The present invention relates to the field of turbines and more specifically concerns turbines with oscillating foils.
The prospect of harvesting water flow energy with hydrokinetic turbines is becoming more attractive than ever among renewable forms of energy, due to the high energy density of flowing water, to its predictability with both tidal and river applications, and the minimal environmental and human impact.
Known to the Applicant are the following publications and patent documents:
[1] The European Marine Energy Centre Ltd (EMEC), (2010): http://www.emec.org.uk/tidal_devices.asp
[2] Bernitsas, M., Raghavan, K., Ben-Simon, Y., and E.M.H., G., (2008). VIVACE (Vortex Induced Vibration Aquatic Clean Energy): A new concept in the generation of clean and renewable energy from fluid flow. ASME Journal of Offshore Mechanics and Arctic Engineering, 130(4), November, p. 041101.
[3] Bernitsas, M., Ben-Simon, Y., Raghavan, K., and E.M.H., G., (2009). The VIVACE Converter: Model tests at high damping and Reynolds number around 105. ASME Journal of Offshore Mechanics and Arctic Engineering, 131(1), February, p. 011102.
[4] Jones, K., Lindsey, K., and Platzer, M. (2003). An investigation of the fluid-structure interaction in an oscillating wing micro-hydropower generator. Fluid Structure Interaction II, Chakrabarti, Brebbia, Almorza, and Gonzalez-Palma, eds. WIT Press, Southampton, UK, pp. 73-82.
[5] Kinsey, T. and Dumas, G. (2010). Testing and Analysis of an Oscillating Hydrofoils Turbine Concept. ASME 2010 3rd Joint US-European Fluids Engineering Summer Meeting, Paper FEDSMICNMM2010-30869, Montreal, Canada
[6] Kinsey, T. and Dumas, G. (2008). Parametric Study of an Oscillating Airfoil in a Power-Extraction Regime. AIM Journal, 46 (6), pp. 1318-1330
[7] McKinney, W. and DeLaurier, J. (1981). The Wingmill: An Oscillating-Wing Windmill. Journal of Energy, Vol. 5, No. 2, pp. 109-115
[8] Pulse Tidal Limited, (2010): http://www.pulsegeneration.co.uk.
[9] The Engineering Business Limited, (2002). Research and development of a 150 kw tidal stream generator. Tech. rep., Crown Copyright.
[10] The Engineering Business Limited, (2003). Stingray tidal energy device—phase 2. Tech. rep., The Engineering Business Limited.
[11] The Engineering Business Limited, (2005). Stingray tidal energy device—phase 3. Tech. rep., Crown Copyright.
[12] Anderson, J. M. et al., (1998). Oscillating Foils of High Propulsive Efficiency. Journal of Fluid Mechanics, Vol. 360, April 1998, pp. 41-72. doi:10.1017/S0022112097008392
[13] Dumas, G. (2010). HAO-Laval: Le projet d'hydrolienne à ailes oscillantes. Journal de I'AQME, September 2010, Vol. 25 (3), pp. 8-10.
[14] Kinsey, T., Dumas, G., Lalande, G., Ruel, J., Mehut, A., Viarouge, P., Lemay, J. and Jean, Y. (2011). Prototype Testing of a Hydrokinetic Turbine Based on Oscillating Hydrofoils. Renewable Energy, 36 (6), pp. 1710-1718.
Also known to the Applicant are these related patents:
U.S. Pat. No. 7,493,759 B2 February 2009 Bernitsas et al. (VIVACE); WO 2004110859A1 June 2004 Lambert-Bolduc (Éolo); WO 2005108781A1 May 2005 Paish (Pulse Tidal); US 20060275109 A1 December 2006 Paish (Pulse Tidal); WO 2008053167A1 May 2008 Paish (Pulse Tidal); WO 2010015821A2 February 2010 Paish (Pulse Tidal); WO 2008144938A1 May 2008 Dumas et al. (U. Laval); U.S. Pat. No. 6,273,680 B1 August 2001 Arnold; and U.S. Pat. No. 6,323,563 B1 November 2001 Kallenberg.
Referring to
When submitted to a fluid flow, an oscillating foil undergoes a combined sinusoidal, or quasi-sinusoidal, heave-pitch motion. It is known that the efficiency of a turbine is improved when the heaving, or translational, motion is leading the pitching, or angular motion.
With reference to
Although functional, this implementation has some drawbacks. One of them comes from the use of the elongated rods 18a, 18b oscillating into the flowing water which causes a loss of energy. Another drawback is that the hydrodynamic forces on the rods generate vibrations which contribute to premature wear of the bearings. Also, the phase difference between the oscillating motions of both hydrofoils is 180°. This means that they reach their zero-production points, at top and bottom positions, at the same time, which results in an undesirable fluctuating power output.
There is therefore a need to transmit energy from a fluid flow with increased efficiency. It would also be desirable to provide a transmission system or method which limits mechanical losses, improves robustness and resistance to wear, and evens out the output power curve.
An object of the present invention is to provide a turbine, a propulsive system, a method or a hydrofoil addressing at least one of the above-mentioned needs.
According to a first aspect of the invention, a turbine is provided. The turbine is for converting kinetic energy from a fluid flow into mechanical energy by driving a rotatable shaft.
The turbine comprises a support structure, first and second hydrofoils, a heaving-to-pitching assembly and a linear-to-rotary transmission system.
The first and second hydrofoils extend from the support structure, each hydrofoil being slidably and rotatably connected to the structure, to allow each of the hydrofoils to move linearly in a heaving motion and to oscillate about a spanwise axis in a pitching motion.
The heaving and pitching motions are quasi-sinusoidal, wherein for a given one of the hydrofoils, the heaving and pitching motions are out of phase by a pitch-heave motion phase, and wherein the respective heaving motions of the first and second hydrofoils are out of phase by an inter-hydrofoil phase.
The heaving-to-pitching assembly is for coupling the heaving motions of the first and second hydrofoils to the pitching motions of the second and first hydrofoils respectively, the pitch-heave motion phase being substantially equal to the inter-hydrofoil phase, the heaving motion of one of the hydrofoils thereby drives the pitching motion of the other hydrofoil.
The linear-to-rotary transmission system is operatively connected to the first and second hydrofoils and to the rotatable shaft. The heaving motions of the first and second hydrofoils therefore drive a rotational motion of the shaft.
According to another aspect of the invention, there is provided a method for converting kinetic energy from a fluid flow into mechanical energy. The method comprises the steps of:
According to yet another aspect of the invention, there is provided a propulsive system for transmitting mechanical energy from a rotatable driving shaft. The system comprises a support structure, first and second hydrofoils, a heaving-to-pitching assembly and a rotary-to-linear transmission system.
The first and second hydrofoils extend from the support structure, each hydrofoil being slidably and rotatably connected to the structure, to allow each of the hydrofoils to move linearly in a heaving motion, and to oscillate about a spanwise axis in a pitching motion. The heaving and pitching motions are quasi-sinusoidal, whereby for a given one of the hydrofoils, the heaving and pitching motions are out of phase by a pitch-heave motion phase, and the respective heaving motions of the first and second hydrofoils are out of phase by an inter-hydrofoil phase.
The heaving-to-pitching assembly is for coupling the heaving motions of the first and second hydrofoils to the pitching motions of the second and first hydrofoils respectively. The pitch-heave motion phase being substantially equal to the inter-hydrofoil phase, the heaving motion of one of the hydrofoils thereby drives the pitching motion of the other hydrofoil.
The rotary-to-linear transmission system is operatively connected to the rotatable shaft and to the first and second hydrofoils, the rotational motion of the driving shaft thereby driving the heaving and pitching motions of the hydrofoil.
Yet another aspect of the invention concerns a hydrofoil. The hydrofoil comprises a pair of foils extending in parallel, the foils being connected via rigid links.
Other features and advantages of the present invention will be better understood upon a reading of the preferred embodiments thereof with reference to the appended drawings.
In the following description, similar features in the drawings have been given similar reference numerals. In order to preserve clarity, certain elements may not be identified in some figures if they are already identified in a previous figure.
Referring to
The turbine 30 includes first and second hydrofoils 34a, 36a extending from a support structure, in this case a post 38, which is preferably in an upright vertical orientation. The hydrofoils 34a, 36b extend from one side of the post, and are substantially parallel to one another. Preferably, when the support structure 38 is a single post, another pair of first and second hydrofoils 34b, 36b extend on the opposite side of the post, such as to maximize the lifting surfaces of the turbine 30. Although shallower configurations are achieved when the post is in an upright or vertical orientation, the post may also be positioned in a horizontal orientation, the hydrofoils thus extending in a vertical orientation. The hydrofoils 34, 36 have an elongated and substantially planar body. Each of the hydrofoils 34, 36 also has an extending curved profile. They also have a symmetrical transversal cross-section.
Now referring to
Now turning to
This configuration of the hydrofoil also favours a modular fabrication, where the overall length of the hydrofoil can be adapted, that is, increased or decreased, according to specific applications, using the same basic components. This modular configuration can also facilitate transport of the hydrofoil.
As will be appreciated, a hydrofoil 34, 36 can be composed of a single lifting surface, or alternatively incorporates multiple lifting surfaces rigidly connected to each other.
The mechanism involved in the oscillating motion of the hydrofoils can be divided in two main parts, according to their respective tasks. The first task implies the coupling of a linearly-oscillating or heaving-oscillating motion into an alternating rotary motion or pitching-motion. This first task is achieved with a heaving-to-pitching assembly, in which pitch-heave couplings are used to obtain a 1 degree-of-freedom system. The second part relates to the coupling of a linearly-oscillating motion into a rotary motion. This second part is achieved with a linear-to-rotary transmission system, using a power transmission link between the cyclical heaving motions of the hydrofoils and a rotating shaft.
The Heaving-to-Pitching Assembly
Referring now to
As can be appreciated, for a given hydrofoil, its heaving and pitching motions are out of phase by a pitch-heave motion phase, which is equal to Pi/2, or 90 degrees which corresponds to T/4. It can also be observed that the heaving motion y1 of the first hydrofoil 34 is out of phase relative to the heaving motion y2 of the second hydrofoil 36, by an inter-hydrofoil phase. While the pitch-heave phase for a hydrofoil is typically Pi/2, the heaving-to-pitching assembly 48 sets the inter-foil phase between y1 and y2 to be also equal to Pi/2, making it possible to use the heaving motion of each foil to drive the pitching motion of its neighbour foil.
Back to
The first linear actuator 50 is connected to the first hydrofoil 34, and the second linear actuator 52 is connected to the second hydrofoil 36. When a hydrofoil 34, 36 moves linearly, in a heaving motion induced by water current for example, the corresponding linear actuator 50, 52 is driven by this heaving motion. In this case, the first and second linear actuators 50, 52 are hydraulic cylinders.
Similarly, the first rotary actuator 54 is connected to the first hydrofoil 34 and the second rotary actuator is connected to the second hydrofoil 36. The heaving-to-pitching coupling system 58, which preferably consists of hydraulic conduits, serves to couple the first linear actuator 50 to the second rotary actuator 56, and to couple the second linear actuator 52 to the first rotary actuator 54.
When the first hydrofoil 34 moves linearly under the flow of current, fluid is pushed outside the cylinder 50 through the conduits 58, the fluid in turn actuating the rotary actuator 56, thereby driving the pitching motion of the hydrofoil 36. The same relationship exists between the hydrofoil 36, the cylinder 52, and the rotary actuator 54. The hydraulic cylinders 50, 52 and rotary actuators 54, 56 are sized and configured such that the inter-foil phase is equal to the heaving-to-pitching phase, which is 90 degrees.
Preferably, as shown in
In order to lower the operating pressure of the hydraulic cylinders, it is possible to double the components of the heaving-to-pitching assembly. In this case, embodiments such as those shown in
Referring now to
Preferably, the heaving-to-pitching assembly comprises a pitch-controlling mechanism 74 for controlling the pitching amplitude of the corresponding hydrofoil. In the present case, this mechanism 74 consists of stoppers 64a, 64b and of relief valves 66a, 66b. The fluid volume of the actuator 56 is designed to be slightly less than the fluid volume displaced by the hydraulic cylinder 50. This results in an automatic referencing system which operates when necessary. The extra fluid ensures that the vane 68 reaches the stoppers 64a, 64b, such that the preset maximum pitching amplitude is reached. Once the vane 68 touches one of the stoppers 64a, 64b, pressure rises and the extra fluid, which is preferably eco-friendly, such as surrounding water that has been filtered, is ejected through the relief valves 66a, 66b.
Back to
Now turning to
The Linear-to-Rotary Transmission System
With reference to
As shown in either one of the embodiments of
As can be appreciated, both embodiments of the linear-to-rotary links 94 shown in
With reference to
Back to
This embodiment can be advantageous for applications where several turbines 30 are deployed together, such as in tidal farms, also called hydrokinetic turbine parks, where the linear-to-rotary transmission system of each turbine unit 30 connects to a same rotating shaft and electrical generator, with the relative motion phases between the turbines set in such a way as to further smoothes out the applied torque and rotation velocity.
Preferably, the hydraulic fluid used is low-pressure, around 150 psi, and consists of conditioned water or vegetable oil which limits energetic losses (minimal friction in hoses and minimal leaks in the ambient water) and ensures an environmentally friendly operation.
It should also be noted that the inter-foil phase of 90 degrees in a basic unit pair of hydrofoils implies a relative motion of each foil with its neighbouring foil. As a consequence, the hydraulic hoses interconnecting the hydraulic cylinders and the rotary actuators need to allow for this relative motion.
Advantageously, an inter-foil phase of 90 degrees allows avoiding that both hydrofoils 34, 36 reach their zero-production point, at top and bottom positions, at the same time, which effectively smoothes out the torque signal at the generator and makes the whole turbine self-starting at low water current velocity. Preferably, the heaving-to-pitching assembly and the linear-to-rotary transmission system 88 are compact enough so that most of the components fit inside the two side posts 38a, 38b forming the base structure. By doing so, most of the components are shielded from the flowing water, while the hydrofoils remain exposed.
With reference to
Referring to
Referring to
In this embodiment of the turbine 30, linear-to-rotary transmission links 94 are connected to the shaft 90 and the two transmission cylinders 126, 128 are each connected to the linear-to-rotary transmission links 94.
The first hydraulic cylinder 126 comprises a rod 130 and two pistons 134a, 134b located at both ends of the rod 130, each piston marking the boundaries of first and second chambers on both sides of the cylinder 126. The second hydraulic cylinder 128 has a similar configuration with rod 132, and pistons 136a, 136b. The rods 130, 132 are preferably articulated, to facilitate their alignment and displacement. Each rod 130, 132 is connected to a corresponding one of the hydrofoils 34, 36. For a given cylinder 126 or 128, the first chamber 138 is connected to its corresponding rotary actuator 56, 54 via the coupling means, and the second chamber 140 is connected to the transmission cylinders 96a, 96b. The rotatable shaft 90, moving in a constant rotational movement, can be coupled with any means 142 to an electric generator 144. In this preferred embodiment of the turbine 30, the hydraulic cylinders 126, 128 are part of both the heaving-to-pitching assembly and of the linear-to-rotary transmission system.
Referring to
Method for Converting Kinetic Energy from a Fluid Flow into Mechanical Energy
With reference to
Preferably, the method includes the sub-steps of providing a pair of first and second linear actuators, a pair of first and second rotary actuators and a heaving-to-pitching coupling system. The first linear actuator is connected to the first hydrofoil, and the second linear actuator to the second hydrofoil, each of the first and second linear actuators being driven by the heaving motion of the corresponding hydrofoil. The first rotary actuator must also be connected to the first hydrofoil, and the second actuator to the second hydrofoil, each of the first and second rotary actuators driving the corresponding hydrofoil in the pitching motion. Finally, the first linear actuator is coupled to the second rotary actuator, and the second linear actuator to the first rotary actuator, using the heaving-to-pitching coupling system.
Still preferably, the method comprises a sub-step of providing two spaced-apart posts, the first and second hydrofoils extending between the posts. The first and second hydrofoils each comprises a pair of foils extending in parallel between the posts.
Performances are also improved when the pitch-heave motion phase, and the inter-hydrofoil phase are approximately 90 degrees. Preferably, the method further includes a step of controlling the pitching amplitudes of the first and second hydrofoils.
The turbine described above offers an obvious advantage in shallow water sites due to its rectangular harvesting plane, allowing the possibility to scale up the rated power by simply increasing the turbine hydrofoil span. Furthermore, the untwisted rectangular hydrofoils in the oscillating concept have a much simpler geometry, and are easier to produce than typical rotor blades.
For tidal operation, in which the turbine should be able to operate with both ebb and flood tides, i.e. in both opposite directions, the system can be reversed by rotating the hydrofoils by 180 degrees. This can be performed by mounting each foil's rotary actuator on an additional 0-180° hydraulic actuator which can be fed on demand by the pump feeding the hydrostatic bearings. Alternatively, the foil pitching-center junction with its structural spar may incorporate a clutch coupling. In such an embodiment, the 180° rotation of the foil may be initiated passively from the action of the water flow. To complete the turbine reversal, a change of phase is also necessary.
This is preferably accomplished by inverting the rotational motion of the electrical generator through the electrical drive.
Oscillating foils can generate efficient propulsive forces when operating with the proper pitching angles. The embodiment presented above may be used for propulsion purposes in applications aiming to generate thrust from oscillating hydrofoils. In such cases, the electrical generator would operate as a motor and work would be performed by the foils on the fluid, rather than energy being extracted from the fluid flow.
Numerous modifications could be made to the embodiments above without departing from the scope of the present invention.
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/CA2011/001107 | 9/30/2011 | WO | 00 | 3/29/2013 |
Number | Date | Country | |
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61388892 | Oct 2010 | US |