Abstract
Hydraulic jump is of fast altering flow type, within which a critical flow transforms into a subcritical flow, and such alteration occurs within a relatively short path of the channel. In the present study, the impact of lateral angles of trapezoidal channel walls in the continuous form on the relative loss of hydraulic jump energy is investigated. For this purpose, the meta-heuristic harmony search algorithm is used for declaring the continuous lateral angles within the range of 45°–75°. With regard to the hydraulic definition for the hydraulic jump phenomenon, the harmony search algorithm, which is widely used for optimization and continuous problems, is considered as a simple concept of a useful algorithm. The results demonstrated the high efficiency of harmony search in the optimization of hydraulic problems. The highest value of jump energy loss up to 81% was recorded for the angle of 45°, implying the high efficiency of this section. As can be clearly seen in the results, the amount of destructive energy loss of hydraulic jump in the meta-heuristic algorithm is significantly higher than other previous methods.
HIGHLIGHTS
In the present study, the impact of lateral angles of trapezoidal channel walls in the continuous form on the relative loss of hydraulic jump energy is investigated. For this purpose, the meta-heuristic harmony search algorithm is used for declaring the continuous lateral angles with the range of 45°–75°.
Continuously assuming trapezoidal channel angles in this research has been one of the most impressive functions of this algorithm.
At the angle of 45 degrees, the highest amount of hydraulic jump energy loss has been shown compared to other responses obtained from the algorithm.
NOMENCLATURE
- b
Base width (m)
- Q
Discharge (L/s)
- y1
First depth of the hydraulic jump (m)
- y2
Secondary depth of the hydraulic jump (m)
- m
Cotangent of the side slope
- Fr2
Froude number before the hydraulic jump (−)
- E1
Energy loss before the hydraulic jump (m)
- E2
Energy loss after the hydraulic jump (m)
- ΔE
E1 − E2 = EL
- g
Acceleration of gravity (m/s2)
- V1
Velocity of flow before the hydraulic jump (m/s)
- V2
Velocity of flow after the hydraulic jump (m/s)
- RL
Relative energy loss (%)
INTRODUCTION
![](https://iwa.silverchair-cdn.com/iwa/content_public/journal/aqua/72/8/10.2166_aqua.2023.074/4/m_aquawies-d-23-00074if01.gif?Expires=1739877193&Signature=qKCku5fOtNFtftk-vd5KIrhpsze~W8Lhmk6bpDC7fBFVXNZA89NdzzHXe~C-7H~OmdeLCHnfRcpHitEbO6PSt-96HB-faNi23WtY6CcbSP8D5neEA23czaW8mP828kWdFubWIYz163DEpVyEKw2O-Hb7WyZhKF01KUurC51pImLNIMnGub6RF-YfFp8don2G5snkmL00GV78bnx~JfSiN-t45yZ0M1mpbjogLoRqCExqfNRGx7ex-9J6RymGtPbuQ91aXaBzXPdvnQXzFdGQkyX-Grrg91sxP-VFZSGdP86UIzkZlq-5gCcxna7GH4ZsZ4GUi7XYBtU64bqRAlq51w__&Key-Pair-Id=APKAIE5G5CRDK6RD3PGA)
General structure of the hydraulic jump within a horizontal channel.
Meta-heuristic method
Harmony search is a meta-heuristic method used for optimizing hydraulic structures. It was developed in 2001 and is one of the newest and simplest meta-heuristic methods. The algorithm is inspired by the simultaneous playing of music and is a desirable method for routing in the sensor network. It is a powerful algorithm with excellent exploitation capabilities, and it can find solutions to optimization problems.
The meta-heuristic methods use the information obtained from the former point as the guidance for selecting the next point(s). These methods are known as the optimization algorithms that seek to establish a balance between the diversification in the search space and results intensification. These methods are capable of solving various problems, regardless of the good behavior of the objective function or whether the search space is discrete or continuous.
Evolutionary algorithms
This algorithm is known as a music-inspired harmony search algorithm. Indeed, the main purpose of harmony search is to find a relation between the musical notes and the optimal solution for a difficult engineering problem. This algorithm was proposed by Geem et al. (2001). An HS algorithm is inspired from the search mechanism used for reaching a full harmony in the music. That is, a musician attempts to generate thoroughly harmonic music free from any deficiency. The quality, beauty, and the elegance of musical instruments are intrinsically determined by the pitch (sound frequency), resonance (sound quality), and amplitude (sound loudness).
Steps of harmony search algorithm
In the present research, the lateral angle of the trapezoidal channel is taken into account as the continuous variable, while the flow discharge is considered as a variable, and Table 1 presents the associated properties and calculation order.
Flow discharge order used in the present study
Row . | Discharge (L/s) . | Side slope range . |
---|---|---|
1 | 90 | 0.26 ≤ m ≤ 1.0 |
2 | 70 | 0.26 ≤ m ≤ 1.0 |
3 | 50 | 0.26 ≤ m ≤ 1.0 |
4 | 30 | 0.26 ≤ m ≤ 1.0 |
5 | 10 | 0.26 ≤ m ≤ 1.0 |
Row . | Discharge (L/s) . | Side slope range . |
---|---|---|
1 | 90 | 0.26 ≤ m ≤ 1.0 |
2 | 70 | 0.26 ≤ m ≤ 1.0 |
3 | 50 | 0.26 ≤ m ≤ 1.0 |
4 | 30 | 0.26 ≤ m ≤ 1.0 |
5 | 10 | 0.26 ≤ m ≤ 1.0 |
As seen in the flow chart, if a new harmony is better than the worst member, the new harmony will be appended to the memory, and the order is updated, until the moment that the terminating condition is met; otherwise, it returns to the phase, which is responsible for creating a new harmony and such a cycle continues.
Governing equations of relative energy dissipation
![](https://iwa.silverchair-cdn.com/iwa/content_public/journal/aqua/72/8/10.2166_aqua.2023.074/4/m_aquawies-d-23-00074if02.gif?Expires=1739877193&Signature=qzOCYG6j5xLUF-pIptuDZSku7Nroz1EjYJTNoXpPJL4cHfp~B-0IMru2wkLY7V93-FEpbY8jH25tvZFZwyUyPVoRd7b0Nj3XUpQY2n6zzoaQQOhULb5IqXMvvOcCZba61lB9H3IuI~HyCrm~gLv5ChrlM95uiJJ43a6ADmBCC2T6sc5H7zEbL3-ElU3dxyi-ViidcNNPJr6or9YlWY8jAsPOsVdcea6Vu7LxItt80IHmB6wAw6GhUACk1kN0BX3x~s0cE7up4pNOUgTPyuNJ7wN6CJXailwAl~XFSrW-iRAYrzXhKSQsKdN3LtLN5ELMeYHt82gZS1jrQZg4WlOIcw__&Key-Pair-Id=APKAIE5G5CRDK6RD3PGA)
As seen, the relative energy dissipation for a hydraulic jump is dependent on parameters such as Froude number, flow cross-section, and conjunctive depths. Of course, it should be noted that the value of flow cross-section for the trapezoidal channels alters along with changes in the lateral angle of the channel wall.
RESULTS AND DISCUSSION
Schematic of the trapezoidal channel incorporating the lateral angle.
Side slope range
From a hydraulic consideration perspective, the trapezoidal channels are cost-effective and more practical, compared to the other channels; as a result, the side slope of the trapezoidal channel is determined based on the soil type and vegetation. Hence, the side slope of the buried channels is considered to be steeper than that of the channels deployed on the embankment. For huge and highly deep channels, the side slope of the section associated with the free board can be considered steeper than that of the underwater area. The side slope of the coated channels is usually steeper than the non-coated channels.
As noted, all angles between 45° and 75° are scrutinized, that is, the continuous distance of angles is taken into account, while the experimental or numerical studies are merely capable of using a limited number of the angles, which may result in constrained results. The continuous feature of the lateral angles boosts the energy field efficiency of the hydraulic jump, which is relative to the various flow discharges. In this research, five stream discharges, as presented in Table 1, are used.
As seen in Table 1, the angle in the range of 45°–75° for the side wall of the channel and all discharge rates are studied.
The geometrical properties of the channel are presented in Table 2.
Geometrical properties of the study channel
Section type . | Width of channel bottom (m) . | Water height in the channel (m) . |
---|---|---|
0.26 ≤ m ≤ 1.0 | 0.2 | 0.45 |
Section type . | Width of channel bottom (m) . | Water height in the channel (m) . |
---|---|---|
0.26 ≤ m ≤ 1.0 | 0.2 | 0.45 |
Generally, an optimal model is characterized by three sections as below:
- (1)
Objective function
- (2)
Constraints
- (3)
Decision-making variables
Pseudocode for geometrical section optimization in trapezoidal channels.
In the present research, the coding phase considers the aforementioned sections. The harmony development is realized in two modes based on the HMCR probability using the HM components and the HMCR probability using random numbers.
Changes in the relative energy dissipation of the hydraulic jump relative to the continuous lateral angle for 90 L/s discharge.
Changes in the relative energy dissipation of the hydraulic jump relative to the continuous lateral angle for 90 L/s discharge.
Changes in the relative energy dissipation of the hydraulic jump relative to the continuous lateral angle for 70 L/s discharge.
Changes in the relative energy dissipation of the hydraulic jump relative to the continuous lateral angle for 70 L/s discharge.
Changes in the relative energy dissipation of the hydraulic jump relative to the continuous lateral angle for 50 L/s discharge.
Changes in the relative energy dissipation of the hydraulic jump relative to the continuous lateral angle for 50 L/s discharge.
Changes in the relative energy dissipation of the hydraulic jump relative to the continuous lateral angle for 30 L/s discharge.
Changes in the relative energy dissipation of the hydraulic jump relative to the continuous lateral angle for 30 L/s discharge.
Changes in the relative energy dissipation of the hydraulic jump relative to the continuous lateral angle for 10 L/s discharge.
Changes in the relative energy dissipation of the hydraulic jump relative to the continuous lateral angle for 10 L/s discharge.
The reason for the breakdown of the energy loss graph in the range of 60° from the hydraulic channel was because the calculation process of the algorithm was based on the continuous method, and usually the algorithm reviews the best answers in the range between the two banks of minimum and maximum. For this reason, a break in the trend of the chart can be seen in this range, but there has been no change in the overall trend of the result. As can be clearly seen in the results, the amount of destructive energy loss of hydraulic jump in the meta-heuristic algorithm is significantly higher than other previous methods. Therefore, the effectiveness of this method in examining macroscopic hydraulic problems is much higher and this method can be considered a better alternative to previous numerical methods. As can be seen in Figures 6–10, the slope of the hydraulic jump energy drop line was much higher at angles of 45°, and this energy drop was directly related to the Froude number, that is, the higher the Froude number, the greater the drop. With regard to the presented curves, it can be deduced that the horizontal axis of the variation curve for the lateral angle of the channel wall ranging from 45° to 75° is continuous and the vertical axis of the relative energy dissipation in the hydraulic jump is per percent. In the curve of Figure 6 for the discharge rate of 90 L/s, the maximum relative energy dissipation of jump with a value of 81% is attributed to the 45° section, which is considered as the highest relative energy dissipation.
Comprehensible comparison of the results with previous researches
Row . | Research's report . | Description . | Results . |
---|---|---|---|
1 | Fatehi-Nobarian et al. (2019) | It has been done in trapezoidal channels with a 45° side wall, experimentally on the hydraulic jump | In Froude number 4, 40% of hydraulic jump energy has been reduced. And the same process has continued with the increase in the Froude number. |
2 | Wanoschek & Hager (1989) | It has been done in trapezoidal channels with a 45° side wall, experimentally on the hydraulic jump | In Froude number 4, 36% of hydraulic jump energy has been reduced. |
3 | Present study | The influence of the changes of the (continuous) side angles of the trapezoidal channels. | In Froude number 4, 47% of hydraulic jump energy has been reduced. And the same process has continued with the increase in the Froude number. |
4 | Fatehi-Nobarian et al. (2022) | The influence of the geometric cross-section of the semicircular on the energy loss of the jump has been done. | With the increase of Froude number, the energy loss of hydraulic jump has increased. |
5 | Kim et al. (2015) | The hydraulic jump and energy dissipation in the classic section have been done. | With the increase in the length of the jump, the energy loss of the hydraulic jump has also increased. |
Row . | Research's report . | Description . | Results . |
---|---|---|---|
1 | Fatehi-Nobarian et al. (2019) | It has been done in trapezoidal channels with a 45° side wall, experimentally on the hydraulic jump | In Froude number 4, 40% of hydraulic jump energy has been reduced. And the same process has continued with the increase in the Froude number. |
2 | Wanoschek & Hager (1989) | It has been done in trapezoidal channels with a 45° side wall, experimentally on the hydraulic jump | In Froude number 4, 36% of hydraulic jump energy has been reduced. |
3 | Present study | The influence of the changes of the (continuous) side angles of the trapezoidal channels. | In Froude number 4, 47% of hydraulic jump energy has been reduced. And the same process has continued with the increase in the Froude number. |
4 | Fatehi-Nobarian et al. (2022) | The influence of the geometric cross-section of the semicircular on the energy loss of the jump has been done. | With the increase of Froude number, the energy loss of hydraulic jump has increased. |
5 | Kim et al. (2015) | The hydraulic jump and energy dissipation in the classic section have been done. | With the increase in the length of the jump, the energy loss of the hydraulic jump has also increased. |
Variation in the relative energy dissipation of the hydraulic jump compared to shifts in the Froude number for m = 1.0.
Variation in the relative energy dissipation of the hydraulic jump compared to shifts in the Froude number for m = 1.0.
For more proper validation of the results obtained from the optimization algorithm, these results are compared with that of the previous studies (Figure 11).
Normally, in the investigation of energy loss in trapezoidal channels, the experimental results of Wanoschek and Hager for an angle of 45° are considered as a benchmark, and the same process has been done in this research, and apart from that, the results of the algorithm with the experimental results of Fathi-Nobarian et al. have been evaluated. With regard to the results of Wanoschek & Hager (1989) for the 45° section, the comparison and validation are accomplished for a section of m = 1.0 between the experimental results of Fatehi-Nobarian et al. (2019) and the numerical results derived from Flow-3D software for the Froude number in the range of 1.7–9. Accordingly, the results obtained by the HS algorithm indicate 6% increase, compared to that of experimental results presented by Fatehi-Nobarian et al. (2019). The results derived from the harmony search algorithm are consistent with experimental results obtained by Wanoschek & Hager (1989) and Fatehi-Nobarian et al. (2019), which refers to the fact that the proposed method exhibited a desirable performance.
CONCLUSION
The limitations of the performed method are only for classic sections, because in rectangular sections there is no side angles for the channel walls, while the potential field of the method used in this research is its ability to be expanded for all channels whose side walls have an angle. It is variable or has radial adjustments for circular geometric sections, because nowadays most of the flow channels in dams and upstream plains are designed from trapezoidal sections. With regard to the results, it can be concluded that the behavior of trapezoidal channels using various side slopes is different from the channels with non-trapezoidal sections. The trapezoidal channels with the wall slope of 45° exhibited a better behavior.
At the 45° section, the flow moves slowly near the surface and is directed toward the side walls due to the formation of the rolling zone at the bottom. The flow can include higher air due to the adequate opening in the wall at an angle of 45°, leading to relative energy dissipation in the hydraulic jump for these sections, even for higher discharge rates.
Compared to the preceding numerical studies, the results obtained for geometrical section optimization of the trapezoidal channels using the harmony search algorithm ascertained the efficiency of HSA.
For a discharge rate of 90 L/s, the highest relative energy dissipation (81.6%) in the hydraulic jump is attained at the 45° section, which demonstrated the considerable efficiency of these sections.
For other geometrical sections of the channel, the following results are obtained for discharge rates of 70, 50, 30, and 10 L/s, and the relative energy dissipation in jump was equal to 71.3, 53, 20, and 9%, respectively, implying that the higher side slope (m) of the trapezoidal channel leads to a higher increase in energy dissipation.
The present optimization results were compared to previous research, and it was found that there is a 6 and 10% increase relative to the experimental research conducted by Wanoschek & Hager (1989) and Fatehi-Nobarian et al. (2019), and the results of Flow-3D. These values indicate a desirable agreement between the results and the validation, all of which refer to the efficiency of harmony search algorithm for studying the relative energy dissipation in the hydraulic jump phenomenon.
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.