that, with increasing the shear Reynolds number (Re∗), the numerical value of the V/U∗ ratio also increases; in other words the amount of roughness coefficient increases with a slight difference in the cases without vegetation, checkered arrangement, and cross arrangement, respectively [54].Roughness in river vegetation is simulated in mathematical models with a variable floor slope flume by different densities and discharges. The vegetation considered submerged in the bed of the flume. Results showed that, with increasing vegetation density, canal roughness and flow shear speed increase and with increasing flow rate and depth, Manning’s roughness coefficient decreases. Factors affecting the roughness caused by vegetation include the effect of plant density and arrangement on flow resistance, the effect of flow velocity on flow resistance, and the effect of depth [45, 55].One of the works that has been done on the effect of vegetation on the roughness coefficient is Darby [56] study, which investigates a flood wave model that considers all the effects of vegetation on the roughness coefficient. There are currently two methods for estimating vegetation roughness. One method is to add the thrust force effect to Manning’s equation [47, 57, 58] and the other method is to increase the canal bed roughness (Manning-Strickler coefficient) [45, 59–61]. These two methods provide acceptable results in models designed to simulate floodplain flow. Wang et al. [62] simulate the floodplain with submerged vegetation using these two methods and to increase the accuracy of the results, they suggested using the effective height of the plant under running water instead of using the actual height of the plant. Freeman et al. [49] provided equations for determining the coefficient of vegetation roughness under different conditions. Lee et al. [63] proposed a method for calculating the Manning coefficient using the flow velocity ratio at different depths. Much research has been done on the Manning roughness coefficient in rivers, and researchers [49, 63–66] sought to obtain a specific number for n to use in river engineering. However, since the depth and geometric conditions of rivers are completely variable in different places, the values of Manning roughness coefficient have changed subsequently, and it has not been possible to choose a fixed number. In river engineering software, the Manning roughness coefficient is determined only for specific and constant conditions or normal flow. Lee et al. [63] stated that seasonal conditions, density, and type of vegetation should also be considered. Hydraulic roughness and Manning roughness coefficient n of the plant were obtained by estimating the total Manning roughness coefficient from the matching of the measured water surface curve and water surface height. The following equation is used for the flow surface curve:(8)∂y∂x=S0−Sf1−Fr2,where ∂y/∂x is the depth of water change, S0 is the slope of the canal floor, Sf is the slope of the energy line, and Fr is the Froude number which is obtained from the following equation:(9)Fr=VgD,where D is the characteristic length of the canal. Flood flow velocity is one of the important parameters of flood waves, which is very important in calculating the water level profile and energy consumption. In the cases where there are many limitations for researchers due to the wide range of experimental dimensions and the variety of design parameters, the use of numerical methods that are able to estimate the rest of the unknown results with acceptable accuracy is economically justified.FLOW-3D software uses Finite Difference Method (FDM) for numerical solution of two-dimensional and three-dimensional flow. This software is dedicated to computational fluid dynamics (CFD) and is provided by Flow Science [67]. The flow is divided into networks with tubular cells. For each cell there are values of dependent variables and all variables are calculated in the center of the cell, except for the velocity, which is calculated at the center of the cell. In this software, two numerical techniques have been used for geometric simulation, FAVOR™ (Fractional-Area-Volume-Obstacle-Representation) and the VOF (Volume-of-Fluid) method. The equations used at this model for this research include the principle of mass survival and the magnitude of motion as follows. The fluid motion equations in three dimensions, including the Navier–Stokes equations with some additional terms, are as follows:(10)∂u∂t+1VFuAx∂u∂x+vAyR∂u∂y+wAz∂u∂z−ξAyv2xVF=−1ρ∂P∂x+Gx+fx−RSORρVFu,∂v∂t+1VFuAx∂v∂x+vAyR∂v∂y+wAz∂v∂z−ξAyvuxVF=−1ρR∂P∂y+Gy+fy−RSORρVFv,∂w∂t+1VFuAx∂w∂x+vAyR∂w∂y+wAz∂w∂z=−1ρ∂P∂z+Gz+fz−RSORρVFw,where Gx,Gy,GZ are mass accelerations in the directions x, y, z and fx,fy,fz are viscosity accelerations in the directions x, y, z and are obtained from the following equations:(11)ρVFfx=wsx−∂∂xAxτxx+R∂∂yAyτxy+∂∂zAzτxz+ξxAxτxx−Ayτyy,ρVFfy=wsy−∂∂xAxτxy+R∂∂yAyτyy+∂∂zAzτyz+ξxAx−Ayτxy,ρVFfz=wsz−∂∂xAxτxz+R∂∂yAyτyz+∂∂zAzτzz+ξxAxτxz.Shear stressesτxx,τyy,τzz,τxy,τxz,τyz in equation (11) are obtained from the following equations:(12)τxx=−2μ∂u∂x−13∂u∂x+R∂v∂y+∂w∂z+ξux,τyy=−2μ∂v∂y+ξux−13∂u∂x+R∂v∂y+∂w∂z+ξux,τzz=−2μ∂w∂z−13∂u∂x+R∂v∂y+∂w∂z+ξux,τxy=−μ∂v∂x+R∂u∂y−ξvx,τxz=−μ∂u∂z+∂w∂x,τyz=−μ∂v∂z+R∂w∂y.The standard model is used for high Reynolds currents, but in this model, RNG theory allows the analytical differential formula to be used for the effective viscosity that occurs at low Reynolds numbers. Therefore, the RNG model can be used for low and high Reynolds currents.Weather changes are high and this affects many factors continuously. The presence of vegetation in any area reduces the velocity of surface flows and prevents soil erosion, so vegetation will have a significant impact on reducing destructive floods. One of the methods of erosion protection in floodplain watersheds is the use of biological methods. The presence of vegetation in watersheds reduces the flow rate during floods and prevents soil erosion. The external organs of plants increase the roughness and decrease the velocity of water flow and thus reduce its shear stress energy. One of the important factors with which the hydraulic resistance of plants is expressed is the roughness coefficient. Measuring the roughness coefficient of plants and investigating their effect on reducing velocity and shear stress of flow is of special importance.Roughness coefficients in canals are affected by two main factors, namely, flow conditions and vegetation characteristics [68]. So far, much research has been done on the effect of the roughness factor created by vegetation, but the issue of plant density has received less attention. For this purpose, this study was conducted to investigate the effect of vegetation density on flow velocity changes.In a study conducted using a software model on three density modes in the submerged state effect on flow velocity changes in 48 different modes was investigated (Table1).Table 1
The studied models.
Model indexStudy modelsZGHydraulic depthInput speedFroude numberPlant densityManning coefficient based on Chow's experiencesModel1-V3-Ch 0.03Model 119.810.8831.0164090.250.03Model2-V3-Ch 0.035Model 219.810.8831.0164090.50.035Model3-V3-Ch 0.04Model 319.810.8831.0164090.750.04Model4-V3-Ch 0.02Model 419.810.8831.01640900.02Model5-V3.1-Ch 0.03Model 519.810.883.11.05028930.250.03Model6-V3.1-Ch 0.035Model 619.810.883.11.05028930.50.035Model7-V3.1-Ch 0.04Model 719.810.883.11.05028930.750.04Model8-V3.1-Ch 0.02Model 819.810.883.11.050289300.02Model9-V3.2-Ch 0.03Model 919.810.883.21.08416960.250.03Model10-V3.2-Ch 0.035Model 1019.810.883.21.08416960.50.035Model11-V3.2-Ch 0.04Model 1119.810.883.21.08416960.750.04Model12-V3.2-Ch 0.02Model 1219.810.883.21.084169600.02Model13-V3.3-Ch 0.03Model 1319.810.883.31.11804990.250.03Model14-V3.3-Ch 0.035Model 1419.810.883.31.11804990.50.035Model15-V3.3-Ch 0.04Model 1519.810.883.31.11804990.750.04Model16-V3.3-Ch 0.02Model 1619.810.883.31.118049900.02Model17-V4-Ch 0.03Model 1729.811.4641.0554553380.250.03Model18-V4-Ch 0.035Model 1829.811.4641.0554553380.50.035Model19-V4-Ch 0.04Model 1929.811.4641.0554553380.750.04Model20-V4-Ch 0.02Model 2029.811.4641.05545533800.02Model21-V4.1-Ch 0.03Model 2129.811.464.11.0818417210.250.03Model22-V4.1-Ch 0.035Model 2229.811.464.11.0818417210.50.035Model23-V4.1-Ch 0.04Model 2329.811.464.11.0818417210.750.04Model24-V4.1-Ch 0.02Model 2429.811.464.11.08184172100.02Model25-V4.2-Ch 0.03Model 2529.811.464.21.1082281050.250.03Model26-V4.2-Ch 0.035Model 2629.811.464.21.1082281050.50.035Model27-V4.2-Ch 0.04Model 2729.811.464.21.1082281050.750.04Model28-V4.2-Ch 0.02Model 2829.811.464.21.10822810500.02Model29-V4.3-Ch 0.03Model 2929.811.464.31.1346144880.250.03Model30-V4.3-Ch 0.035Model 3029.811.464.31.1346144880.50.035Model31-V4.3-Ch 0.04Model 3129.811.464.31.1346144880.750.04Model32-V4.3-Ch 0.02Model 3229.811.464.31.13461448800.02Model33-V5-Ch 0.03Model 3339.811.9151.1530229080.250.03Model34-V5-Ch 0.035Model 3439.811.9151.1530229080.50.035Model35-V5-Ch 0.04Model 3539.811.9151.1530229080.750.04Model36-V5-Ch 0.02Model 3639.811.9151.15302290800.02Model37-V5.1-Ch 0.03Model 3739.811.915.11.1760833660.250.03Model38-V5.1-Ch 0.035Model 3839.811.915.11.1760833660.50.035Model39-V5.1-Ch 0.04Model 3939.811.915.11.1760833660.750.04Model40-V5.1-Ch 0.02Model 4039.811.915.11.17608336600.02Model41-V5.2-Ch 0.03Model 4139.811.915.21.1991438250.250.03Model42-V5.2-Ch 0.035Model 4239.811.915.21.1991438250.50.035Model43-V5.2-Ch 0.04Model 4339.811.915.21.1991438250.750.04Model44-V5.2-Ch 0.02Model 4439.811.915.21.19914382500.02Model45-V5.3-Ch 0.03Model 4539.811.915.31.2222042830.250.03Model46-V5.3-Ch 0.035Model 4639.811.915.31.2222042830.50.035Model47-V5.3-Ch 0.04Model 4739.811.915.31.2222042830.750.04Model48-V5.3-Ch 0.02Model 4839.811.915.31.22220428300.02The number of cells used in this simulation is equal to 1955888 cells. The boundary conditions were introduced to the model as a constant speed and depth (Figure1). At the output boundary, due to the presence of supercritical current, no parameter for the current is considered. Absolute roughness for floors and walls was introduced to the model (Figure 1). In this case, the flow was assumed to be nonviscous and air entry into the flow was not considered. After 7.7×10−4 seconds, this model reached a convergence accuracy of 2.39×10−5.Figure 1
The simulated model and its boundary conditions.Due to the fact that it is not possible to model the vegetation in FLOW-3D software, in this research, the vegetation of small soft plants was studied so that Manning’s coefficients can be entered into the canal bed in the form of roughness coefficients obtained from the studies of Chow [69] in similar conditions. In practice, in such modeling, the effect of plant height is eliminated due to the small height of herbaceous plants, and modeling can provide relatively acceptable results in these conditions.48 models with input velocities proportional to the height of the regular semihexagonal canal were considered to create supercritical conditions. Manning coefficients were applied based on Chow [69] studies in order to control the canal bed. Speed profiles were drawn and discussed.Any control and simulation system has some inputs that we should determine to test any technology [70–77]. Determination and true implementation of such parameters is one of the key steps of any simulation [23, 78–81] and computing procedure [82–86]. The input current is created by applying the flow rate through the VFR (Volume Flow Rate) option and the output flow is considered Output and for other borders the Symmetry option is considered.Simulation of the models and checking their action and responses and observing how a process behaves is one of the accepted methods in engineering and science [87, 88]. For verification of FLOW-3D software, the results of computer simulations are compared with laboratory measurements and according to the values of computational error, convergence error, and the time required for convergence, the most appropriate option for real-time simulation is selected (Figures 2 and 3 ).Figure 2
Modeling the plant with cylindrical tubes at the bottom of the canal.Figure 3
Velocity profiles in positions 2 and 5.The canal is 7 meters long, 0.5 meters wide, and 0.8 meters deep. This test was used to validate the application of the software to predict the flow rate parameters. In this experiment, instead of using the plant, cylindrical pipes were used in the bottom of the canal.The conditions of this modeling are similar to the laboratory conditions and the boundary conditions used in the laboratory were used for numerical modeling. The critical flow enters the simulation model from the upstream boundary, so in the upstream boundary conditions, critical velocity and depth are considered. The flow at the downstream boundary is supercritical, so no parameters are applied to the downstream boundary.The software well predicts the process of changing the speed profile in the open canal along with the considered obstacles. The error in the calculated speed values can be due to the complexity of the flow and the interaction of the turbulence caused by the roughness of the floor with the turbulence caused by the three-dimensional cycles in the hydraulic jump. As a result, the software is able to predict the speed distribution in open canals.


## 2. Modeling Results

After analyzing the models, the results were shown in graphs (Figures4–14 ). The total number of experiments in this study was 48 due to the limitations of modeling.Figure 4
Flow velocity profiles for canals with a depth of 1 m and flow velocities of 3–3.3 m/s. Canal with a depth of 1 meter and a flow velocity of (a) 3 meters per second, (b) 3.1 meters per second, (c) 3.2 meters per second, and (d) 3.3 meters per second.
(a)(b)(c)(d)Figure 5
Canal diagram with a depth of 1 meter and a flow rate of 3 meters per second.Figure 6
Canal diagram with a depth of 1 meter and a flow rate of 3.1 meters per second.Figure 7
Canal diagram with a depth of 1 meter and a flow rate of 3.2 meters per second.Figure 8
Canal diagram with a depth of 1 meter and a flow rate of 3.3 meters per second.Figure 9
Flow velocity profiles for canals with a depth of 2 m and flow velocities of 4–4.3 m/s. Canal with a depth of 2 meters and a flow rate of (a) 4 meters per second, (b) 4.1 meters per second, (c) 4.2 meters per second, and (d) 4.3 meters per second.
(a)(b)(c)(d)Figure 10
Canal diagram with a depth of 2 meters and a flow rate of 4 meters per second.Figure 11
Canal diagram with a depth of 2 meters and a flow rate of 4.1 meters per second.Figure 12
Canal diagram with a depth of 2 meters and a flow rate of 4.2 meters per second.Figure 13
Canal diagram with a depth of 2 meters and a flow rate of 4.3 meters per second.Figure 14
Flow velocity profiles for canals with a depth of 3 m and flow velocities of 5–5.3 m/s. Canal with a depth of 2 meters and a flow rate of (a) 4 meters per second, (b) 4.1 meters per second, (c) 4.2 meters per second, and (d) 4.3 meters per second.
(a)(b)(c)(d)To investigate the effects of roughness with flow velocity, the trend of flow velocity changes at different depths and with supercritical flow to a Froude number proportional to the depth of the section has been obtained.According to the velocity profiles of Figure5, it can be seen that, with the increasing of Manning’s coefficient, the canal bed speed decreases.According to Figures5 to 8, it can be found that, with increasing the Manning’s coefficient, the canal bed speed decreases. But this deceleration is more noticeable than the deceleration of the models 1 to 12, which can be justified by increasing the speed and of course increasing the Froude number.According to Figure10, we see that, with increasing Manning’s coefficient, the canal bed speed decreases.According to Figure11, we see that, with increasing Manning’s coefficient, the canal bed speed decreases. But this deceleration is more noticeable than the deceleration of Figures 5–10, which can be justified by increasing the speed and, of course, increasing the Froude number.With increasing Manning’s coefficient, the canal bed speed decreases (Figure12). But this deceleration is more noticeable than the deceleration of the higher models (Figures 5–8 and 10, 11), which can be justified by increasing the speed and, of course, increasing the Froude number.According to Figure13, with increasing Manning’s coefficient, the canal bed speed decreases. But this deceleration is more noticeable than the deceleration of Figures 5 to 12, which can be justified by increasing the speed and, of course, increasing the Froude number.According to Figure15, with increasing Manning’s coefficient, the canal bed speed decreases.Figure 15
Canal diagram with a depth of 3 meters and a flow rate of 5 meters per second.According to Figure16, with increasing Manning’s coefficient, the canal bed speed decreases. But this deceleration is more noticeable than the deceleration of the higher model, which can be justified by increasing the speed and, of course, increasing the Froude number.Figure 16
Canal diagram with a depth of 3 meters and a flow rate of 5.1 meters per second.According to Figure17, it is clear that, with increasing Manning’s coefficient, the canal bed speed decreases. But this deceleration is more noticeable than the deceleration of the higher models, which can be justified by increasing the speed and, of course, increasing the Froude number.Figure 17
Canal diagram with a depth of 3 meters and a flow rate of 5.2 meters per second.According to Figure18, with increasing Manning’s coefficient, the canal bed speed decreases. But this deceleration is more noticeable than the deceleration of the higher models, which can be justified by increasing the speed and, of course, increasing the Froude number.Figure 18
Canal diagram with a depth of 3 meters and a flow rate of 5.3 meters per second.According to Figure19, it can be seen that the vegetation placed in front of the flow input velocity has negligible effect on the reduction of velocity, which of course can be justified due to the flexibility of the vegetation. The only unusual thing is the unexpected decrease in floor speed of 3 m/s compared to higher speeds.Figure 19
Comparison of velocity profiles with the same plant densities (depth 1 m). Comparison of velocity profiles with (a) plant densities of 25%, depth 1 m; (b) plant densities of 50%, depth 1 m; and (c) plant densities of 75%, depth 1 m.
(a)(b)(c)According to Figure20, by increasing the speed of vegetation, the effect of vegetation on reducing the flow rate becomes more noticeable. And the role of input current does not have much effect in reducing speed.Figure 20
Comparison of velocity profiles with the same plant densities (depth 2 m). Comparison of velocity profiles with (a) plant densities of 25%, depth 2 m; (b) plant densities of 50%, depth 2 m; and (c) plant densities of 75%, depth 2 m.
(a)(b)(c)According to Figure21, it can be seen that, with increasing speed, the effect of vegetation on reducing the bed flow rate becomes more noticeable and the role of the input current does not have much effect. In general, it can be seen that, by increasing the speed of the input current, the slope of the profiles increases from the bed to the water surface and due to the fact that, in software, the roughness coefficient applies to the channel floor only in the boundary conditions, this can be perfectly justified. Of course, it can be noted that, due to the flexible conditions of the vegetation of the bed, this modeling can show acceptable results for such grasses in the canal floor. In the next directions, we may try application of swarm-based optimization methods for modeling and finding the most effective factors in this research [2, 7, 8, 15, 18, 89–94]. In future, we can also apply the simulation logic and software of this research for other domains such as power engineering [95–99].Figure 21
Comparison of velocity profiles with the same plant densities (depth 3 m). Comparison of velocity profiles with (a) plant densities of 25%, depth 3 m; (b) plant densities of 50%, depth 3 m; and (c) plant densities of 75%, depth 3 m.
(a)(b)(c)


## 3. Conclusion

The effects of vegetation on the flood canal were investigated by numerical modeling with FLOW-3D software. After analyzing the results, the following conclusions were reached:(i)
Increasing the density of vegetation reduces the velocity of the canal floor but has no effect on the velocity of the canal surface.(ii)
Increasing the Froude number is directly related to increasing the speed of the canal floor.(iii)
In the canal with a depth of one meter, a sudden increase in speed can be observed from the lowest speed and higher speed, which is justified by the sudden increase in Froude number.(iv)
As the inlet flow rate increases, the slope of the profiles from the bed to the water surface increases.(v)
By reducing the Froude number, the effect of vegetation on reducing the flow bed rate becomes more noticeable. And the input velocity in reducing the velocity of the canal floor does not have much effect.(vi)
At a flow rate between 3 and 3.3 meters per second due to the shallow depth of the canal and the higher landing number a more critical area is observed in which the flow bed velocity in this area is between 2.86 and 3.1 m/s.(vii)
Due to the critical flow velocity and the slight effect of the roughness of the horseshoe vortex floor, it is not visible and is only partially observed in models 1-2-3 and 21.(viii)
As the flow rate increases, the effect of vegetation on the rate of bed reduction decreases.(ix)
In conditions where less current intensity is passing, vegetation has a greater effect on reducing current intensity and energy consumption increases.(x)
In the case of using the flow rate of 0.8 cubic meters per second, the velocity distribution and flow regime show about 20% more energy consumption than in the case of using the flow rate of 1.3 cubic meters per second.



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*Source: 9048808-2021-08-11.xml*