Aerovortex Mill 2: A pressure differential device that consists of a converging nozzle and it's fitted with vortex generators (VIASAD: Vortex Induced Air Speed Amplification Device) or without vortex generators (JETIASAD: JET stream Induced Air Speed Amplification Device), generates suction. Ultimately, the generated suction can be used in the following two ways: (1) Improve the aerodynamic performance of wind turbine blades by applying Active/Laminar Flow Control (AFC/LFC) on their surface and/or (2) The air flow generated by the suction can be used to drive a wind turbine's rotor blades. This technology will help harness the energy from low-wind areas with high efficiency.
CROSS-REFERENCE TO RELATED APPLICATIONS
Not Applicable
STATEMENT REGARDING FEDERALLY SPONSORED RESEARCH OR DEVELOPMENT
Not Applicable
REFERENCE TO SEQUENCE LISTING, A TABLE, OR A COMPUTER PROGRAM LISTING COMPACT DISC APPENDIX
Not Applicable
BACKGROUND OF INVENTION
The invention relates to the use of wind turbines for power generation. Wind constitutes one of the major sources of renewable or “green” energy production. Wind turbines are widely used all over the world in order to harness this power from the wind.
Currently there are two types of wind turbines: vertical axis and horizontal axis machines. They both use some kind of propeller which is primarily used for extracting or converting the Kinetic Energy of the wind into mainly two types of energies: (1) Electrical energy (Power generators) and (2) Potential energy of the water (Water pumps). These propellers or rotors are either drag-based or lift-base devices. The drag-based rotors have slower rotational speeds than the lift-based devices. Generally the lift-based devices are a lot more efficient than the drag-based devices, and consequently the wind power generators are mostly lift-based devices.
A lot of research and development has been done by a number of companies around the world in order to improve the efficiency and performance of lift-based wind turbines. This lead to a number of considerable advances in this field, primarily focused on the following three areas:
- 1. Improve the aerodynamic performance of the rotor blades using passive mechanisms. Basically the goal is to maximize the Lift-to-Drag ratio (L/D) of the rotor blades.
- 2. Wind turbine yaw control and rotor blade pitch control.
- 3. Improvement of the gear system which amplifies rotation from the main rotor with the blades to the generator. Lately a gearless design has been introduced. This advancement considerably drives down the maintenance costs, since the gear system is one of the most sensitive parts, and wares out the most.
How many advances have been achieved in Wind Turbine technology, even the most advanced and efficient Wind Turbines can only operate in areas with mean annual wind speeds exceeding 6.0 m/s. Only then, they can generate enough useful energy or electricity to justify their extremely high cost. As a result, areas with low mean annual wind speeds (below 6.0 m/s), are left with no reliable and efficient enough technology to harness the energy of the wind.
Current wind capacity in the U.S. is almost entirely produced by wind farms in high wind, Class 6 areas. Class 4 wind resource areas, which are significantly closer to the major load centers than Class 6 sites, are not being utilized for wind power generation. If Class 4 wind resource areas were developed to their full potential, transmission costs for wind energy would be greatly reduced, and total land area available for wind development would increase 20 times. The concept device incorporates those technological advances which promise to render the Class 4 sites economically viable for wind development.
BRIEF SUMMARY OF THE INVENTION
The proposed device will harness the energy from the wind to generate suction, that ultimately will be used to improve the aerodynamic performance of wind turbine rotor blades. The use of this device will render the conventional wind turbine a far more efficient device at low wind speeds. The generated suction can also be used to expose a turbine in an air flow with higher speed than the wind speed. This way the energy output of the air turbine will have a higher output coefficient.
The proposed device compresses and thus accelerates the incoming air flow from the wind and as result it lowers its static pressure. It can also make use of vortex generators in order to amplify the generated suction effect. It is given the name VIASAD which stands for “Vortex Induced Air Speed Amplification Device”. The device which is not fitted with vortex generators, creates high-speed jet-streams and it is given the name JETIASAD which stands for “JET stream Induced Air Speed Amplification Device”. The Wind Turbine carrying the VIASAD/JETIASAD device, is called: “Aerovortex Mill 2”.
The suction that is generated by the proposed pressure differential mechanism, enhances the aerodynamic performance of the wind turbine rotor blades, by applying Active/Laminar Flow Control (AFC/LFC) on their surface. The aerodynamic improvements can be summarized as follows:
Increase of Lift to Drag (L/D) ratio of the wind turbine rotor blades.
Noise reduction.
Current blade aerodynamic advances including advanced airfoil design and passive mechanisms for drag reduction, have reached their maximum potential. The aerodynamic benefits of the VIASAD/JETIASAD concept device constitute the next step in the direction of rotor blade aerodynamics technological advancement. This will help to efficiently harness the energy of the wind in all sites and especially the low-wind areas.
BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS
FIGS. 1, 2, 3: The source of inspiration for the recommended mechanisms (VIASAD/JETIASAD), consists of specific lessons from nature which can be summarized as follows: The Hydrodynamic mechanisms of Aquatic Locomotion used by fishes to propel their way through fluids and the Flight propulsion mechanisms used by birds and insects moving through Air. This idea is illustrated further in FIGS. 1, 2 and 3.
FIGS. 1 and 2 illustrate the Aquatic Locomotion which can be summarized as follows:
- The Momentum-Impulse Couple of Vortex REAR DRIVEN Bodies:
- The rear body parts (feet, caudal fin) can both (A) accelerate the vortex flow generated by the body moving through the water and/or (B) generate vortices:
- A. The vortex flow generated by the body of the fish is allowed to expand laterally and eventually it is beaten by the caudal fin. This effectively restricts its path and hence the vortex flow is being accelerated.
- B. The rear body parts preform the aquatic surroundings by applying some work on the water, which in turn stores this energy. The preformed water masses flow into the zone of the underpressure creating a rolling vortex (Ungerechts et al). Due to the high geometrical organization, vortices ‘carry a high amount of momentum in relation to the energy spent for their production’ (Lighthill, 1969). The generated trailing vortex induces a velocity field which is influencing the flow in front of the moving body.
FIG. 1. Human Swimmer.
- Related Figures: 2, 3.
- Part terminology: Jet stream (1), Vortex (2).
- Description: The feet strokes up and down in the water generate ‘barrel’ like trailing vortices (2). These vortices are the cause for a backward-moving jet stream (1) in between them, and as a result the swimmer acquires forward momentum. It looks as if the human body is translating through the water between rollers.
FIG. 2. Shark Locomotion—Tail Stroke movements.
- Related Figures: 1, 3.
- Part terminology: Shark (1), Vortex (2), Generated Jet Stream (3), Shark Tail (4).
- Description: The periodical (left/right) movement of the shark's caudal fin shreds vortices on each side which are rotating in an opposite sense (Blickman, 1992). Due to the lasting rotation of the generated vortices, a jet stream is produced. This jet stream flows in between the trailing vortices and with a direction opposite to the direction of travel of the shark (backwards). The thrusting impulse responsible for pushing the shark forwards is a reaction to this jet stream (similar to the jet stream behind modern aircraft).
FIG. 3. Insect Flight—Flapping Wings.
- Related Figures: 1, 2.
- Part terminology: Insect (1), Wing Section (2), Generated Vortex (3), Jet Stream (4).
- Description: The very slow velocities by which insects fly in the air and hence the low Reynolds numbers associated with these velocities, do not justify the lift generated on their wings in order to keep them airborne. For this reason, insects use flapping along with rotational movement of their wings, in order to increase the airflow in the vicinity of each of their flapping wings and in this way generate the required lift so that they are able to fly. The way this is achieved is by generating wing leading-edge vortices (LEV) (3) which in turn produce a jet stream (5) on top of the wing.
FIG. 4A. Dual Air Flow Variant—Front View.
- Related Figures: 4B, 4C.
- Part Terminology: Throat Tube (1), Suction Flow Tubes (2), Inlet to Blower Fan (3), JETIASAD/VIASAD Inlet (4), Conical Blower Fan (5), Conical Hub (6) (For diverting air flow to the fan blades).
- Description: In this variant, the VIASAD/JETIASAD device consists of multiple converging nozzles with circular inlets facing the wind. The incoming air is accelerated and then vortices are being generated. The accelerated vortical flow induces suction which drives a secondary flow through the fan, the fan outlet and finally through a suction flow tube which leads to the vortical and/or accelerated incoming wind flow.
FIG. 4B. Dual Air Flow Variant—Top View.
- Related Figures: 4A, 4C.
- Part Terminology: Outlet (1), Diffuser (2), Throat Pipe (3), Suction Flow Tube (4), Contraction (5), Inlet (6), Wind (7), Convergent Nozzle (8), Inlet to Fan (9), Fan Casing (10), Conical Blower Fan (11), Flow Deflector Wall (12).
- Description: This is the top view of the variant described in FIG. 4A.
FIG. 4C. Dual Air Flow Variant—Side View.
- Related Figures: 4A, 4B.
- Part Terminology: Wind (1), Conical Blower Fan (2), Contraction (3), Air Flow Deflector (4), Shaft (5), Diffuser (6), Outlet (7), Suction Tube (8), Sucked Air (9), Fan Outflow Guide Wall (10), Inlet (11).
- Description: This is the side view of the variant described in FIG. 4A.
FIG. 5A. Dual Air Flow Variant.
- Related Figures: 5B, 5C, 5D, 5E.
- Part Terminology: JETIASAD/VIASAD Inlet (1), Contraction (2), Vortex Generator (3), Suction Flow Tube (4), Fan Casing (5), Conical Blower Fan (6), Inlet to Blower Fan (7), Conical Hub Air Flow Deflector (8).
- Description: A JETIASAD/VIASAD device consisting of two 2D contraction nozzles. The two converging nozzles guide the accelerated wind inflow past vortex generators in order to created vortices. The vortices are further being accelerated as they go through the contraction inducing suction which drives a secondary flow through the fan, the fan outlet and finally through a suction flow tube.
FIG. 5B. Dual Air Flow Variant.
- Related Figures: 5A, 5C, 5D, 5E.
- Part Terminology: Suction Flow Tube (1), JETIASAD/VIASAD Inlet (2), Wind (3), Intake Nozzle (4), Conical Blower Fan (5), Inlet to Fan (6), Fan Casing (7), Contraction or Converging Nozzle (8), Outflow (9), Shaft (10), Air Flow Deflector (1), Contraction Outlet (12), Diffuser (13).
- Description: This is the top view of the variant described in FIG. 5A. The impeller shown is a conical blower fan.
FIG. 5C. Dual Air Flow Variant.
- Related Figures: 5B, 5C, 5D, 5E.
- Part Terminology: Suction Flow Tube (1), JETIASAD/VIASAD Inlet (2), Wind (3), Intake Nozzle (4), Multistage Axial Fan (5), Inlet to Fan (6), Fan Casing (7), Contraction or Converging Nozzle (8), Outflow (9), Shaft (10), Air Flow Deflector (11), Contraction Outlet (12), Diffuser (13).
- Description: This is the top view of the variant described in FIG. 5A with axial fans arranged in series.
FIG. 5D. Dual Air Flow Variant.
- Related Figures: 5A, 5B, 5C, 5E.
- Part Terminology: Contraction (1), Suction Flow Tube (2), Diffuser (3), Conical Blower Fan (4).
- Description: This is the side view of the variant described in FIG. 5A with one type of the contraction inlet nozzle.
FIG. 5E. Dual Air Flow Variant.
- Related Figures: 5A, 5B, 5C, 5D.
- Part Terminology: Contraction (1), Suction Flow Tube (2), Diffuser (3), Conical Blower Fan (4).
- Description: This is the side view of the variant described in FIG. 5A with another type of the contraction inlet nozzle.
FIG. 6. Dual Air Flow Variant.
- Related Figures: 7, 8, 9.
- Part Terminology: Air Suction Tube (1), Diffusion Nozzle (2), Fan/Fan Housing (3), Branch Suction Tube (4), VIASAD/JETIASAD (5), Air Inflow (6).
- Description: This is a 3D view of a variant with two VIASAD/JETIASAD devices. Suction induced in the VIASAD/JETIASAD devices drive the air flow through the fans which are connected to the air suction tubes.
FIG. 7. Dual Air Flow Variant.
- Related Figures: 6, 8, 9.
- Part Terminology: Air Suction Tube (1), Fan Inlet (2), Diffusion Nozzle (3), VIASAD/JETIASAD device (4), Fan/Fan Housing (5), Air Inflow (6).
- Description: This is a 3D view of a variant with two VIASAD/JETIASAD devices. Suction induced in the VIASAD/JETIASAD devices drive the air flow through the fans which are connected to the air suction tubes.
FIG. 8. Dual Air Flow Variant.
- Related Figures: 6, 7, 9.
- Part Terminology: Air Suction Tube (1), Fan/Fan Housing (2), Fan Outlet (3), Diffusion Nozzle (4), VIASAD/JETIASAD (5), Fan Inlet (6), Air Inflow (7).
- Description: This is a 3D view of a variant with two VIASAD/JETIASAD devices. Suction induced in the VIASAD/JETIASAD devices drive the air flow through the fans which are connected to the air suction tubes.
FIG. 9. VIASAD Device.
- Related Figures: 6, 7, 8.
- Part Terminology: Air Inflow (1), Contraction Nozzle (2), Vortex Generator (3), Vortex Lateral Expansion Chamber (4), Hinge (5), Air Suction Tube (6), Diffusion Nozzle (7), Low Pressure Region (8), Vortex Lateral Contraction Mechanism (9), Vortex (10).
- Description: This is the side section view of a VIASAD device. The air inflow is initially compressed and thus its energy per unit volume increases. Vortex generators are then used to generate vortices. These vortices are allowed to expand laterally and eventually are accelerated by restricting their path towards the outlet.
FIG. 10. VIASAD—Wind Turbine APG suppressor.
- Related Figures: 11, 12, 13, 14A/B.
- Part Terminology: Rotor hub (1), Rotor Blade (2), VIASAD Contraction (3), VIASAD Suction Flow (4), Low Pressure Chamber (5), VIASAD Diffuser (6), Vortex (7), Vortex Generator (8), Wind (9).
- Description: A VIASAD device is used to generate suction which is ultimately used to suppress adverse pressure gradients on the rotor blades. This is done by absorbing slow-moving air on the surface of the rotor blades close to the trailing edge. As a result the flow stays attached and smooth at higher angles of attack, increasing the blade's lift coefficient and hence enhancing its performance.
FIG. 11. VIASAD/JETIASAD—Wind Turbine APG suppressor with suction Holes.
- Related Figures: 10, 12, 13, 14A/B.
- Part Terminology: Blade Leading Edge (1), Rotor Hub (2), Suction Holes—APG suppressor (3), Blade Trailing Edge (4), Wind Turbine Blade (5).
- Description: Slow moving air is sucked through the holes of the APG suppressor. As a result the flow stays attached and smooth at higher angles of attack, increasing the blade's lift coefficient and hence enhancing its performance.
FIG. 12. VIASAD/JETIASAD—Wind Turbine APG suppressor with trailing edge suction inlet.
- Related Figures: 10, 11, 13, 14A/B.
- Part Terminology: Blade Leading Edge (1), Rotor Hub (2), Suction Inlet—APG suppressor (3), Blade Trailing Edge (4), Wind Turbine Blade (5).
- Description: Slow moving air is sucked through the trailing edge inlet of the APG suppressor. As a result the flow stays attached and smooth at higher angles of attack, increasing the blade's lift coefficient and hence enhancing its performance.
FIG. 13. VIASAD/JETIASAD—Wind Turbine APG suppressor with trailing edge suction vanes.
- Related Figures: 10, 11, 12, 14A/B.
- Part Terminology: Blade Leading Edge (1), Rotor Hub (2), Suction Vanes—APG suppressor (3), Blade Trailing Edge (4), Wind Turbine Blade (5).
- Description: Slow moving air is sucked through the trailing edge vanes of the APG suppressor. As a result the flow stays attached and smooth at higher angles of attack, increasing the blade's lift coefficient and hence enhancing its performance.
FIG. 14A. VIASAD/JETIASAD—Wind Turbine APG suppressor with suction inlet—Blade airfoil section with suction flow.
- Related Figures: 10, 11, 12, 13, 14B.
- Part Terminology: Air Flow over the Blade (1), Suction Inlet opening (2), Suction Inlet APG suppressor (3), Blade Trailing Edge (4), Hinge (5), Suction Flow (6), Blade Airfoil Section (7), Suction Tube (8), Blade Leading Edge (9).
- Description: Slow moving air is sucked through the trailing edge inlet of the APG suppressor. As a result the flow stays attached and smooth at higher angles of attack, increasing the blade's lift coefficient and hence enhancing its performance.
FIG. 14B. VIASAD/JETIASAD—Wind Turbine APG suppressor with suction holes—Blade airfoil section with suction flow.
- Related Figures: 10, 11, 12, 13, 14A.
- Part Terminology: Air Flow over the Blade (1), Suction Flow through the APG holes (2), Blade Trailing Edge (3), Suction Flow (4), Suction Tube (5), Blade Leading Edge (6).
- Description: Slow moving air is sucked through the suction holes of the APG suppressor. As a result the flow stays attached and smooth at higher angles of attack, increasing the blade's lift coefficient and hence enhancing its performance.
FIG. 15. Offshore Wind Turbine with VIASAD/JETIASAD device which works with underwater currents.
- Related Figures: All.
- Part Terminology: Underwater current (1), Water surface (2), VIASAD/JETIASAD device (3), Suction Flow—Secondary Flow (4), Wind (5), Tower base (6), Wind Turbine blade (7), Wind Turbine Tower (8), Wind Turbine nacelle (9).
- Description: The VIASAD/JETIASAD device generates suction (low pressure) by the use of underwater currents. This is used to suck the slow moving air in the boundary layer on the low-pressure surface of the rotor blades. As a result the flow remains attached even at high angles of attack and also transition to turbulent flow is delayed by enhancing the laminar flow. This improves the Lift to Drag (L/D) ratio and ultimately the aerodynamic performance of the blade is improved.
FIG. 16. Wind Turbine fitted with a VIASAD/JETIASAD device.
- Related Figures: All.
- Part Terminology: Rotor Blade (1), Wind Turbine (2), Wind Turbine Tower (3), Suction Flow—Secondary Flow (4), VIASAD/JETIASAD device (5), Wind (6).
- Description: The VIASAD/JETIASAD device is attached to a single wind turbine. The suction or secondary flow that generates drives the Active/Laminar Flow Control on the rotor blades.
FIG. 17. Wind Turbine fitted with a VIASAD/JETIASAD device.
- Related Figures: All.
- Part Terminology: Wind Turbine (1), VIASAD/JETIASAD device (2), Wind (3).
- Description: The VIASAD/JETIASAD device is attached to a single wind turbine. The suction or secondary flow that generates drives the Active/Laminar Flow Control on the rotor blades. The size of the VIASAD/JETIASAD device is a little bit exaggerated here.
FIG. 18. A VIASAD/JETIASAD device driving Active Flow Control on multiple wind turbines.
- Related Figures: All.
- Part Terminology: Wind Turbine (1), VIASAD/JETIASAD device (2).
- Description: The VIASAD/JETIASAD device is supporting multiple wind turbines or a whole wind farm. The suction or secondary flow that is generated by the VIASAD/JETIASAD device, drives the Active/Laminar Flow Control on the rotor blades of the wind turbines.
DETAILED DESCRIPTION OF THE INVENTION THE INSPIRATION
The source of inspiration for the recommended concept device (VIASAD/JETIASAD), consists of specific lessons from nature which can be summarized as follows: The Hydrodynamic mechanisms of Aquatic Locomotion used by fish to propel their way through water and the Flight propulsion mechanisms used by birds and insects moving through Air.
1. Aquatic Locomotion
The Momentum-Impulse Couple of Vortex REAR DRIVEN Bodies:
- The rear body parts (feet, caudal fin) can both (A) accelerate the vortex flow generated by the body moving through the water and/or (B) generate vortices.
- A. The vortex flow generated by the body of the fish is allowed to expand laterally and eventually it is beaten by the caudal fin. This effectively restricts its path and hence the vortex flow is being accelerated.
- B. The rear body parts preform the aquatic surroundings by applying some work on the water, which in turn stores this energy. The preformed water masses flow into the zone of the underpressure creating a rolling vortex (Ungerechts et al). Due to the high geometrical organization, vortex ‘carry a high amount of momentum in relation to the energy spent for their production’ (Lighthill, 1969). This generated trailing vortex induces a velocity field which is influencing the flow in front of the moving body.
1.1 Human Swimmer
- The feet strokes up and down in the water generate ‘barrel’ like trailing vortices. It looks as if the human body is translating through the water between rollers. See FIG. 1.
1.2 Shark
- The periodical (left/right) movement of the shark's caudal fin shreds vortices on each side which are rotating in an opposite sense (Blickman, 1992). Due to the lasting rotation of the generated vortices, a jet stream is produced. This jet stream flows in between the trailing vortices and with a direction opposite to the direction of travel of the shark (backwards). The thrusting impulse responsible for pushing the shark forwards is a reaction to this jet stream (similar to the jet stream behind modern aircraft). See FIG. 2.
2. Flight Propulsion
2.1 Insect Flapping Flight
- The very slow velocities by which insects fly in the air and hence the low Reynolds numbers associated with these velocities, do not justify the lift generated on their wings in order to keep them airborne. For this reason, insects use flapping along with rotational movement of their wings, in order to increase the airflow in the vicinity of each of their flapping wings and in this way generate the required lift so that they are able to fly. The way this is achieved is by generating wing leading-edge vortices (LEV) which in turn produce a jet stream on top of the wing. See FIG. 3.
The Wind as an Energy Resource
Large areas of the world appear to have mean annual windspeeds below 3.0 m/s, and are unsuitable for wind power systems, and almost equally large areas have wind speeds in the intermediate range of 3.0-7.0 m/s where wind power may or may not be an option. These areas, are mainly unexploited for harnessing the wind energy, because technology does not exist to serve this purpose yet.
Those areas with mean annual wind speeds exceeding 7.0 m/s are the most economically viable for power generation. In these areas, existing technology of wind turbines or lift-based devices are being used, because they are usually more efficient than drag-based devices.
In summary, the most efficient current technology based on lift-generating rotor wind turbines, can operate in areas with mean annual wind speeds exceeding 7.0 m/s and generate enough useful energy or electricity to justify their extremely high cost. On the other hand, areas with low mean annual wind speeds (below 7.0 m/s), are left with no reliable and efficient enough technology to harness the energy of the wind. The invention seeks to provide those areas with low winds, a pioneering way to harness efficiently the energy of the wind.
The Invention
The invention makes use of the following mechanisms/devices in order to achieve its high efficiency at low winds:
1. VIASAD: Vortex Induced Air Speed Amplification Device.
2. JETIASAD: Jet stream Induced Air Speed Amplification Device.
The above mechanisms are basically pressure differential devices. They consist of contractions or converging nozzles which accelerate incoming air from the wind or incoming water from underwater currents and generate high-speed jets and/or high-speed vortices (Primary Flow).
The combined effect of the generated high-speed jet stream and vortices is the decrease in static pressure and hence inducing a suction effect, which gives rise to a Secondary Air Flow.
The generated secondary air flow can be used in the following ways in order to enhance the efficiency of harnessing the wind energy, especially at low wind speeds:
- (1) Accelerated air flow (Secondary Flow) is passed through the rotating blades of axial impellers or centrifugal impellers placed within a housing. The housing efficiently directs air through an inlet into the rotating impellers and then through an outlet into a duct which eventually leads to the region where suction takes place.
- (2) Use of the Secondary Flow as an Adverse Pressure Gradient suppressor or to drive Active/Laminar Flow Control or Hybrid Laminar Flow Control (HLFC/LFC) on wings or lifting surfaces used by Air Turbines. Basically, low pressure generated by a VIASAD/JETIASAD device sucks slow-moving air from the low-pressure surface of the rotor blade and/or wing. This results in smooth (laminar) and attached air flow at higher angles of attack and hence higher lift coefficients and lower drag coefficients (Higher Lift to Drag L/D ratio).
Currently, the mechanical efficiency of commercial wind turbines is maximized at wind speeds above 7 m/s, usually around some 9 m/s. The thinking behind this, is that efficiency is not important at low wind speeds since there is not much energy to harvest at low winds. Consequently, in low wind areas the choices available are to either not harness the wind energy at all, or harness it with very low mechanical efficiency using existing wind turbine technology. Aerovortex Mill 2 will help close this gap by allowing the efficient harnessing of energy from the wind at very low wind speeds. Even more, it will improve performance at high wind speeds too.
Aerovortex Mill 2 or a wind turbine using a VIASAD/JETIASAD device, makes use of a contraction or a converging nozzle in combination with vortex generators, in order to increase the density of the input energy of the wind and as a result improve its efficiency at low winds. By carefully selecting the design characteristics of the converging nozzle (Inlet Area, Ratio of Inlet to Outlet cross-sectional Areas), the invention can render a wind turbine to start generating electricity at a very low cut-in wind speed.
On the contrary to the Aerovortex Mill 2, current commercial wind turbine technology makes use of large rotor blades in order to maximize the area being swept when they operate, and hence maximize the amount of energy harnessed. Note that the power available in the wind is given by the formula: P=0.5*(Density)*A*V3. However, the use of large blades, increases the inertial forces on the rotor, which results in:
(1) Higher cut-in wind speeds than expected and
(2) Poor overall performance (low efficiency) at low wind speeds.
The solution of using taller towers on which to install the Wind Turbines so that they can reach for higher wind speeds, is very costly and technologically challenging. The invention can eliminate the need for excessive tower heights by increasing the performance of existing wind turbines.
As mentioned above, current commercial wind turbines are optimized for a single design wind speed where they achieve maximum output performance efficiently. Consequently, most of the time, at all other wind speeds, they operate at low efficiency. Aerovortex Mill 2 will operate with comparable efficiency over a wide range of wind speeds.
Also there is another benefit of using the proposed VIASAD/JETIASAD device in combination with an air turbine enclosed in a casing or housing: The air turbine is protected from the rapid flactuations in the speed of the wind. As mentioned above, the VIASAD/JETIASAD device generates the suction or secondary flow which flows through the impeller of the air turbine that is enclosed in a housing. The isolation of the impeller from wind gusts, protects the gear box connected to the impeller through a shaft from excessive loads. As a result, the reliability and maintenability of the wind turbine, improves dramatically.