Design and Analysis of a Dual Rotor Turbine with a Shroud Using Flow Simulations

This paper describes the flow simulation of a dual rotor, three-bladed wind turbine module with a shroud to determine its performance. The parameters that were evaluated are the effects of adding a second rotor, wind speed, distance between the two rotors, the size of the front rotor and the shroud. The results were obtained by using the Solid Works 2015 flow simulation program. Also, the benefits and cost issues for wind generating systems are illustrated.


Introduction
Wind energy is a form of solar energy which delivers uneven heat to various parts of the Earth's surface and causes an imbalance in the pressure distribution in the atmosphere.Due to the horizontal pressure gradient, wind is generated from the horizontal movement of the air.In certain applications, wind energy can be utilized and developed as an important energy source.
The first windmill, which was the vertical axis system developed in Persia about 500-900 A.D, was used for tasks of grain grinding and water-pumping.
Vertical-axis windmills were also used in China, which is often claimed as their birthplace [1].In the 1950s, with the discovery of oil in the Middle East that was used to generate modern mechanical and electrical power, the development of wind turbine development began to slow down.Twenty years ago, due to the "oil crisis", there was an energy shortage problem.The instability and limited nature of conventional fossil energy supply led to the development of clean, renewable energy and the emergence of wind power.Energy technology has significantly improved for over the past decades.Iron-ically, there are still over 1.1 billion people who live without access to electricity.
Figure 1 shows that most people who have limited electricity are living in Africa, Asian, and South America.Also, around 2.8 billion people have to use wood, candles, or other biomass to fulfill the basic needs of nutrition, cooking, heating, and lighting [2].Obviously, using biomass will produce a large increase in air pollution, which causes about 4.3 million deaths each year.Even though the environmental awareness has been growing for about a century, environmental pollution is still a problem, such as the global warming, haze, and acid rain.
However, there is one clean, renewable form of energy that uses virtually no water and pumps billions of dollars into our economy every year-that is wind energy.Since 2008, the U.S. wind industry has generated more than $100 billion in private investment [3]; as a result, it is necessary to continue to develop advanced wind turbine technology to supply this growing market.
Wind turbines convert the kinetic energy of the wind into mechanical power, which can then be converted into electricity by a generator.With the advancement of technology, several types of wind turbines have been created.Both horizontal and vertical axis turbines can be used for power generation.The three primary types are horizontal-axis wind turbines (HAWT), Savonius vertical-axis wind turbines (Savonius VAWT) and Darrieus VAWT turbines, as shown in Figure 2.

Evaluation Process
In this paper, four variables-wind speed, distance between two rotors, scale of the first rotor and a shroud, are evaluated for a three-bladed, dual rotor wind turbine.By using a flow simulation program, the effect of these variables on the flow velocity, pressure, and output power of the wind turbine were evaluated.
Four different wind speeds-10, 20, 30, 40 m/s, were used in the simulation module.The spacing between the rotors was 1.5 m, 3 m and 4 m.Also, the smaller rotors added to the model, as shown in Figure 3, were 60% and 80%   smaller than the larger rotor, respectively.To evaluate the models in the simulation, three variables were kept constant and one variable was changed.For example, for the smaller front rotor flow velocities, which are the wind flow velocities on the front of the second, larger blade, were evaluated with wind speeds of 10, 20, 30, 40 m/s.The front rotor was 60% smaller than the rear one and no shroud on the dual-rotor wind turbine was installed.Then the effects of the distances of 1.5, 3, 4 m between two rotors were evaluated.The flow simulation, using Solid Works 2015, was used to evaluate the different models.
The analysis for an object which has fluid passing through or around it can be very complicated.Evaluations may include the heat transfer, mixing, unsteady and compressible flows around the object.Instead of manufacturing products to test, by using the CAD-embedded Solid Works Flow Simulation program to evaluate the effects of fluid on the performance of the object during the design phase, problems can be addressed early, reducing the cost and avoiding rework.
All the parts-blade, tower, nacelle, smaller rotor and shroud-can be built in Solid Works 2015 and combined as the SLDASM which was used in this evaluation (Figure 3).
The model of the dual rotor wind turbine was designed based on a Vestas V90-3MW wind turbine (Table 1).A smaller rotor was installed in front of the conventional wind turbine to simulate a dual rotor wind turbine.
The local wind speed can be accelerated by capturing and concentrating the wind through some mechanism, such as a shroud.Installing a shroud was the method used in this evaluation.When a shroud was chosen, the most important factor considered was that the shroud have a long diffuser and brim to create vortexes to reduce the pressure downstream of the rotor to cause more flow into the rotor [4].When the entering flow increased, the velocity of the wind speed across the wind turbine increased, resulting in an increase of output power (Figure 4).However, increasing the lengths of the diffuser and brim could adversely affect the durability of the shrouded wind turbine because of the increases of weight and stresses [5].To determine the diameter of the shroud (Dr), the following formula was used:   The next step, after finishing building all the parts of dual rotor wind turbine in Solid Works 2015, was to operate the flow simulation with the following steps: define computational domain, choose the goals, run the active project, insert flow trajectories, and show the results.In order to convert the flow velocities and pressures into numbers, the trajectories of the flows were obtained.The gradients of the velocities and pressures were shown in different colors, so that different levels of velocities and pressures were distinguished.For instance, when using the smaller rotor with 60% reduction with an applied wind speed of 10 m/s, there are two types of images-detailed and overview-as shown in Figure 5 and Figure 6.In Figure 5, the gradients of the velocities are shown in different colors in contrast with the numbers on the left side.Further, the trend of the velocity around the dual rotor wind turbine with a shroud on it can be described as shown in Figure 6.Also, by reading the data shown in the flow simulations, the magnitudes of the velocity and pressure in front and back of the smaller rotor, and front and back of the bigger rotor were obtained.

The Front Velocity of the Large Rotor
One of the most important data obtained was the front flow velocity of the larger rotor (Vf2) which was an important factor in determining the output wind power.2).

Front Velocity Affected by
According to Table 1, Figure 7 and Figure 8, the front flow velocity increased when the wind speed increased.However, the impact of the distance between rotors was not significant.Also, the scale of the rotors had a positive effect.
When the scale of the front rotor was decreased, more air flow was allowed to enter the larger rotor which resulted in more output power.

Front Velocity Affected by Wind Speed, Diameter and Separation
Distance (without Shroud) The shroud was the most important factor that affected the velocity and pressure of the air flow across the wind turbine.In this evaluation, (Vx) speeds of 10, 20, 30, and 40 m/s were used as before, and the spacing between the rotors was changed from 1.5 m up to 4 m.The flow simulations were repeated for each spacing and the results were recorded.In order to show the results more clearly, the results from the flow simulation were converted to numbers, as shown below (Table 3, Figure 9 and Figure 10).
Even though the diameter of the smaller rotor was changed from 60% to 80%, the distance between rotors had a small impact on the flow velocity.However, when the wind speed increased, the flow velocity acting on the rear rotor increased when the smaller rotor was reduced in size.

Front Velocity Affected by Shroud
Since the distance between the two rotors did not have a big effect on the front velocity of the larger rotor, the shroud became an important factor to be evaluated.Using the data in Table 2 and Table 3,          rotor separation distance from 1.5 m to 4 m for both reductions, and for a reduced front rotor of 60% and 80% of the bigger rotor.
According to both Figure 11 and Figure 12, a significant influence resulted using the shroud.The front velocity was increased from around 30 m/s to 120 m/s when the wind speeds were applied from 10 m/s to 40 m/s for the module with a shroud on it.The velocity gradient was around 90 m/s, which is much larger than that for the module without a shroud.Therefore, adding a shroud on the wind turbine generates much more flow energy then changing the distance between rotors [6].theoretical maximum power efficiency of any design of a wind turbine is 0.59 (i.e.no more than 59% of the energy carried by the wind can be extracted by a wind turbine) [7].Using the Betz Limit, there is a maximum Power Coefficient, C p , which is the ratio of power extracted by the turbine to the total contained in the wind resource:  Then, in this case, the power obtained from the wind speed which acts on the front of the rotor is obtained: As shown in the Table 6 and Figure 13 up to Figure 18, the distance between rotors does not change the output power.The power only increases around 200 kW when the distance is changed from 1.5 m to 4 m.On the other hand, the shroud has a significant effect on the output power.For instance, using a rotor separation distance of 1.5 m and wind speed of 40 m/s, the power difference was around 43,000 kW when using a shroud, which was a significant increase (Figure 13 to Figure 18).Therefore, even though the shroud might add to the overall cost of the wind turbine system, it will provide a significant increase in output power.

EES Programing
Using the velocity and pressure of the back rotor for all the different cases, the power was calculated using the Engineering Equation Solver (EES) program.
Because the flow velocity V is not constant, it was convenient to write an EES Figure 13.Power affected by shroud (Small Rotor 60%).
Figure 11 & Figure 12 were developed with the applied wind speed, ranging from 10 m/s up to 40 m/s, and the

Figure 8 .
Figure 8. Bigger rotor front velocity affected by different scales of small rotor (80%), with Shroud.

Figure 9 .
Figure 9. Larger rotor front velocity affected by different scale of small rotor (60%).

Figure 10 .
Figure 10.Larger rotor front velocity affected by different scale of small rotor (80%).
Then the wind turbine power output is:

P
is the maximum value of p C and equals 16/27.However, there is an alternative way to estimate the annual energy output when a wind turbine system is analyzed.This method is based on the Weibull or Rayleigh distribution method using an average wind speed of V (m/s) at the wind turbine hub's height and a capacity factor (CF).The capacity factor can be determined as: Annual energy (kWh/yr) = (KW) 8760 (h/yr) CF R Actual energy delicered 8760 (h/yr) Average power CF

Table 2 .
Front velocity affected by wind speed, diameter and rotor separation distance (without shroud).

Table 3 .
Front velocity affected by wind speed, diameter, and rotor separation distance (With Shroud).