Modular flow accelerator for a wind power plant with a vertical rotation axis A.A. Bubenchikov I.S. Lebedev T.V. Bubenchikova A.A. Zakharov E.A. Manakova Energy Department Energy Department Energy Department Energy Department Energy Department Omsk State Technical Omsk State Technical Omsk State Technical Omsk State Technical Omsk State Technical University University University University University, Omsk, Russia Omsk, Russia Omsk, Russia Omsk, Russia Omsk, Russia privetomsk@mail.ru lisnick@bk.ru Antech-energo@mail.ru a.n.dr.e.w@mail.ru manakova_helen@mail.ru Abstract. The design version of a power generating unit of a multi-tiered wind turbine type with a vertical rotation axis is considered in this article. The results of mathematical modeling and the operation principle of the tier elements of the power generating area with a vertical rotation axis are examined both separately and in combination with each other, forming a complete arrangement. The total average coefficient acceleration values of air flow passing through a power generating unit at different ram flow velocities are determined. Keywords: convergent tube, concentrator, air flow acceleration, air flow diffusion, wind power plant with a vertical rotation axis, power generating unit. I. INTRODUCTION Currently, using wind power plants in the central part of the Russian Federation is not absolutely profitable. This is due to the fact that most of wind power plants available on the market are designed for a wind velocity of 10 m/s. Since power produced by a wind turbine depends on the velocity cubed, such installations in our region, where the wind velocity is in the range of 3-5 m/s, will produce no more than 30% of its committed capacity and the payback period will reach about 150 years. The instability conditions of the low-velocity air mass flow, which are typical for low-rise buildings and regions remote from a world of waters, require the development of wind power systems capable of stabilizing and selecting wind flow power [1-3]. This will be caused by using special geometric designs for vortex-type installations. The proposed development is a wind power system unit and it gives the possibility to combine three tiers (concentration, acceleration and dispersion) of a power generating unit (PGU) of a wind turbine (WT), obtaining the optimal power generation effect. II. PROBLEM SETTING The proposed installation consists of three modules. The first module is designed to concentrate and reorient air flow from horizontal to vertical direction. There is acceleration and additional flow ejection in the second module. The third block is used to create a zone of reduced pressure for additional suction of the operating flow and its acceleration in power take-off area. The installation shape is a sandglass. To determine the optimal geometry of the first module The work was performed with financial support of RF President Grant MK-5446.2018.8 XXX-X-XXXX-XXXX-X/XX/$XX.00 ©20XX IEEE designs, forming five converging chambers and channels, which are a cone at the base, as well as the outer case for a converging channel will be investigated. Using the second module, conditions for obtaining a compacted laminar flow changing the main movement direction will be created. It is important to emphasize that both modules should also be oriented to an additional flow turn relative to the horizontal axis. The third module will be designed taking into account the dispersion and final corner rotation of outward air flow parallel to external environment flow. The effective proper use of separate structural members of PGU which in the first approximation are represented by different areas of production is proved by their operation practice of (table. 1): for the first module they are TPP cooling plants (cooling towers), for the second one– the elements of water intake from great depths, for the third one – ventilation systems. The design of PGU is based on previously known ideas of effective use of air flow accelerator elements [46]. The distinctive feature of this article is a proposed design version, permitting to study the complete cycle of air flow within PGU in analyzing driving forces at power take-off area. III. THEORY In any power plant, special attention should be paid to a power generation (selection) unit along with subsequent optimization of mechanical and electrical components taking up electromechanical power loads. Getting obviously large efficiency values is due to using optimal solutions of the interaction between a power generating unit (PGU) and the requirements of the power plant placement and operation. In the present study an aerodynamic concentrator confuser-diffuser installation of a tower-modular type is presented as a power take-off unit. Venturi effect is the base of operating all wind power concentrators, as a result of Bernoulli law. It is that pressure drops and velocity increases when gas flow passes through a narrowed pipe part [4]. Therefore, it can be stated that power increase can be obtained by reducing cross-sectional flow area with its simultaneous increase in velocity. Hence, accelerating air flow is the main development tendency to improve the efficiency of wind power plants (WPP). TABLE I. MAIN COMPONENTS (TIERS) OF A POWER GENERATING UNIT Tier name 1. Spiral converging tube 2.1 Ejection and acceleration chamber Objects and examples of using structural elements Cooling towers, aerators Gas-liquid pumps Fuselage and wing elements in the field of low velocity aero building 3. Deflector Ventilation and air conditioning systems Taking into account the experience of designing and operating wind-dynamic systems under low wind pressure [7], it can be argued that the most optimal installations will be vertical-axial wind turbines for the considered conditions. In this case, the hypothesis proving greater efficiency in using concentric surfaces than rectangular bodies in PGU designs will be tested (Fig. 1-3) To facilitate the task of finding optimal design solutions in general, any PGU is divided into separate parts – modules which functions can have both similar and different purposes. Operating a power generating unit is based on the following processes: concentration, direction reorientation, contraction, ejection, air flow rarefaction and diffusion, increasing its velocity and density [8-9]. According the world practice, constructing modules is expedient based on the principle of similarity (analogization) to the geometries of the living world, using: – the Golden ratio between installation components; – spatial logarithmic spiral kinematics, – the configuration of low-dimensional mathematical topology, – internal spatial areas in Gaussian distribution. Using the above methods permits to obtain hypothetically efficient power systems, which efficiency, as well as the legitimacy of mathematical apparatus selection, are specified in the subsequent mathematical modeling and full-scale designing. The whole considered power system should take into account the peculiarity of its operation in the conditions of low wind flow velocities. This makes a large set of source data comparable with those of kinematic processes values be considered. However, the dynamics of low velocities today remains poorly understood and this creates additional complexity in the wind turbine development. The constant dimensional air flow redirection in modules 1 and 2 enables to maintain and increase the total forces of centripetal accelerations, which allow to maintain the laminar-vortex structure of the main flow. The laminar-vortex structure of the air flow permits to concentrate the driving forces in a certain area of mechanical energy removal. Depending on the driving forces nature, it is necessary to use the appropriate geometry of the power impeller surface fixed to the power take-off shaft. 2.2 Additional acceleration chambers XXX-X-XXXX-XXXX-X/XX/$XX.00 ©20XX IEEE An additional kinetic energy increment in the area of its removal is due to the functions of the third PGU module: ejection, air flow rarefaction and dispersion. And the mechanical rotation energy transmitted to the power take-off shaft by means of mechanical systems (gearbox) makes the electric generator rotate. Thereby power is supplied to the inverter through the regulator unit. After the system start-up, the mode of its operation is quickly stabilized, and the conditions for electrical energy removal from the inverter terminals appear. Since the structure of the electromechanical system is quite complex, it requires the constant operational adjusting and surveying. Setting up mathematical correspondence of the considered dynamic system will require final full-scale experiments. IV. EXPERIMENT RESULTS The PGU operation principle includes: concentration, direction reorientation, contraction, additional ejection, air flow rarefaction and dispersion (Fig. 1). Fig. 1. Longitudinal cross section of PGU There is an obstacle downwind in the form of statically located cone 1 and channels 2, built along the trajectory of a three-dimensional logarithmic spiral twisted around the cone 1 of the first module. The effect of concentration and reorientation of wind direction in the earth's surface plane by 72 degrees takes place. The geometry of the cross-sectional area of the channels 2 resembles an elongated drop, which space decreases proportionally as the air flow passes upwards, thereby creating the effect of contraction and its twisting. The formed air flow in each of the channels 2 enters the second module - the placement zone of the first corrugated diffuser ring 3. Corrugation is represented by five flange-shaped troughs with their displacement by 72 degrees (the plane of the earth's surface), coinciding with air flow trajectory along the diffuser circle. Then the flow moves to the zone of the second saddle-shaped diffuser ring 4 (module 3), which region is dissected by five floworiented blades 5 twisted by 144 degrees (the plane of the earth's surface), directed also along the main trajectory of air movement. The profile of both rings is comparable to the mixing ejector [6] in geometric parameters, which experimentally proves its structural efficiency. Moreover, the cross-sections of the diffuser ring walls 3 and 4 are made in the form of a low-velocity wing profile (long and thin). To increase the pressure and integrity of the formed flow in the body of the diffuser ring 4, structural elements in the form of elliptical air intake/air dispersion openings 6 are added. At the outlet of the second diffuser ring 4, the air flow will enter the dispersion zone. At the air flow outlet from the channels 2, the wind wheel 11 is installed in front of the corrugated diffuser 3. This wheel acquires additional dynamics of movement due to the ejection effect of external wind flow through the structural formation of gaps between the channel group 2 and the corrugated diffuser 3. Additionally, in the channels 2, oriented downwind, there is the cross-flow of operating air masses (reverse thrust), increasing the driving moment. Moreover, the module two is installed on the module one, taking into account the technological overlap of dimension projections. An additional improvement in the quality of flow twisting and its distribution is obtained by placing the entire system in the core diffuser 3 presented by a drop 7. The second half of the core 7 is closed by the second diffuser 4 with an outlet to flow dispersion area. The kinetic energy of the air flow is converted into rotational motion of the wind wheel 11 by sensing area air pressure on the blade. Further torque is transmitted to the gearbox by means of the shafting line on which the wind wheel 11 (power take – off impeller) is mounted, and then to the generator (not specified in figure 1). They are located at the convergent tube base – cone 1 of the first module. Module three is a chamber of reorientation, rarefaction and dispersion of the working and external flows. The total oriented flow, leaving the module two, is entrained by an additional wind flow of external environment, which enters the air intake ducts 6. Besides an additional external flow meets the installation, entering the air cavities between the diffuser ring 4 and the dome 8 with an opening in the center. The air flow inside the module 3 after the rarefaction stage is divided into two components, scattering between the diffuser ring 4 and the dome 8, and also, reorienting along the guides 9, and comes out between the dome 8 and the cap 10. The diameters and heights of concentration, acceleration and dispersion modules are also determined by the following structural elements (parameters): 1. The scale of spiral turns of a static blade (this affects on the angle of the wind flow rotation and the channel width) -in our case it equals to 72according to the laboratory tests [10]. 2. The number of twisting turns (affecting on the channel width) was determined earlier, on the conducted studies basis [10], it is possible to determine the optimal XXX-X-XXXX-XXXX-X/XX/$XX.00 ©20XX IEEE number of sections for the first tier (module) as 5 in number. 3. The geometry of a guide channel (affecting on the wind flow rotation angle) – it is simulated according to the geometry of a three-dimensional logarithmic spiral. 4. The conjugation form of an extended static blade, providing a smooth entry of the wind flow into the wind turbine convergent tube (affecting on the concentrator flow inlet area) – two options are proposed in using: straight and rounded ones. 5. The shape and rotation angles of the blades 5 and guides 9 in the second module body (affecting on the density and flow rate). 6. The height of the convergent tube – the constant parameter of 1500 mm is defined. 7. The height of the lower dome boundary of the convergent tube above the ground surface (air inlet channels) – proposed options are in the range from 450 to 1200 mm. 8. Dimensions and conjugation angles of the second and third tier elements of a power generating unit [10]. 9. Cross-section profiles of diffuser rings 3 and 4, dome 8 and cap 10 10. Configuration of air intake openings 6. To ensure optimal efficiency of the installation, it is necessary to observe the condition of the exhaust air flow outlet parallel to the external one. This factor is necessary in constructing the geometry of modules deploying flow to certain angle values, which total sum must be multiple of 180 degrees. In experimental studies for the first module (tier) in [10], the value of the optimal flow rotation angle was determined, which value varies from 51 to 120 degrees. For the third module – the dispersion unit, the values of the flow twisting angles were laid according to the experimental data obtained in operating full-scale models and completed units. In our case of borrowing the elements of the well-known deflector design [5], the flow twisting interval was from 5 to 90 degrees. Hence, considering two previous modules, the flow twisting value for the second tier should be in the range from 126 to 211 degrees. The value of 144 degrees was determined experimentally. In order to determine the final design of the PGU, it is necessary to identify the most optimal design solutions for separate module units at preliminary testing stages. It is necessary to consider the conditions of the best performance parameters for each unit separately. However, there is a high probability that in some cases operating the elements taken separately is ineffective or simply impossible [9]. The refusal from rectilinear geometries, despite the sufficient assembling and manufacturing simplicity in favor of using concentric bodies in the PGU elements, is due to the practice of comparing mathematical modeling results in order to obtain the best acceleration coefficients (Fig. 2-3). Fig. 2. General view of the first tier versions a) b) c) d) Fig. 3. Horizontal section of airflow outlet plane from a concentrator: a) external structural elements of a convergent tube are presented by symmetrical planes; b) convergent tube elements are smooth planes; c) internal structures of a convergent tube are symmetrical planes; d) internal structure of a convergent tube is presented by smooth planes Fig. 3 a, b shows that in changing symmetrical planes of an external convergent tube construction into smooth concentric ones, velocities inside the convergent tube body will get greater values. A more uniform distribution of flow velocities inside the convergent tube proved the necessity to divide the internal space into five channels (Fig. 3b, C). Organizing the internal space of channels by replacing sharp corners with static blades allowed to localize an operating channel and increase the velocity value inside it (Fig. 3b, g). For the selected geometry, the height of an external truncated cylindrical dome was chosen. The data obtained are presented in table 2. Based on the data obtained, the most optimal configuration of the first module (tier) was chosen for the further power generating unit construction. The height of the earth's surface indentation was 1000 mm. The geometry of the second module construction is similar to the proposed mixing ejector characteristics of the scientific study [6]. When conducting mathematical research on obtaining the highest acceleration values in module 2 it was discovered that in adding capacity directed flange channels of the first diffuser of a mixing ejector [6] the effect of the supplemental local flow acceleration appeared. This effect was taken as a basis and improved in constructing shaped fence chambers– separate channels in the module 1 (Fig. 4). The cone parameters remained unchanged. It was decided to replace the inner blades and the outer casing with separate channels, which allowed to give them influence of integrity and softness on the flow. The generatrix (arc, R=275mm) and its trajectory (straight on the surface of a cone with a twist of 72 degrees) were left from the inner blade in the previous version, the contour was closed by an arc (R=193mm). To observe the conditions for maintaining and increasing air flow density, it is necessary to sustain the constant forced change of movement direction when stabilizing the formation of vortex flow (especially in extended and volumetric chambers). This is due to the flow contraction by centrifugal forces. And in the transition of the air flow from one element of the module to another, it will be especially important to create this effect of changing the dimensional flow direction. The second tier outside is represented by the first corrugated diffuser ring (Fig. 5, hereinafter "corrugation"), designed to create an ejection effect. The lower edge of the ring is a set of channel profiles of the first tier, formed into a ring. The corrugation is located relative to the first tier in such a way that the first tier is immersed in it by 44 mm, and the distance between the outside channel walls and the corrugation is 1:1.63. Constructing such geometry is due to the wall layer presence in the flow [11], which kinematic viscosity is much higher than the operating one, freely moving from the channels to the corrugation inside. a DETERMINING THE ACCELERATION AIR FLOW COEFFICIENT OF THE LOWER TIER (MODULE), DEPENDING ON THE OVERALL PARAMETERS WHEN THE BASE CIRCLE DIAMETER IS 1567, 8 MM b TABLE II. Lower dome generatrix height, mm Flow velocity, m/s 450 600 1000 1200 4.9 5.5 XXX-X-XXXX-XXXX-X/XX/$XX.00 ©20XX IEEE 5.8 5.5 Fig. 4. Views of the first module channel versions: a) general view, b) side view a b Fig. 5. Views of channel versions of combining the first and second module: а) general view, б) side view assembly. We can see the non-directional and nonstructured rarefaction and dispersion of the air flow, which ultimately reduces power take-off efficiency at the appropriate area. The received data served the basis for forming the third tier structure, which began to acquire the properties of concentration, direction reorientation, ejection, rarefaction and dispersion of the air flow, typical to the deflector properties [5] and was determined in terms of the transition diameter between the modules two and three. Besides, for ordering the flow motion better, additional elements such as a central guide (position 7, Fig. 1), blades twisting around it (position 5, Fig. 1) and elliptical openings (position 6, Fig. 1) placed on the second saddle-shaped diffuser ring. In analyzing the velocities picture of the mathematical modeling results of a transition tube of the first and second modules (Fig. 6) it can be stated that the twisting corrugation nature has a great influence on the ejection parameter values. The greater the twisting angle of elliptical corrugation flanges along the flow movement, the higher the velocity entering into the structure. With more twisted ring the velocity of the incoming flow is in the range of 6-7 m/s, with less spun one it is about 5 m/s. Moreover, the high velocity area expands (Fig. 6). Fig. 8. Velocity map of mathematical positioning of the developed model in the general flow at a velocity of 5 m/s а) Fig. 6. б) Comparing twisting versions of ejector ring flanges a) spun at 72º, b) spun at 10º The third tier became a chamber for the exhaust flow removal outwards. And the installation is domed and capped (position 8.10, Fig. 1). Guide blades are designed taking into account the thickness gap of the wall layer [11]. The twisting angle of five blades (position 9, Fig. 1) is due to the exhaust flow outlet in the direction of the ram environment air and amounted to 144º. After measuring the main dimensional performance parameters of PGU, data are summarized in table 3. The data obtained indicate the performance of the system, but with small efficiency. It provides maintenance, distribution and acceleration of incoming flow, but certainly requires further development. Determining the optimal ratios of all the abovementioned structural parameters will allow to obtain the greatest flow acceleration from 34% to 50% and increase the power generated by a wind turbine from 2.2 to 3.3 times. V. Fig. 7. Flow pattern in an installation with the third tier ring (the external flow moves along the glance trajectory, from an observer to PGU) After forming the second module geometry, the question about the design of the second saddle-shaped diffuser ring arose (Fig. 7). The result was obtaining the visual air mass movement at the stage of step GPU XXX-X-XXXX-XXXX-X/XX/$XX.00 ©20XX IEEE CONCLUSION The simulated design gives the possibility of estimating the acceleration air flow coefficient. It allows to analyze separate concentration units: direction reorientation, contraction, additional ejection, rarefaction and dispersion of the air flow. At the same time, the functionality of the proposed flow acceleration system will be minimally influenced by such factors as temperature, intensity and frequency in wind direction changes. Constructing a wind flow accumulation unit through the optimal combination of modules and additional toppings, along with the process of increasing power and averaging the air flow at the outlet, will also help to TABLE III. reduce the vibration loads both on structural elements themselves and on adjacent territories. This is one of the most important factors in locating wind turbines near social facilities and residential infrastructure. MEASUREMENT RESULTS Obtained values of flow velocities at an external wind of 5 m / s Tier Name separately, m / s 1. Spiral convergent tube 2.1 Ejection and acceleration chamber 2.2 Additional acceleration chambers 3. Deflector 5.35 5.5 3.88 3 While investigating it was revealed that the data obtained by preliminary hypothetical analysis were corrected by means of mathematical modeling. These data will provide the basis for the further research of the proposed designs with due account for the influence of additional geometry elements in a power generating unit. REFERENCES [1] A. A. Bubenchikov, T. V. Bubenchikova, E. Y. Artamonova and A. O. 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