Comparison between 2D and 3D Hydraulic Modelling Approaches for Simulation of Vertical Slot Fishways

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5 th International Symposium on Hydraulic Structures Brisbane, Australia, 25-27 June 2014 Hydraulic Structures and Society: Engineering Challenges and Extremes ISBN 9781742721156 - DOI: 10.14264/uql.2014.49 Comparison between 2D and 3D Hydraulic Modelling Approaches for Simulation of Vertical Slot Fishways C.S. Lauchlan Arrowsmith 1, Y. Zhu 1 1 Water Technology Melbourne, VIC 3168 AUSTRALIA E-mail: christine.arrowsmith@watertech.com.au Abstract: The performance of a fishway is heavily dependent on the interplay between the hydraulic properties of the structure and adjacent waterway, and the biological variables of the targeted fish species. The optimal parameters for a vertical slot fishway such as the step height and opening size are usually difficult to obtain. To date Water Technology have utilised a 2D hydraulic modelling tool (MIKE21) to understand and design these structures. The limitation of this 2D modelling approach is the assumption of a uniform vertical velocity distribution and at fine grid scales inconsistencies in velocity and turbulence estimates provided by such models have been noted. To improve the ability to resolve fine scale velocity distributions and turbulence structures to the level required for fishway design the fully 3D modelling hydrodynamic package ANSYS CFX was used to model an existing fishway design. This allowed enhanced resolution and therefore understanding of the velocity distribution and turbulence structure within the fishway and provided a direct comparison between the 2D and 3D approaches. Based on the outcomes of this assessment a generalised design approach has been developed for vertical slot fishways, which will improve the understanding of the hydraulic properties of each structure, and the adjacent waterway and improve our ability to meet the specific requirements of Australian fish species. Keywords: fishway, hydraulic modelling, turbulence, CFD modelling 1. INTRODUCTION Fishways (also known as fish ladders) are hydraulic structures used to facilitate migratory fish to overcome obstacles, such as dams, in regulated waterways. The first recorded fishway can be dated back to the 17th Century in Europe (Alvarez-Vázquez, Martínez et al. 2008). In Australia, significant research efforts have been undertaken with a number of fishways designed and constructed to preserve and enhance the natural stocks for the whole native fish communities, including catadromy, amphidromy and potamodromy (Stuart, Zampatti et al. 2008). Fishways come in a range of forms including pool types (e.g. vertical slot), denil fishways, and rock ramp fishways. The vertical-slot fishway consists of rectangular channels with sloping or stepped floors that are divided into several pools (Alvarez-Vázquez, Martínez et al. 2007). The water flow forms a jet at the slot and the energy is dissipated by mixing in the pool (Rajaratnam, Van der Vinne et al. 1986). The main challenge in a fishway design is to integrate the conservative fishway hydraulics with highly variable water level (Stuart, Zampatti et al. 2008). The hydraulic conditions suitable for Australian native fish are well established; however, the hydraulic and fish passage performance of fishways under various conditions (such as flow rates and tail water levels) has been difficult to gauge. Importantly, fishways are expensive to build and modify or replace if found not to be functioning to the design specification. Hydraulic modelling provides a convenient and cost-effective means to characterize and predict the behaviours of environmental systems (Karisch and Power 1994). The performance of a fishway is heavily dependent on the interplay between the hydraulic properties of the structure and adjacent waterway and the biological variables of the targeted fish species. The optimal parameters for a vertical slot fishway, such as the step height and opening size, are usually difficult to obtain. To date Water Technology have utilised a 2D hydraulic modelling tool (MIKE21) to understand and design these systems. A limitation of this 2D modelling approach is that a uniform vertical velocity distribution is assumed and at fine grid scales inconsistencies in velocity and

turbulence estimates can occur. To improve the ability to resolve fine scale velocity distributions and turbulence to the level required for fishway design a fully 3D computation fluid dynamics package (ANSYS CFX) was used to simulate an existing vertical slot fishway design, which was then compared with the original 2D model results and comparisons drawn between the flow patterns, velocities and turbulence structures produced. 2. FISHWAY DESIGN & ANALYSIS 2.1. Review of Previous Design A vertical slot fishway design was previously developed for a site on the Thomson River near Cowwarr, West Gippsland, Victoria. The site comprised an existing flow gauging station weir, which formed a barrier to the migration of fish due to supercritical velocities over the weir crest. A range of options were investigated as to the most appropriate fishway design for the site, including removal of the weir and regrading of the existing rock ramp fishway; combining a full width rock ramp with a vertical slot fishway; and using a pre-fabricated vertical slot fishway with a rock chute. Site constraints, such as access load limitations and the requirement to maintain the weir crest elevation and flow discharge capacity meant that the pre-fabricated vertical slot design was adopted as most appropriate for the site. From a review of fish monitoring data, critical hydraulic parameters to cater for successful migration of the fifteen native and six non-native fish species present in the river were determined to be maximum velocities of 1 m/s and energy dissipation factor within the fishway cells in the order of 40 W/m 3 or lower. Two preliminary designs developed for the vertical slot fishway and are detailed in Zhu et al. (2011). For this comparison assessment only Design A, as shown in Figure 1 and Figure 2, was modeled. This design consisted of five 1200 x 900 mm box culverts placed in steps, separated by the 150 mm wide vertical slots. 4 3 2 1 Figure 1 Plan View of Vertical Slot Fishway Design (Design A)

Figure 2 Side Elevation of Vertical Slot Fishway Design (Design A) 2.2. 2D Modelling The MIKE21 modelling package by DHI was used for analysis of the original design. The model inputs included a 2D square grid representing the geometry of the structure, a set of initial and boundary conditions, as well as other computational parameters such as Manning s coefficients and eddy viscosity. A 5 cm grid size was adopted; the boundary condition conditions consisted of two constant water levels. The water levels were determined by a broader scale 2D hydraulic study of the river system at the subject site. The provision of an environmental flow to the Thomson River ensures that the headwater level is relatively constant at or below 99.82 m. A constant water surface level 99.5 m was applied to the downstream water level boundary. The Manning s coefficient value used for the model was 0.045. The eddy viscosity used for the model was velocity based Smagorinsky formulation with a coefficient of 0.5. The model outputs were analyzed in terms of water depths and velocities through the structure, and the energy dissipation factor (P/V) was computed. The energy dissipation factor is an indicator of biological efficiency of the fishway. Fish tend to struggle to orient themselves when there is excessive turbulence. Their respiration may also be disturbed if there is an abundance of large air bubbles (Rodríguez, Agudo et al. 2006). Yagci (2010) reviewed and documented the maximum energy dissipation factor for an effective vertical slot fishway from a range of literature. It was suggested that the maximum energy dissipation should not exceed 150 W/m 3 for smaller North American fish species. It is recognised that small bodied Australian Native fish are impeded by energy dissipation factors above 40 W/m 3. The resultant water level and flow velocity distribution for Design A is shown in Figure 3 and Figure 4. The design was estimated to provide a discharge of 33.2 L/s and P/V of 41.4 W/m 3. Figure 3 Resultant Water Depth Distribution from 2D Model (Design A)

Figure 4 Resultant Velocity Distribution from 2D Model (Design A) 2.3. CFD Modelling The fully 3D hydrodynamic modelling package ANSYS CFX was used to develop a fishway model for this study. CFX is a general purpose fluid dynamics programs that has been applied to solve wideranging fluid flow problems, such as environmental, motor industry, process industry and medical. The model domain was created using the DesignModeler tool and contained 334,572 elements, with a minimum size of 1 mm. A roughness height of 0.01 m was applied for the bottom, and the side walls as being concrete were considered to be hydraulically smooth. The atmospheric pressure was set to be 1 atm. The same constant water level boundary conditions were applied, and the shear stress transport turbulence model was used in the simulations. The resultant flow velocity distribution and turbulent energy dissipation rate for Design A is shown in Figure 5 to Figure 8. Figure 5 Resultant Velocity Distribution from 3D Model (Design A) Figure 6 Resultant area where the energy disspation factor (P/V) is less than 40 W/m 3

Figure 7 Resultant Energy Dissipation Factor from the 3D Model (Design A) Figure 8 Resultant Water Depth from the 3D Model (Design A) 3. DISCUSSION 3.1. Model Setup and Simulation Times The initial setup of the CFX model was more complicated and time consuming that the 2D MIKE21 model. However, once the model was configured, the meshing algorithms in ANSYS CFX are more flexible making it easier to modify design parameters of the structure, such as slot lengths and angles without regeneration of the model mesh and boundaries. To modify the design in the 2D model required a new model grid to be constructed. For the simulation of Design A, the simulation in ANSYS CFX took approximately 4 hours, which was around 4 times longer than the time required to complete the 2D simulation. 3.2. Model Results 3.2.1. Depths and Velocities A comparison of the average water depths and velocities is provided in Table 1. Overall, the 3D model results show significantly lower average velocities at the upstream saw cut and vertical slots, with more similar values at the downstream slots. There is corresponding increase in average water depths for the upstream sections. The location of each slot is noted in Figure 1, with Slot 1 at the most downstream location within the structure.

The resultant discharge rate through the structure was one third less in the 3D model. This was a result of three aspects; firstly, the 2D model has not accounted sufficiently for the skin friction effects of the walls given that the length of slot wall exposed to the flow is around 3 times the width of the slot. A more accurate approach would be to increase the roughness values for the grid cells at the slots to account for this. The second aspect is the formation of a vortex upstream of the slot. This resulted in a non-uniform non-hydrostatic velocity distribution upstream of the slot entrance which is not accounted for in the 2D model. The third factor was that the on further examination of the 2D model it appeared the model may not have reached full convergence during the simulation. Therefore improvements in the 2D model setup would improve the accuracy of the results. Table 1 Comparison of Average Velocity and Water Depth Results Average Velocity (m/s) Average Water Depth in the Slot (m) Location 2D 3D 2D 3D Slot 1 0.64 0.66 0.25 0.22 Slot 2 0.69 0.63 0.28 0.25 Slot 3 0.78 0.51 0.28 0.26 Slot 4 0.93 0.48 0.22 0.31 Saw Cut 0.82 0.52 0.26 0.31 3.2.2. Turbulence and Energy Dissipation The original design modelled in both MIKE 21 and CFX obtained energy dissipation factors (P/V) meeting the general requirements for Australian fish species of < 40 W/m 3 (Table 1). However, the 2D model could not provide detailed spatial variation of the turbulence distribution, which is also critical for evaluating the fishway performance, as shown in Figure 6 and summarised in Table 3. From the 3D results it can be seen that energy dissipation factor in Slot 1 and 3 are 74.2 and 45.5 W/m 3 respectively, which exceeds the recommended value. Turbulence is a complex process and a three dimensional problem. The lack of ability to detail the spatial variation in turbulence is a key limitation of the 2D approach. Table 2 Comparison of Flow Rate and Global Turbulent Energy Dissipation Rate Results Location Modelling Approach Flow rate Q (L/s) Energy Dissipation Factor (W/m 3 ) 2D MIKE21 model 33.2 41.4 3D ANSYS CFX model 22.1 37.8 Table 3 Variation in Energy Dissipation Factor Results from the 3D Model Energy Dissipation Factor (W/m 3 ) Minimum Average Maximum Slot 1 0.8 74.2 323.7 Slot 2 4.3 34.7 195.8 Slot 3 0.8 45.5 203.1 Slot 4 4.2 36.6 176.0 Saw Cut 0.0 28.0 412.7 3.2.3. Design Modifications Although Design A satisfies the energy dissipation factor criteria, the majority of the flow area in the most upstream unit (Unit F) experiences very high turbulence (Figure 6). This could potentially compromise the overall performance of the fishway. To investigate this, Design A was modified by removing slot 4 and the modified design was remodeled in CFX.

The modified fishway had slightly higher energy dissipation factor, 39.36 W/m 3 and the discharge rate also increased by 3% to 22.87 L/s. However, the removal of the slot shifted the highly turbulent region towards the downstream section of Unit E and created a larger area with low turbulence which would allow the fish improved conditions for resting prior to continuing to the next unit. Table 4 Comparison of Average Velocity and Water Depth Results Average Velocity (m/s) Average Energy Dissipation Factor (W/m 3) Location Design A Modified Design Design A Modified Design Slot 1 0.66 0.68 74.2 64.8 Slot 2 0.63 0.55 34.7 61.7 Slot 3 0.51 0.50 45.5 39.2 Slot 4 0.48 36.6 Saw Cut 0.52 0.69 28.0 38.1 Figure 9 Resultant Energy Dissipation Factor for Modified Design A Although not undertaken for this study, the design layout of the vertical slots and cell arrangements could be modified further to optimize the arrangement for the all design criteria. 4. CONCLUSIONS The main purpose of this study was to compare 2D and 3D hydraulic modelling approaches for the design of vertical slot fishways through the analysis of an existing vertical-slot fishway design. The critical hydraulic design parameters included the velocity distributions and energy dissipation factor. A hydraulic model of the vertical slot fishway was developed using the 2D MIKE21 hydraulic model, and the fully 3D ANSYS CFX model. Findings of the comparison between the two models include: The fully 3D model setup was more complicated but once the structure mesh was created modifications to the design could be undertaken in a systematic and easy to implement manner. The 2D model, while simple to setup initially, is more difficult to implement design modifications. The 3D model simulation time required was of the order of 4 x that for the 2D model for this particular comparison. Wall friction and the formation of vortex structures in the velocity fields are incorporated in the 3D model and resulted in a reduction in flow rates through the fishway compared with the 2D model. As a result, the overall water depth simulated by 3D model is less than that of 2D model. The 2D model does not explicitly include a wall friction loss, and therefore some localised modification of the element roughness at the slots is necessary to take into account of the friction loss along the side walls.

The 3D model provided a spatial map of the turbulence distribution in the fishway which highlighted locations where energy dissipation due to turbulence exceeded or were close to the maximum permissible values, which was not possible to identify with the 2D model. While the energy dissipation factor was very close to the design value of 40 W/m 3, the 3D model identified regions of high turbulence within Unit F of Design A, which may impede the passage of fish through the structure. It can be concluded that fully three dimensional hydraulic models, such as ANSYS CFX, provide significant advantages for the design of vertical slot fishway structures: They can successfully determine the spatial distributions of velocity and turbulence in a vertical slot fishway design; The 3D approach is effective in identifying the constraints and opportunities for design improvements; Modifications to the designs are easy to implement and remodel; Despite longer simulation times, fully 3D models such as ANSYS CFX provide improved capabilities for fishway design. Based on the outcomes of this study our proposed approach for the design of vertical slot fishway structures is as follows: 1. Identification to biological requirements. The fishway design process must firstly assess the requirements of the fish species that require migration within the particular river to complete their life cycle. Different species will have different tolerances with regard to velocity and turbulence. Design criteria of velocity and turbulence will need to be selected. 2. Determination of the physical constraint of the watercourse. Prior to design, the study team should identify the physical constraints of the proposed location. These constraints may include public safety hazards, machinery access, location of attraction flows and fishway maintenance. Hydrologic conditions drive for the hydraulics of the fishways and seasonal or other variations in flows and water levels are important for defining the design parameters. A broad scale 2D hydraulic model can be used to assess the hydraulics at the site and set the local water level and flow parameters. 3. Preliminary conceptual design arrangements. Based on the biological requirement and physical constraints identified, the study team can develop conceptual designs. 4. Hydraulic modelling. The preliminary designs should be tested using fully 3D hydraulic models to enable accurate representation of wall friction and turbulence structures. In consultation with fish biologists, opportunities for design improvement can be identified. The performance of each design is then evaluated against the performance criteria. 5. Design selection. The most appropriate design is selected based on its hydraulic properties to best match the performance requirements of target fish species. Consideration should be given to performance over the full range of stream flow conditions. 5. ACKNOWLEDGMENTS This work was conducted with the support of LEAP Australia, who provided the ANSYS CFX software and training. 6. REFERENCES Alvarez-Vázquez, L.J., A. Martínez, et al. (2007). Vertical slot fishways: Mathematical modeling and optimal management. Journal of Computational and Applied Mathematics 218(2): 395-403. Alvarez-Vázquez, L.J., A. Martínez, et al. (2008). An optimal shape problem related to the realistic design of river fishways. Ecological Engineering 32(4): 293-300. Rajaratnam, N., G. Van der Vinne, et al. (1986). Hydraulics of Vertical Slot Fishways. Journal of Hydraulic Engineering 112(10): 909-927.

Rodriguez, T.T. Agudo, J.P Mosquera, L.P, Gonzalez, E.P. (2006). Evaluating vertical-slot fishway designs in terms of fish swimming capabilities, Ecological Engineering, 27, 37-48 Stuart, I G., B.P. Zampatti, et al. (2008). Can a low-gradient vertical-slot fishway provide passage for a lowland river fish community? Marine and Freshwater Research 59(4): 332-346. Karisch, S.E. and M. Power (1994). A Simulation Study of Fishway Design: an Example of Simulation in Environmental Problem Solving. Journal of Environmental Management 41(1): 67-77. Yagci, O. (2010). Hydraulic aspects of pool-weir fishways as ecologically friendly water structure, Ecological Engineering, 36, 36-46 Zhu, Y., Rennie, J.R.., Beardshaw, CM., Donohue, F.(2011). Using Hydrodynamic Modelling Tools to Optimise the Design of Fishways in Victoria. In: 34th World Congress of the International Association for Hydro- Environment Research and Engineering: 33rd Hydrology and Water Resources Symposium and 10th Conference on Hydraulics in Water Engineering. 26 June-1 July 2011, Brisbane, Australia, pp. 3010-3017.