INCREASED SWEPT AREA

FIELD OF THE INVENTION

The invention relates to the class of crossflow axes rotary mechanical devices, which may provide the basis for a new class of crossflow axes rotary mechanical devices with Dynamic Increased Swept Area, suitable for different fluid types and a range of applications such as wind turbines, hydro turbines, propellers, fan-blowers, pump-compressors, mixers etc.

BACKGROUND OF THE INVENTION

The crossflow axes rotary mechanical devices include different types of devices such as wind turbines, hydro turbines, propellers, fan-blowers, pump-compressors, mixers etc. These devices share common characteristics, effects, parameters and mechanisms such as rotors with arms and blades, support structures, electric machines (electric generators or electric motors) along with the parameters defining the devices and their mechanical and physical behaviors, but above all they share the main characteristic which is the orientation of their axes of rotation being always perpendicular to the flow.

The crossflow axes turbines represent the main crossflow axes rotary mechanical devices and have a long history of designs (the drag type disclosed in the US Patent No. 1,766,765, the lift type disclosed in the US Patent No. 1,835,018).

Main advantage of crossflow axes turbines is being omni directional (compare to the flow axes turbines, the crossflow axes turbines do not need to be pointed into the flow direction).

Main disadvantage of crossflow axes turbines is being less efficient than the flow axes turbines, mainly because of the limited swept area used by the devices to create positive torque (to extract energy). Fig. la is a schematic display of a crossflow axes lift turbine 10, rotor 1 1, the swept area 24 and the limited swept area "Lift Area" used by the turbine to create positive torque, while Fig. lb is a schematic display of a crossflow axes drag turbine 10, rotor 1 1, the swept area 24 and the limited swept area "Energy Extraction Area" used by the turbine to create positive torque (from the free fluid flow point of view, the amount of the fluid being "processed" by the crossflow axes turbines is less than the amount of the fluid being "processed" by the flow axes turbines, space wise).

Other disadvantages of the crossflow axes turbines are the pulsation of the blades for each revolution passing through different pressure parts (especially for the lift type crossflow axes turbines that have stress forces on the blades vary from compressional to tensional for each revolution), bending moment created on the rotor shaft (especially for large structures), the negative effects that the turbulent wakes created by the blades of lift type turbine have on the blades that passes them, the transmission of the fluctuating loads to the support structure (as well as to the other systems such as the foundation system, shaft system, generator system, bearings etc), self starting problem (the lift type turbines), lack of fluid dynamic braking (aerodynamic braking or hydrodynamic braking), unsmooth torque curve and vibrations.

The present invention seeks to provide a new class of crossflow axes rotary mechanical devices, which may become more efficient than the current class of crossflow axes rotary mechanical devices and may overcome some of the disadvantages listed above. SUMMARY OF THE INVENTION

(From here on DISA means Dynamic Increased Swept Area, CARM means Crossflow Axes Rotary Mechanical, Y - Device Yawing Angle, TSR - Tip Speed Ratio, S - Solidity of the blade turbine, R - Reynolds Number, BL - Blade Boundary Layer, VT - Vortex Type, Βχ - Blade Type (shape, foil), F _T - Fluid Type (air, water), B _N - Blade Numbers, β - Blade Pitch Angle (foil blades), Ro - Rotors Offset, 6BR - the space between each blade's tip and the opposite rotor's plane, 5B - the minimum space between two crossing blades from opposite rotors, BS - Blade Spacing per Rotor, BSBR - Blade Spacing Between Rotors).

The CARM devices with DISA create a new class (a super class) compare to the conventional CARM devices class, because they include (inherit) all the characteristics, effects, parameters and mechanisms of the conventional CARM devices plus new ones such as:

• New characteristics - the main new characteristic the CARM devices with DISA have compare to the conventional CARM devices (without DISA), is the increased swept area (especially the energy extracting/exerting part of the swept area) in a dynamic way, comparing to the conventional CARM devices that may increase their swept area statically by static ducting, helical blades etc. The increase of the "energy extracting/exerting" part of the swept area means more fluid being "processed" by the CARM devices with DISA (space and material wise), or less fluid escaping "unprocessed" from these devices (from this point of view the Dynamic Increased Swept Area concept is equivalent to the Dynamic Increased Processed Fluid concept). The CARM devices with DISA may change the size of their swept area (or the amount of fluid being processed) depending on different factors, such as the device relative position to the flow direction, counter or co rotating rotors, blade pitch angle etc. Another characteristic of the CARM devices with DISA is the modularity. The base of the CARM devices with DISA is a module of at least two rotors sharing their spaces, the fluid, the support structure, the rotors synchronizing mechanisms, the electric machines, the braking systems, the yawing systems, as well as the characteristics, parameters, and effects. The CARM devices with DISA can have a plurality (array) of modules, where they can share among them the support structure, the electric machines as well as the torque, the fluctuating loads etc.

New effects - the CARM devices with DISA experience new effects compare to the conventional CARM devices (without DISA), such as:

> Dynamic Ducting - it is created by the blades of opposite rotors rotating relative to each other, decreasing the "escaping" or "unprocessed" fluid from the device, increasing the "processed" fluid by the device space and material wise (it effects both lift and drag devices)

> Dynamic Flow Deflection - it is created by the blades of opposite rotors rotating relative to each other, changing in turn the direction of the fluid by "entrapping" it, increasing the "processed" fluid by the device and the speed of it, space and material wise (it effects both lift and drag devices)

> Dynamic Fluid Shield - it is created by the blades of opposite rotors rotating relative to each other, where for the lift type devices each blade of one rotor forms a fluid "shield" to the blades of the opposite rotor decreasing the negative drag forces, while for the drag type devices the blades rotating against the fluid direction reduce their shape thus decreasing the negative drag forces (it effects both lift and drag devices)

> Dynamic Fluid Braking - it is created by positioning the new CARM devices with DISA relative to the flow direction, thus changing the size of the "energy

extracting/exerting" part of the swept area, or the amount of the fluid processed by the device (it effects both lift and drag devices)

> Dynamic Wake Cancel - it is created by the lift type blades of the opposite rotors counter rotating relative to each other, producing counter rotating wakes that may cancel each other in the process, thus decreasing the wake effect to the blades on the down flow part (it effects the lift devices)

> Dynamic Change of Blade Angle of Attack (by Dynamic Flow Deflection) - it is created by the foil (lift) blades of opposite rotors rotating relative to each other, maintaining an optimal blade angle of attack for the lift forces during the rotation, as well as delaying the deep stalling and the wake creation process (it effects the lift devices)

These effects depend on different factors such as the type of the devices (lift, drag), relative position of the devices to the flow direction, rotors offset Ro counter rotating or co rotating rotors, blade numbers, blade pitch angle, blade spacing between Rotors BSBR etc

(different combination of the factors mentioned above may favor some effects and disfavor the others).

• New parameters - the CARM devices with DISA have new parameters compare to the conventional CARM devices (without DISA), such as:

> 5BR - the space between each blade's tip and the opposite rotor-arm plane

δβ - the minimum space between two crossing blades from opposite rotors

> Ro - Rotors Offset, which is the distance between two offset parallel rotors axes

> Y - Yaw angle, which determines the position of the devices "energy

extracting/exerting" part of the swept area relative to the flow direction > BSBR - Blade Spacing Between Rotors 0° <= BSBR < 180°, which is the angle

between the two close blades from opposite rotors on a plane parallel to the rotors, where one of the blades is at the φ = 0° rotating phase angle

> BRA - Blade Rotation Angle 0° < BRA < 90°, which is the maximum angle of the rotating blade (drag type) relative to its rotor on the rotor-arm plane

· Additional mechanisms - the CARM devices with DISA have additional mechanisms compare to the conventional CARM devices (without DISA), such as:

> rotors synchronizing mechanism - a mechanism that synchronizes the rotors rotation relative to each other with the same TSR, avoiding the blades of the opposite rotors collision during the rotation, serving as shaft mechanism (lift and drag devices) blade-rotor synchronizing mechanism - a mechanism that synchronizes the rotation of the blade relative to its rotor along with the rotors synchronizing mechanism in such way that the blades of the opposing rotors do not collide during the rotation (drag devices)

> blades synchronizing mechanism - a mechanism that synchronizes the blades rotation (for the same rotor) during the rotors rotation, and is linked to the blade-rotor synchronizing mechanism in such way that the blades of the opposing rotors do not collide during the rotation (drag devices) > yaw mechanism - a mechanism that orients the new devices "energy extracting/exerting" part of the swept area relative to the flow direction for a maximum "energy extracting/exerting" value (lift and drag devices)

The CARM devices with DISA of the new class (supper class) tent to become conventional CARM devices without DISA (conventional class) when the CARM devices with DISA are dismounted or half mounted (in this case the CARM devices with DISA loses completely the new characteristics, new parameters, new effects and the additional mechanisms, becoming conventional CARM devices without DISA), or when the CARM devices with DISA change their position relative to the flow direction (in this case the CARM devices with DISA decrease the "energy extracting/exerting" part of swept area, decreasing their gains from the new characteristics, new parameters, new effects and the additional mechanisms, tenting to become conventional CARM devices without DISA).

A CARM device with DISA include at its base at least two rotors with equal radial arm sizes (meaning two rotors with equal radius size where each rotor's radius is the arm) attached to a support structure, where the rotors with arms are parallel to each other and have parallel axes of rotation on a plane perpendicular to the fluid (the rotors axes of rotation may be vertical, horizontal or have any angle on the plane that is always perpendicular to the fluid). The rotors rotate (counter rotate or co rotate in the case of lift devices) relative to each other in synchrony with the same TSR by at least one rotors synchronizing mechanism. The rotors can be coaxial or non coaxial with a rotors offset 0 <= Ro < 2R, where R is the rotor radius or the radial arm size (for the value of Ro = 0 the rotors are coaxial). The CARM device with DISA further includes at least one blade attached to each rotor via the radial arm on the side between the rotors (the device may have different number of blades varying on different factors, such as the type of CARM device, fluid type, fluid speed etc). There is a space between each blade's tip and the opposite rotor's plane 5BR >= RFR, where RFR is the Rotors Freedom of Rotation (meaning that the blades of one rotor do not collide with the opposite rotor during the rotation), and a minimum space between two close blades from opposite rotors crossing each other during the rotation 5B >= BNCS, where BNCS is the Blades Non Collision Space (meaning that the blades of the opposite rotors do not collide during the rotation). There is a Blade Spacing Between Rotors 0° <= BSBR < 180°, which is the angle between two close blades from opposite rotors on a plane parallel to the rotor-am plane, where one of the blades is at the 0° rotating phase angle.

A CARM device with DISA further includes at least one electric machine, which might be an electric generator (turbines), or an electric motor (propellers, fan-blowers, pump-compressors, mixers etc). A CARM device with DISA has one support structure of different types, where the whole device is mounted. A CARM device with DISA may extract (exert) energy from gases, liquids or both of them. The two opposite rotors of a CARM device with DISA with blades attached via arms share a common space, fluid and other systems like the support structure system, the synchronizing mechanism, the electric machine (generator/motor), the braking system, the yawing system etc, forming one device module.

The synchronization of relative rotating rotors of a CARM device with DISA at the same TSR (avoiding the collision of the opposite rotors blades during the rotation) can be realized by at least one synchronizing mechanism. The rotors synchronizing mechanism can be mechanical, including one shaft connected to both rotors parallel to the rotors axes of rotation and gearing mechanism to keep the rotors synchronized at the same TSR (the shaft transmits the torque of one rotor to the electric machine connected to the other rotor), or can be electrical including one electric motor/generator per each rotor, an algorithm, and a system that links the electric motor/generator by wire or wireless (in this case the synchronizing electromechanical system behaves like an electromagnetic gearing system, while the algorithm programme can synchronize counter (co) rotating rotors, as well as their speed according to the maximum efficiency curve for different fluid speeds, with the right chosen parameters).

A CARM device with DISA may include blades on the side not between the rotors as well, where the angle between two closest blades of each rotor on the rotor-arm plane is 0° <= BSR <= 180°. In this case there is a hybrid of a CARM device with DISA operating on the side between the rotors, and a conventional CARM device operating on the side not between the rotors.

A CARM device with DISA may have an array of modules, where the angle between two closest blades of each rotor on the rotor-arm plane may be 0° <= BSR <= 180°. The modules may have blades with the same height (one module of rotors have always the same blades height and this is defined by the 6BR), or different modules may have blades with different heights. The array of modules may have one electric machine or different ones along the array of modules (in this case each electric machine may have a dual role as a generator/motor and a synchronizer).

The CARM devices with DISA that have an electric machine as an electric generator for extracting energy from the fluid, creates a subclass of crossflow axes turbines with DISA.

A crossflow axes turbine with DISA may have different braking systems such as mechanical braking, electromagnetic braking, fluid dynamic braking or the combination of them (the fluid dynamic braking is a new characteristic of the new devices with DISA, and this may be realized by changing the device position relative to the flow, by changing the blade pitch angle for lift type turbines or combination of them). A crossflow axes turbine with DISA is not "fully" omni directional, but instead a "semi" omni directional device (meaning that the new device would always work on any position relative to the flow direction, but its performance would be different for different positions of the device relative to the flow direction). The position of the new device relative to the flow direction may be defined by the yaw angle Y. The yaw system of a crossflow axes turbine with DISA may include a passive yaw system (vane system), an active yaw system with electric motors, or a combination of them.

The crossflow axes turbines with DISA where the blades profile is a foil create a new subclass of crossflow axes lift turbines with DISA. In this case the rotors are non coaxial and the rotors offset Ro is a function of Ro = f (δ _Β . Y, TSR, S, R _N , B _L , V _T , B _T , F _T , B _N , β _, B _SR, B _SB ).

A crossflow axes lift turbine with DISA may have rotors counter rotating or co rotating in synchrony by the rotors synchronizing mechanism.

A crossflow axes lift turbine with DISA may have fixed blade pitch angle, where the pitch angle may be a function of β = f (Y, Ro, TSR, S, R _N , B _L , V _T , B _T , F _T , B _N , B _SR , B _S BR). The fixed pitch angle may be the same for all the blades, or may be different for different blades of the same rotor or different rotors, and this depends on β function parameters (especially the BsR and BsBR parameters).

A crossflow axes lift turbine with DISA may have variable blade pitch angle, where the variable pitch angle may be a function of β = f (Y, Ro _, TSR, S, R _N , B _L , V _T , B _T , F _T, B _N , B _SR , B _SBR ). The variable pitch angle does not change per one revolution, but it is more a reset of the pitch angle adjusted to the flow speed and direction changes (in the case of flow direction changes, the variable pitch angle may be adjusted to combine with different yaw systems).

A crossflow axes lift turbine with DISA may have different blades geometry per rotor or between rotors, such as straight, curved (semi helical blade), swept (semi delta blade) or a combination of them. The new turbine may have different blade foils per rotor or between rotors, as well as symmetric or asymmetric foil (the blades with asymmetric foil may have an advantage compare to symmetric one, because it can extract all the energy on the up flow part where there is less fluid flowing through new devices, so there is no need for a symmetric foil getting lift on the down flow part, as a result the stress forces on the blades would not vary from compressional to tensional for each revolution).

A crossflow axes lift turbine with DISA may include a plurality of struts, mechanically coupling the blade to its arm. The crossflow axes turbines with DISA having curved vanes (drag type blades) and counter rotating rotors create a subclass of crossflow axes drag turbines with DISA, where the rotors can be co axial or non coaxial.

A crossflow axes drag turbine with DISA of type 1 includes at least two coaxial rotors rotating relative to each other in synchrony by a rotor synchronizing mechanism. It includes at least two opposite symmetric base blades fixedly attached to each rotor via the radial arm, overlapping each other in the centre of the rotor, where each base blade has an angle to its rotor plane on the rotors axes side <= 90°. It further includes one base blade extension on the outer side of each base blade of one rotor having an angle to its rotor plane on the rotors axes side < 90°, and one base blade extension on the inner side of each base blade of the other rotor having an angle to its rotor plane on the rotors axes side < 90°. In addition, the shape of each blade extension is configured to create a maximum dynamic fluid ducting and dynamic fluid deflection with the opposite rotor blade extensions crossing each other at their crossing section during the rotation, having a minimum space between them δβ.

A crossflow axes drag turbine with DISA of type 2 includes at least two non coaxial rotors rotating relative to each other in synchrony by a rotor synchronizing mechanism, and at least two opposite symmetric blades fixedly attached to each rotor where the closest distance of each blade to the rotor centre is greater than the half of the respective rotor's arm.

A crossflow axes drag turbine with DISA of type 3 includes at least two coaxial rotors rotating relative to each other in synchrony by a rotor synchronizing mechanism, at least two opposite symmetric blades per rotor attached to the respective rotating axis perpendicular to the rotor-arm plane on the radial arm where the blades rotate relative to their rotor with a maximum BRA angle <=90°, and the distance of the blade rotating axis from the rotor centre is greater than the half of rotor's radial arm. It further includes at least one curved rail blade-rotor relative rotation mechanism per rotor fixedly attached to the support structure parallel to the rotor-arm plane on the side not between the rotors at the lower flow side, where the curved rail rotates each blade with a maximum BRA angle from its radial arm. It further includes a wheel at the outer lower edge of each blade with an axis of rotation perpendicular to the rotor-arm plane contacting the inner curved rail during the rotation at the lower flow side, one step on the rotor arm for each blade to stop the blade rotating relative to its rotor and one curved blades synchronizing mechanism for the blades of the same rotor.

A crossflow axes drag turbine with DISA of type 3 that have non coaxial rotors form a crossflow axes drag turbine with DISA of type 4 (in this case the blades may rotate partially around the axis which is perpendicular to the rotors plane). A crossflow axes drag turbine with DISA of type 5 includes at least two coaxial rotors rotating relative to each other in synchrony by a rotor synchronizing mechanism, at least two opposite symmetric blades per rotor fixedly attached to a diameter arm with an angle B A ^<= 90° between them where the arm is attached to the rotor to rotate relative to it around its own axis with a maximum B A angle, at least one curved rail blade-rotor relative rotation mechanisms per rotor fixedly attached to the support structure on the side not between the rotors at the lower flow side, where the curved rail lays on a cylinder with a radius greater than the rotors radius perpendicular to the rotor-arm plane and the curved rail rotates each blade with a maximum BRA angle, including a wheel at the outer edge of each blade opposite to its rotor with an axis of rotation parallel to the rotor-arm plane, where the wheels of the blades of one rotor contact the inner side of the curved rail while the wheels of the blades of the opposite rotor contact the outer side of the curved rail during the rotation at the lower flow side and one step on the rotor plane for each diameter arm to stop the arm with blade rotating relative to its rotor where the BRA angle is maximum.

A crossflow axes drag turbine with DISA of type 3, type 4 or type 5 may have both the blade- rotor relative rotation mechanisms of a module of two rotors rotating around the rotor axes of rotation according to the flow direction. In this case, the rotating of the blade-rotor relative rotation mechanisms behaves like a yawing mechanism.

A crossflow axes drag turbine with DISA of type 1, type 2, or type 5 that have one module of two rotors, may have an end disk for each rotor to increase the static ducting (for the array of modules there is no need of such end disks).

The crossflow axes drag turbine with DISA of type 1, type 2, type 3, type 4 or type 5 may include different static ducting systems connected to the support structure.

The CARM devices with DISA that inherit all the characteristics of any of the devices mentioned above, having an electric machine as an electric motor for exerting energy to the fluid create different type of CARM devices with DISA, such as crossflow axes propeller with DISA, crossflow axes fan-blower with DISA, crossflow axes pump-compressor with DISA, and crossflow axes mixer with DISA.

BRIEF DESCRIPTION OF THE DRAWINGS Fig. la is a schematic display of the swept area of a conventional crossflow axes lift type turbine (prior art). Fig. l b is a schematic display of the swept area of a conventional crossflow drag type turbine (prior art). Fig.2a is a schematic display of the swept area of a crossflow axes lift turbine with DISA, where the rotors counter rotates relative to each other. Fig.2b is a schematic display of the crossflow drag turbine swept area.

Fig.3a is a schematic display of the size changes (decrease) of the energy extracting (lift) zone of a crossflow axes lift turbine with DISA. Fig.3b is a schematic display of the size changes (decrease) of the energy extracting zone of a crossflow axes drag turbine with DISA compare. Fig.4a is the axonometric view of a crossflow axes lift turbine with DISA. Fig.4b is a schematic display of a crossflow axes lift turbine with DISA.

Fig.5a is a schematic display of the drive shaft rotors synchronizing mechanism for a CARM device with DISA. Fig.5b is a schematic display of the electric rotors synchronizing mechanism for a CARM device with DISA.

Fig.6 is the axonometric views of crossflow axes lift turbines with DISA having different blades number, spacing and geometry per each rotor.

Fig.7a is the front view of a crossflow axes lift turbine with DISA having an array of two rotor modules with the same blades height. Fig.7b is the front view of a crossflow axes lift turbine with DISA having an array of two rotor modules with different blades height per different modules, having different electric machine along the array of modules.

Fig.8a is the axonometric view of a crossflow axes lift turbine with DISA having a passive yawing mechanism. Fig.8b is the front view of a crossflow axes lift turbine with DISA with an array of rotors, having an active yawing mechanism. Fig.8c is a schematic display of a crossflow axes lift turbine with DISA having a passive yawing mechanism. Fig.8d is a schematic display of a crossflow axes drag turbine with DISA having a passive yawing mechanism.

Fig.9a and Fig.9b are the schematic displays the crossflow axes lift turbines with DISA, having fixed blade pitch angle. Fig.9c is the schematic display of the Dynamic Wake Cancel effect. Fig.10 is the axonometric view of a crossflow axes drag turbine with DISA type 1, having fixed drag blades type and coaxial rotors.

Fig. l 1 is the axonometric of a crossflow axes drag turbine with DISA type 2, having fixed drag blades type and non coaxial rotors (including static ducting).

Fig.12 is the axonometric view of a crossflow axes drag turbine with DISA type 3, having variable drag blades rotating around an axis which is perpendicular to the rotor plane (coaxial rotors).

Fig.13 is the axonometric view of a crossflow axes drag turbine with DISA type 4, having variable drag blades rotating around an axis which is perpendicular to the rotor plane (non coaxial rotors). Fig.14 is the axonometric view of a crossflow axes drag turbine with DISA type 5, having variable drag blades rotating around an axis which is parallel to the rotor plane (coaxial rotors).

DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS

Fig.2a is a schematic display of a crossflow axes lift turbine with DISA 10 showing counter rotating Rotor 1 1 and 12 with a rotors offset Ro, the general swept area of each rotor 24 and 25 creating an increased of general swept area of the turbine (space wise) compare to the swept area of a conventional crossflow lift turbine (Fig. la), the energy extracting Lift Area 1 1 and Lift Area 12 created by respective Rotor 1 1 and 12. The lift part of the swept area for each rotor starts close to φ = 0 (the blades have a negative pitch angle), where the lift swept areas of the opposite rotors are distanced from each other, creating favorable condition for dynamic effects such as Dynamic Ducting, Dynamic Flow Deflection and Dynamic Change of Blade Angle of Attack. Fig.2b is a schematic display of a crossflow axes drag turbine with DISA 10, showing counter rotating Rotors 1 1 and 12 with a rotors offset Ro, the swept areas 24 and 25, the Energy

Extracting Area 1 1 and 12 created by respective Rotor 1 1 and 12 on both sides of the device (compare to the Energy Extracting Area of conventional crossflow drag turbine Fig. lb).

Fig.3a is a schematic display of a crossflow axes lift turbine with DISA 10, showing counter rotating Rotors 1 1 and 12 with a rotors offset Ro, the energy extracting area Lift Area 11 and 12 created by respective rotors 1 1 and 12. In this case the Lift Area 1 1 is decreased because of the change of the flow direction relative to the device compare to Fig.2a, and this can be used as a device dynamic fluid braking.

Fig.3b is schematic displays of a crossflow axes drag turbine with DISA 10, showing counter rotating Rotors 1 1 and 12 with a rotors offset Ro, the Energy Extracting Area 1 1 and 12 created by respective Rotor 11 and 12. In this case both the Energy Extracting Areas are decreased because of the change of the flow direction relative to the device compare to Fig.2b.

Fig.4a shows a crossflow axes lift turbine with DISA 10, Rotor 11 and Rotor 12 with radial arms 2 of equal sizes attached to a support structure 6 parallel to each other, having their respective axes of rotation 3 on a plane perpendicular to the fluid (it can be different angles of rotors axes of rotation 3 on a plane perpendicular to the fluid) with a rotors offset Ro > 0. There are two blades 21 attached to Rotor 1 1 and two blades 22 attached to Rotor 12 via radial arms 2 on the side 50 between the two rotors, a space 5BR ^>= RFR between each blade's tip and the opposite rotor's plane and a minimum space 6B >- BNCS between two close blades from opposite rotors crossing each other during the rotation. The rotors counter rotate relative to each other in synchrony at the same TSR by at least one rotors synchronizing mechanism 4, forming one module of two rotors. There is one electric machine 5 (in this case an electric generator) connected to the rotors, and there is a support structure 6 supporting the rotors with arms, blades, rotors synchronizing mechanism and the electric generator.

Fig.4b is a schematic display of a crossflow axes lift turbine with DISA 10 having one module of two counter rotating rotors 11 and 12 with rotors offset Ro, two blades 21 attached to Rotor 1 1 via arms 2 and two blades 22 attached to Rotor 12 via arms 2, the blades spacing per each rotor B _S R of blades 22 of Rotor 12, the blades spacing between rotors B _SB R (90° in this case), blade 21 of Rotor 1 1 and blade 22 of Rotor 12 where the blade 22 is at the φ = 0° rotating phase angle. Fig.5a shows the mechanical rotors synchronizing mechanism 4 for CARM devices with DISA, composed by the shaft 7 and the gearing mechanism 8 to keep the rotors rotation synchronized at the same TSR. Gearing mechanisms 8 may have different variations, such as:

A. offset rotor counter rotating, having x:y gears (x = y for the same TSR)

•B. offset rotor co rotating, having x:z:y gears (z serves for co rotating rotors)

C. coaxial rotors counter rotating, having 3x: lz / 2z:6x gears

D. coaxial rotors co rotating, having x:y / y.x gears

Fig.5b shows the electrical rotors synchronizing mechanism 4 for CARM devices with DISA, composed by one electric motor/generator 5 per each rotor, an algorithm and a system that links the electric motor/generator by wire or wireless (in this case the synchronizing electromechanical system it may behave like an electromagnetic gearing system to keep the rotors synchronized). Fig.6 shows a crossflow axes lift turbine with DISA 10 having one module of two counter rotating rotors 1 1 and 12 with a rotors offset Ro, synchronizing mechanism 4, generator 5, support structure 6, including blades on the side 51 not between the rotors. This embodiment has a hybrid of crossflow axes lift turbine with DISA operating on the side 50 between the rotors, and a conventional crossflow axes turbine operating on the side 51 not between the rotors. This embodiment has different numbers of blades per each rotor (on the side between and not between the rotors), and different blades spacing BSR per each rotor. It shows the straight blade 21 , curved blade 22 and swept blade 23, including blade struts 13.

Fig.7a shows a crossflow axes lift turbine with DISA 10 having an array of modules 7 (rotor 1 1 and 12 per module counter rotating with a rotors offset Ro), blades 1 with the same height attached to the rotors via arms, one rotors synchronizing mechanism 4 per module, one shared electric generator 5 and support structure 6. This embodiment has different blades spacing BS per each rotor on each side of it (this can smooth the torque curve, and share the loads on different modules). Fig.7b shows a crossflow axes lift turbine with DISA 10 having an array of modules 7 (rotor 1 1 and 12 per module counter rotating with a rotors offset Ro) with different blades height per different modules attached to the rotors via arms, having different electric machine 5 along the array of modules (in this case each electric machine may have a dual role as a generator/motor and rotors synchronizer) and support structure 6.

Fig.8a shows a crossflow axes lift turbine with DISA 10, counter rotating Rotors 1 1 and 12 with a rotors offset Ro, two blades 1 per rotor attached to the rotors via arms 2, synchronizing mechanism 4, generator 5, support structure 6, and a passive yaw mechanism 9.

Fig.8b shows a crossflow lift turbine with DISA 10 having an array of modules 7 (counter rotating rotors 1 1 and rotor 12 per module with a rotors offset Ro) mounted on each side of a support structure 6, synchronizing mechanism 4 per each module, and generator 5 (in this embodiment the array of modules rotate around the support structure by an active yaw system 9). Fig.8c is a schematic display of a crossflow axes lift turbine with DISA 10, counter rotating Rotors 1 1 and 12 with a rotors offset Ro, the yaw angle Y(l) for the lift type devices, which is the angle between the fluid direction (the upper side) and the perpendicular of the device rotors co diameter (or the angle between the fluid direction and the yaw vane 9 direction).

Fig.8d is a schematic display of a crossflow axes drag turbine with DISA 10, two counter rotating rotors 1 1 and 12, the yaw angle Y(d), which is the angle between the fluid direction (the upper side) and parallel of the device "energy extracting/exerting" part of swept area, where the "energy extracting/exerting" part swept area of these device is maximum (or the angle between the fluid direction and the yaw vane 9 direction).

Fig.9a shows a schematic display of a crossflow axes lift turbine with DISA 10, two counter rotating rotors 1 1 and 12 with a rotors offset Ro, blades 21 and 22 having blade pitch angle β fixed where pitch angle is a function of β = f (Y, Ro_ TSR, S, R _N , B _L , V _T , B _T , F _T, B _N, BS _, B _S BR)- The fixed pitch angle β may be the same for all the blades or may be different for different blades for the same rotor or different rotors, and this depends on different parameters, especially the BSR and BSBR parameters. The fixed pitch angle β for the counter rotating rotors may be negative to create an earlier lift for each rotor blades, so each blade from opposite rotors have a lift swept area distanced from each other (the preset negative pitch angle may decrease the drag on the blades as well). The blade 22 of rotor 12 has a pitch angle β at φ = 90, fluid speed U,

V= -UJ*R, the relative fluid speed W, angle of attack a, lift force L, and drag force D, while the blade 21 of rotor 1 1 has the same pitch angle β, at φ = 0 the fluid speed U, V= -U)*R, the relative fluid speed W, angle of attack a, lift force L, and drag force D. The zone 26 of the rotor path 24 represents the Dynamic Fluid Shield from the blades of rotor 12 to the blades of rotor 1 1, while the zone 27 of the rotor path 21 represents the Dynamic Fluid Shield from the blades of rotor 1 1 to the blades of rotor 12.

Fig.9b shows a schematic display of crossflow axes lift turbine with DISA 10, two counter rotating rotors 1 1 and 2 with a rotors offset Ro, the blade 21 of rotor 1 1 with a pitch angle β at φ = 45, fluid speed U, increased fluid speed Ui deflected by the blade 22 of rotor 12 at φ = 45, a resultant fluid speed U ₂ , V= -w*R, the relative fluid speed Wi which comes as a result of U ₂ and V, angle of attack ai which is different because of U ₂ and Wi, lift force Li, and drag force D. It shows the Dynamic Ducting 28 that entraps some of the fluid coming from opposite rotor blades, the Dynamic Change of Blade Angle of Attack 29 caused by Dynamic Flow Deflection maintaining a steady increase of angle of attack ai for an optimal lift, as well as delaying the deep stalling process and the wake creation process.

Fig.9c shows a schematic display of crossflow axes lift turbine with DISA 10, two counter rotating rotors 1 1 and 12 with a rotors offset Ro, the blade 21 of rotor 1 1, the blade 22 of rotor 12, Vortex 1 1 created by the blades 21 of rotor 11, Vortex 12 created by the blades 22 of rotor 12 at a different time compare to Vortex 1 1, and the Dynamic Wake Cancel process.

Fig.10 shows a crossflow axes drag turbine with DISA 10 type 1, having coaxial rotors 11 and 12 counter rotating relative to each other, synchronizing mechanism 4, generator 5, support structure 6, two opposite symmetric fixed base blades 30 per rotor, two opposite symmetric fixed base blades extension 31 on the outer part of base blade 30, two opposite symmetric fixed base blades extension 32 on the inner part of base blade 30, base blade angle to the rotor plane 33, base blade extension angle to the rotor plane 34, the minimum space between two crossing blades from opposite rotors 5B.

Fig. l 1 shows a crossflow axes drag turbine with DISA 10 type 2, having non coaxial rotors 1 1 and 12 with a rotors offset Ro counter rotating relative to each other, two fixed blade 1 per rotor, the minimum space between two crossing blades from opposite rotors 5B, synchronizing mechanism 4, generator 5, support structure 6..

Fig.12 shows a crossflow axes drag turbine with DISA 10 type 3, having coaxial rotors 1 1 and 12 counter rotating relative to each other, synchronizing mechanism 4, generator 5, support structure 6, two symmetric blades 1 per rotor rotating relative to their rotor around an axis 44 which is perpendicular to the rotors plane on the arm 2 with a maximum BRA angle, at least one curved rail blade-rotor relative rotation mechanisms 40 per rotor fixed to the support structure parallel to the rotors plane, a wheel 41 at the outer lower edge of each blade with an axis of rotation perpendicular to the rotor-arm plane, one rotor step 43 on the rotor plane for each blade, and one curved blades synchronizing mechanism 42 for the blades of the same rotor. Fig.13 shows a crossflow axes drag turbine with DISA 10 type 4, having non coaxial rotors 11 and 12 counter rotating relative to each other with a Rotors Offset Axes Ro, synchronizing mechanism 4, generator 5, support structure 6, two symmetric blades 1 per rotor rotating relative to their rotor around an axis 44 which is perpendicular to the rotors plane on the arm 2 with a maximum BRA angle, at least one curved rail blade-rotor relative rotation mechanisms 40 per rotor fixed to the support structure parallel to the rotors plane, a wheel 41 at the outer lower edge of each blade with an axis of rotation perpendicular to the rotor-arm plane, one rotor step 43 on the rotor plane for each blade, and one curved blades synchronizing mechanism 42 for the blades of the same rotor.

Fig.14 shows a crossflow axes drag turbine with DISA 10 type 5, having coaxial rotors 1 1 and 12 counter rotating relative to each other, synchronizing mechanism 4, generator 5, support structure 6, two symmetric blades 1 per rotor fixedly attached to a diameter arm 2 with an angle BRA ^<= 90° between them, where the arm 2 rotate relative to the rotor around its own axis with a maximum BRA angle, at least one curved rail blade-rotor relative rotation mechanisms 40 per rotor fixedly attached to the support structure on the side not between the rotors at the lower flow side, a wheel 41 at the outer edge of each blade opposite to its rotor with an axis of rotation parallel to the rotor-arm plane, one step on the rotor plane for each diameter arm to stop the arm with blade rotating relative to its rotor, wherein the B A angle is maximum.

Fig.4a, Fig.6, Fig.10, Fig.11, Fig.12, Fig.13, Fig.14 represent the CARM devices with DISA, where the electric machine is an electric generator. By replacing the electric generator with an electric motor, these embodiments create different devices such as crossflow axes propeller with DISA, crossflow axes fan-blower with DISA, crossflow axes pump-compressor with DISA, crossflow axes mixer with DISA inheriting any characteristic of the devices mentioned above. The CARM devices with DISA are characterized by a tradeoff between the advantages and disadvantages of the conventional CARM devices. The main advantage of the conventional CARM devices, which is the omni directional mentioned at the background of the invention section would becomes less advantageous for the CARM devices with DISA, because they are not fully omni directional anymore but semi omni directional. On the other hand the main disadvantages of the conventional CARM devices mentioned at the background of the invention section would become less disadvantageous for the new CARM devices with DISA, because of the new characteristics and effects the CARM devices with DISA have compare to the conventional CARM devices.