2.4. Computational Fluid Dynamics
The computational investigation process started with the creation of a 2D model using a blade and guide vane layout (
Figure 12). The layout consists of 2 blades and guide vanes located on a plane. The description of variable dimensions can be seen in
Table 2.
Upon completion, the model was imported to Ansys Fluent software for the purpose of computational fluid dynamics investigation. Subsequently, the model was meshed, and mesh quality was evaluated by analysis of orthogonal quality and skewness. The structure and statistics of the exemplary mesh of the initial blade geometry can be seen in
Figure 13 and
Table 3.
Initial conditions, such as an inlet velocity of 4 m/s and working fluid properties of water, were applied. The exemplary result of such an investigation in terms of velocity can be seen in
Figure 14.
With the use of additional tools available in Ansys software, namely parametric optimisation, an optimal geometry for the system was found. For this purpose, the system had to be defined with observables—values obtained from simulations that the user intends to change (e.g., lift of the blades, force momentum, etc.), as well as a list of elements requiring change (e.g., profile of the blades or pitch). The schematic showing the areas, which were specified for modification, can be seen in
Figure 15.
Parametric optimisation then attempts to create a specified number of iterations to optimise the system using a specified factor, e.g., an increase in lift of 20%. The result of such a study and the overall geometry of the optimised system can be seen in
Figure 16.
The water divider was tested separately from the blade and guide vane system layout (
Figure 17). The investigation followed a similar approach after specifying the boundary conditions of the system and elements available for optimisation, e.g., the length of the cone and the angle of inclination. The model was optimised in terms of produced drag.
Over the course of this investigation, an overall improvement in fluid exit velocity can be observed. These preliminary results proved that such a configuration of the turbine system can address the issue of water extraction capabilities. The pitch of the blades, as well as guide vanes, were evaluated and changed accordingly. The resultant change in observable parameters was convergent with the set percentages of improvement. Furthermore, the obtained blade geometry was then simplified for manufacturing purposes, by straightening the second half of the blade profile, which can be seen in
Figure 16.
Having validated the use of the impulse turbine with optimised blades and guide vanes, the study proceeded to the next step—the development of a 3D model with the aim of conducting 3D transient CFD simulations. The completed model can be seen in
Figure 18. The assembly consists of the following:
Water Divider—forces the working fluid to flow around the nose of the divider, directly towards the turbine system; prevents loss of momentum from direct impact on the hub.
Guide Vanes—a total of 28 guide vanes deflect the working fluid onto the blades at 60°.
Turbine—consists of 30 blades and promotes rotational movement.
Stationary Domain—a cylinder body encompassing the entire turbine assembly. Essential for specifying the flow domain in Ansys Fluent.
Rotational Domain—a cylinder body encompassing the turbine; allows us to specify the mesh motion around the rotating component.
The initial revision of the 0.6 m turbine assembly had a total length of 1.3 m. The flow of the fluid in the system was constrained by the stationary domain with an outer diameter of 0.6 m. The tip clearance (distance from the blade’s tip to the outer wall) was set to 1 mm. Such small tip clearance proved to be problematic when meshing the assembly. The issue mainly included unsatisfactory mesh quality, with orthogonal quality being below 0.1 and skewness above 0.9. For the model to compute properly, these conditions needed to be satisfied. The reduction in mesh size would be one of the solutions. Ultimately, the mesh would have to be reduced to such a small size that the simulations with moving mesh would increase the solution times almost by a factor of 2. Therefore, it was decided to increase the tip clearance to 5 mm.
The meshing was achieved by specifying the maximum and minimum element sizes, as well as mesh defeaturing. Additionally, local mesh control was implemented at the contact surface between the stationary and rotational domains to ensure that the flow of the working fluid is accurate. The statistics and characteristics of the mesh are specified in
Table 4. The cross-sectional view of the generated mesh and overall model can be seen in
Figure 19 and
Figure 20.
After successful meshing, the set-up of the simulation was conducted. Firstly, a viscous model for the working fluid was selected. The 2 main choices for this model were k-epsilon and k-omega. According to the Ansys Fluent guides, the k-omega model is considered to perform better near walls, whereas k-epsilon is best suited for flow away from the wall, e.g., free-surface-flow regions [
23,
24]. As the model has both of those phenomena, the initial simulations were tested with two different models. However, no change in the output values was observed. Therefore, the chosen model was a realisable k-epsilon model with enhanced wall treatment. This is the improved version of a standard k-epsilon model, which was created to close the gap between the standard versions of the 2 models [
24]. The previously mentioned moving mesh (also called dynamic mesh) feature was applied to the model to account for the changes in boundary conditions over time in the simulation. This approach is especially important in the fluid–structure interactions of rotating machinery. It promotes the capture of geometry changes within the model, provides better boundary layer resolution, and conserves fluid flow characteristics within the model through accurate tracking of moving boundaries [
25].
The standard Ansys water properties were applied to the stationary and rotating domains. The rotating domain was specified as a moving mesh, in order to account for the moving walls of the turbine. The turbine itself was initially set to run at 30 rpm, which was later changed to 130 rpm upon obtaining further results of the 3D fluid behaviour under operation. The fluid velocity at the inlet was set to 4 m/s, simulating the output of the pumping chamber of the Dolphin device. As the simulation was transient, the operational time was set to 3 s, which accounts for 300 time steps (increments) of 0.01 s size. This was performed to reduce the solution time, as well as the generated sizes of stored files. The overall length of the simulations was validated by referencing the scaled residual graph for the continuity of the simulation, which achieved a stable state. Moreover, the simulation was further examined by comparing the results with 5 and 10 s simulations, which showed a good convergence, with the results for 5 and 10 s being less suitable due to the increased time step size. The set-up simulation was then checked using Ansys Fluent features and solved.
To analyse and validate the results obtained from computational simulations, a previous study dealing with experimental and computational analyses of impulse turbines was considered [
22]. This allowed for the identification of suitable measurement points, as well as the values needed to evaluate the turbine’s performance. A total of 4 measurement points were created, which are shown, and colour-coded, in
Figure 21.
Position 0—Green—measurement point before the guide vanes, located 200 mm from the midspan of the turbine.
Position 1—Purple—measurement point after the guide vanes and before the turbine, located 70 mm from the midspan of the turbine.
Midspan Point—Yellow—measurement point located directly at the midspan of the turbine.
Position 2—Red—measurement point after the turbine, located −70 mm from the midspan of the turbine.
The evaluation of the turbine’s performance involved the use of the following equations for torque, input power, and flow coefficients, as well as efficiency and power [
26]:
The overall list of variables and their descriptions can be found in
Table 5.
As the last step for the CFD analysis of the system, a comparative validation study was conducted. In this study, the developed simulation environment was tested against the previously referenced literature on numerical and experimental testing of the air impulse turbine in OWC [
22]. Two main differences can be identified between the referenced study [
22] and the investigation conducted in this paper. Firstly, the working fluid in the Dolphin device is water, whereas the OWC turbine is propelled by air. This enforced a change in the domain fluid within the simulations for validation purposes. Secondly, it is crucial to highlight that the system geometries were edited through the previously carried out optimisation techniques for the Dolphin device turbine system. The main differences between the two systems can be seen in
Figure 22 and
Figure 23.
The purpose of this investigation was to validate the overall set-up of the CFD simulations and the behaviour of the fluid throughout the system by comparing the results for the flow coefficient. This meant that the overall axial and circumferential velocities of the fluid at the turbine had to be measured.
The referenced study states that for rotational speeds of the turbine ranging from 125 rpm to 1250 rpm, the recorded flow coefficient ranged from 0.27 to 2.7. Due to the long computational times, the studies for the Dolphin device turbine were limited to the range of 750–1250 rpm, hence a total of 3 simulations with rpm increments of 250 rpm. The required velocities were measured at the midspan of the turbine. Overall, the results showed a good correlation and fit within the specified range, with the flow coefficient ranging from 0.31 to 1.21 for rotational speeds of 1250 rpm to 750 rpm, respectively. Marginal errors are acceptable in both CFD and FEA simulations. Various sources report different error margins, typically ranging from 5% to 13%, depending on the methodology used in the study [
27]. Therefore, it was determined that with extensive and complicated CFD simulations with a moving mesh and altered blade geometry, this value difference of 12.9% is acceptable.
2.5. Turbine Design for Manufacturing
The initial model of the turbine was created for the purposes of computational fluid dynamics simulations. Therefore, some features of the turbine could be questioned and deemed not optimal for manufacturing purposes. This required creation of additional concept models, fit for the application. Recognising this situation, further studies on manufacturing adaptability were performed. The turbine’s design for manufacturing was conducted after performing CFD simulations. This approach allows the possibility of taking into account the fluid behaviour and the ability to gain more comprehensive knowledge of the operational cycle of the system.
The primary objective of conceptual design is to identify and select the most promising and desirable concepts. The chosen concept is subsequently refined in the design phase. Designers who use efficient and effective concept selection methods are likely to achieve reduced cycle time and costs during the conceptual design stage. Moreover, they can lower the risk of expensive design changes later in the process [
28].
A total of 4 different concepts for the turbine were produced. The overall models are presented in
Figure 24,
Figure 25,
Figure 26 and
Figure 27. The permanently fixed blade concept is very similar to the initial design of the turbine, apart from the edited rotor structure and retainment system for the shaft, as well as the specification of permanent fixture—welding. Bolted blades v1 incorporate an off-centre rotor with a retainment system for the blades at the midspan of the rotor. The bolts retaining the blades go through the rotor into the blades; each blade is given a singular bolt. The bolted blades v2 concept presents a symmetric rotor, along with 2 bolts retaining each of the blades. The slot-in blade turbine consists of blades with a root and 2 rotor plates. The blades slide into a slot on one side of the rotor and are secured by connecting a second rotor plate with bolts. Moreover, the blades are further kept in position by bolts through the root of the blades.
For easier representation of the general principle of the slot-in turbine, an additional figure was included showing the geometry of the slot-in blade (
Figure 28).
The concepts were then appraised according to the specified criteria. Ideally, the chosen design would be simple and easy to manufacture, while maintaining a low cost of development. Moreover, it must provide a satisfactory level of reliability and safety during operation. Lastly, it should be easy to perform maintenance activities on the turbine.
The use of a decision matrix supported the accurate rating completion for the studied concepts against the initial design. An example of such a matrix can be seen in
Table 6.
In the case of the manufacturing characteristics, the authors had to appraise the availability of manufacturing capabilities within the project, as well as the suitability of the considered materials. Upon referencing similar studies on 0.6 m impulse turbines for OWC, two suitable materials were selected—aluminium and stainless steel [
28]. Aluminium offers a cheaper price per unit volume; however, stainless steel is more commonly used for marine environments, where aggressive corrosion risks are present [
29]. When considering this, stainless steel was chosen as a base material for the turbine structure. At the moment of the conducted research, various manufacturing processes were available, such as laser cutting and 5- and 3-axis CNC machining, as well as lathe, milling, and welding machines. This step became crucial, as some of the complex geometries, e.g., the slot-in blade, would prove to be challenging to manufacture. This issue could be resolved by taking into consideration a significant investment in additive manufacturing. However, this would ultimately increase the overall development and production costs. This is mainly due to the higher operating and material costs.
The permanently fixed blade concept proved to be hard to manufacture due to possible problems with blade alignment while welding. Moreover, the possibility of warped material during welding was also a deciding factor for the negative rating. Due to the permanent fixture, the blades are not easily replaceable, which means that the safety as well as maintenance factors were given a negative rating. When compared to the initial design, the concept was rated to be around the same in terms of development cost, simplicity, and reliability.
The first iteration of the turbine with bolted blades proved to be an improvement in comparison to the permanently fixed turbine set-up. The main quality favouring this solution was the implementation of the detachable blades. This would, overall, reduce the manufacturing complexity and simplify the maintenance of the turbine. There were no expected major changes regarding the development cost and reliability of the system. The second iteration of the bolted blade solution increased the number of constraining points, therefore improving the overall safety of the turbine through a more secure fixture.
Lastly, the slot-in blade turbine concept was evaluated. This iteration was far more complicated in terms of manufacturing complexity and overall design. However, it presents a sturdy fixture system in both radial and theta directions, while maintaining the favourable quality of detachable blades.
The slot-in and bolted v2 concepts ended up with the highest scores, with the bolted v2 design being more centred around the manufacturing complexity and simplicity of the design. Taking into account the current development stage of the project, manufacturing capabilities, and future plans to conduct physical testing on the turbine system, the bolted v2 solution was chosen.
2.6. Generative Design
Complex topologies are often difficult and time-consuming to obtain by conventional optimisation techniques. New analysis and manufacturing methods can be used in an integrated structural optimisation strategy producing highly efficient and adaptative topologies [
30]. Metal additive manufacturing has experienced rapid development in recent years, with new commercial metal additive manufacturing machines and methods becoming more competitive and cost-effective in comparison with conventional CNC processes [
31,
32]. The utilisation of the latest advances in design and manufacturing techniques offers innovative approaches to high-performance structural optimisation applications over different disciplines, such as aerospace, energy, and automotive industries [
33]. These new approaches represent a revolution in developing highly efficient and cost-effective strategies at an early stage of design projects and overall manufacturing process [
34,
35].
Following the development and choice of the best-fitting concept design for the 0.6 m impulse turbine, a generative design structural optimisation process was conducted based on the study [
18].
An integrated structural optimisation strategy with generative design techniques was applied to the blade and rotor structure of the Dolphin energy system using the finite element analysis package of ANSYS Workbench 2022. The mesh analysis was adapted to each of the two structures with specific mesh control applied to the boundary surfaces and maintenance of a hexahedron element mesh. The load and fixed conditions were exported from the previous analysis performed in this study and adapted for each of the two structures of the blade and the rotor. The parameters for the generative design process were set with a limit of 500 iterations and a convergence rate of 0.1%. Based on the knowledge acquired in [
18], a design for additive manufacturing constraint of an overhang angle of 35 degrees was also applied to the generative design process in order to minimise the support structure during production.
Firstly, the loading conditions on the system had to be defined and exported from the existing Ansys Fluent project, where a mapping of the pressure acting upon the blades was assessed as shown in
Figure 29. The time points for the loading conditions throughout the simulation were analysed and showed marginal differences. The final time step was chosen as the measurement and reference point.
The blade topology was divided into different sectors in order to transfer the pressure acting upon the surface of the blade to develop the generative design structural optimisation. In
Figure 30, we can observe the divisions of the surface of the blade into different facets.
Using the results obtained from the Ansys Fluent simulation, an average pressure value was calculated for each of the facets conforming to the four surfaces of the blade. In
Table 7, the different pressure values associated with each of the facets can be seen.
The calculated pressure values were used to develop the boundary conditions of the blade generative design structural optimisation process. In
Figure 31, the applied pressures are shown in red and the fixed support representing the bolted joint with the rotor structure is shown in blue.
The nature of the loads acting upon the structure of the blade constrains the outer surface of the topology as a boundary condition, limiting the volume optimisation range of the internal volume. The advantage of a design for an additive manufacturing approach allows for the consideration of hollow cavities as part of the optimisation process.
Figure 32 shows the generative design structural optimisation process of the blade representing the initial stage of the process with the considerations of the boundary conditions, a middle stage of the optimisation process where mass is generated to comply with the optimisation objectives, and the final converged solution of the generative design process.
In order to develop the generative design structural optimisation for the rotor topology, a resultant force was calculated to transfer the pressure acting upon the blades into the rotor structure through the bolted joints. We can observe the resultant force calculated in
Figure 33.
Table 8 represents the values of the different components of the resultant force, with a total value of 475.99 N. In this table, we can observe that the value of the component of the resultant force in the y-axis is negligible in comparison with the x and z components of the force.
Following the assessment of the resultant force generated by the pressure acting upon the blade structure, a load was applied on the rotor structure’s bolted joint surface, as can be seen in
Figure 34a marked in red. For an efficient application of the resultant force to each of the 30 blades’ bolted fixed constraints, the component of the force in the z-axis was maintained constant while the x component was translated and rotated for each of the blades’ bolted fixed constraints, as we can observe in
Figure 34b. In
Figure 34b, the gravitational load applied on the centre of mass, a 13.6 rad/s rotational velocity as a worst-case scenario for the turbine operation, and a fixed constraint for the rotor structure on the bolted connection at the shaft are shown.
Figure 35 shows the generative design structural optimisation process of the rotor structure including the initial stage of the process with the considerations of the boundary conditions, a middle stage of the optimisation process where mass is generated to comply with the optimisation objectives, an advanced stage of the optimisation process, and the final converged solution of the generative design process.