WO2013170497A1 - Multi-airfoil collecting blade capable of utilizing wind power efficiently - Google Patents

Multi-airfoil collecting blade capable of utilizing wind power efficiently Download PDF

Info

Publication number
WO2013170497A1
WO2013170497A1 PCT/CN2012/076024 CN2012076024W WO2013170497A1 WO 2013170497 A1 WO2013170497 A1 WO 2013170497A1 CN 2012076024 W CN2012076024 W CN 2012076024W WO 2013170497 A1 WO2013170497 A1 WO 2013170497A1
Authority
WO
WIPO (PCT)
Prior art keywords
wing
blade
collecting
wings
domain
Prior art date
Application number
PCT/CN2012/076024
Other languages
French (fr)
Chinese (zh)
Inventor
李锋
Original Assignee
甘肃科惠特资源综合开发有限公司
苏州飞能可再生能源科技有限公司
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by 甘肃科惠特资源综合开发有限公司, 苏州飞能可再生能源科技有限公司 filed Critical 甘肃科惠特资源综合开发有限公司
Publication of WO2013170497A1 publication Critical patent/WO2013170497A1/en

Links

Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F03MACHINES OR ENGINES FOR LIQUIDS; WIND, SPRING, OR WEIGHT MOTORS; PRODUCING MECHANICAL POWER OR A REACTIVE PROPULSIVE THRUST, NOT OTHERWISE PROVIDED FOR
    • F03DWIND MOTORS
    • F03D1/00Wind motors with rotation axis substantially parallel to the air flow entering the rotor 
    • F03D1/06Rotors
    • F03D1/0608Rotors characterised by their aerodynamic shape
    • F03D1/0633Rotors characterised by their aerodynamic shape of the blades
    • F03D1/0641Rotors characterised by their aerodynamic shape of the blades of the section profile of the blades, i.e. aerofoil profile
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/70Wind energy
    • Y02E10/72Wind turbines with rotation axis in wind direction

Definitions

  • the present invention relates to the technical field of wind turbines (also known as windmills or wind turbines), and in particular to a wind turbine blade capable of efficiently utilizing wind energy.
  • the wind energy utilization coefficient of a blade (expressed as Cp, also known as wind energy utilization efficiency) is a manifestation of blade performance.
  • the Cp of the blade is related to the lift generated by the air flowing through the blade airfoil, and the lift generated by the airfoil is streamlined by the structural airfoil.
  • the shape is determined so that the Cp properties of the blade are determined by the shape of the airfoil formed. Increasing the Cp of the blade is the most fundamental technology in the development of high performance wind power technology.
  • the blades of existing wind power products are single-winged, and the airfoil of the airfoil is NACA series for aircraft, SERI series for wind wheel blades, NREL series, RIS O_A series, G0E series and FFA-W series.
  • the single-wing blades composed of these airfoils cannot improve the wind energy utilization efficiency because they have no current collecting effect, which is one of the reasons for the poor performance of the single-wing blades in the middle and low wind speed range.
  • Aerofoil refers to a two-dimensional shape consisting of a streamlined curve that conforms to certain aerodynamic properties. For example, each vertical section along the span of the wing is referred to as an airfoil. There are types and sizes of airfoils. For example, the NACA4412 and NACA0015 are two airfoils and two airfoils. The two different chord lengths of the NACA4412 are two airfoils, but one airfoil.
  • An airfoil is a three-dimensional shape consisting of a streamlined surface that conforms to certain aerodynamic properties.
  • a three-dimensional body formed by an envelope surface of a wing and an airfoil.
  • the fins formed by one airfoil are of equal width, and the fins formed by one airfoil are of equal width.
  • Blade refers to the basic unit of wind turbines that absorbs wind energy. Several of the units are evenly distributed on the circumference of the hub.
  • the blade referred to in the present invention refers to a blade composed of at least two fins, which is still a basic unit for wind turbines to absorb wind energy.
  • the fins are reflected as airfoils, so the fins described in three dimensions should be described as airfoils in a two-dimensional space.
  • the fins and the airfoil are referred to as wings, in the three-dimensional space, the fins, and in the two-dimensional space.
  • Azimuth refers to the relative direction and position between adjacent wings.
  • a domain is an abbreviation for a fluid flow space formed between adjacent wings.
  • the representation method of the multi-wing collecting blade of the invention :
  • the letter G represents the multi-wing collecting blade
  • the number n (n 2) represents the number of wings
  • the letter f represents The domain between the two wings
  • ni represents the i-th wing of the n wings
  • fij represents the domain between the i-th wing and the j-th wing.
  • G3 represents a three-wing collecting blade composed of a wing 31, a domain 2, a wing 32, a domain f23 and a wing 33
  • Gn represents a wing n1, a domain f 12, a wing n2, a wing ni, a domain fij, a wing nj, ..., multi-wing collecting blades composed of wing n (nl), domain f (n_l) n and wing nn.
  • a multi-wing collecting blade for efficiently utilizing wind energy comprising a domain formed between at least two wings and at least one adjacent wing, by arranging the shape of each of said wings and said domain to make adjacent The wing produces a current collecting effect on the fluid flowing through the domain therebetween, the domain being the space formed between the rear concave surface of the front adjacent wing and the front convex surface of the adjacent adjacent wing, and the adjacent wing
  • the rear concave surface, the front convex surface is oriented upwardly; the relative orientation between the adjacent wings is set to enhance the current collecting effect, and the kinetic energy of the fluid flowing through the domain is increased to increase the phase behind the domain
  • the lift of the adjacent wing thereby increasing the wind energy utilization factor of the overall multi-blade blade comprised of the wing and the domain.
  • the wing ni will flow through the fluid of the domain fij to the tangential direction of the upper surface of the wing nj, providing greater fluid kinetic energy to the boundary layer of the upper
  • the shape of the domain fi j is designed to And the relative orientation between the collecting wing C and the wing ml, the relative orientation between the wing mi and the wing mj, the domain fij being the rear concave surface of the wing mi and the front convex surface of the wing mj a space formed therebetween, and the rear concave surface and the front convex surface are oriented in an upwardly forward direction, so that the collecting wing C flows the fluid passing through the collecting basin F to the tangential direction of the upper surface of the wing
  • the shape of a certain type of single wing A is used as the outer contour of the multi-blade blade Gn or Gndm, and the effect is to reduce the resistance of the blade Gn.
  • the outer contour of the sub-blade Dm in the multi-blade blade Gndm is formed in the shape of a certain one-wing B, and the effect is to reduce the resistance of the sub-blade Dm (m 2).
  • the above-mentioned multi-wing collecting blade with high efficiency utilizing wind energy fully utilizes the Bernoul li effect effect, and the design is more reasonable, and the blade can generate a collecting effect on the fluid flowing through the domain, thereby improving The wind energy utilization coefficient Cp of the multi-blade blade.
  • Figures la, lb, and lc are schematic views of a configuration of the two-wing, three-wing, and four-wing collecting blades G2, G3, and G4 of the present invention, respectively.
  • 2a, 2b, 2c, and 2d are schematic views showing a configuration of the two-wing, three-wing, four-wing, and five-wing collecting blades G2dl, G3d2, G4d3, and G5d4 of the present invention, respectively.
  • Fig. 3 is a schematic view showing the configuration of the multi-wing collecting blade Gn of the present invention.
  • Fig. 4 is a schematic view showing the configuration of the multi-wing collecting blade Gndm of the present invention.
  • Figures 5a, 5b, and 5c are schematic views of a configuration of the outer contours of the collecting blades G2, G3 and G4 of the present invention by a certain wing A, respectively.
  • Fig. 6a is a schematic view showing a configuration of the blade G2dl of the present invention, wherein the sub-blades D1 are single-wing sub-blades.
  • Fig. 6b, Fig. 6c, and Fig. 6d are respectively schematic views showing one of the collecting blades G3d2, G4d3 and G5d4 of the outer contour of the sub-blades D2, D3 and D4 of the sub-blade D1 of Fig. 6a.
  • Fig. 7 is an enlarged view of 1 in Fig. 6a, which is a schematic view showing the orientation of the collecting vane G2dl of the present invention with respect to the wing 11 (i.e., the sub-blade D1).
  • Figure 8 is an enlarged view of ⁇ 2 in Figures 5a and 6b, showing a schematic view of the orientation of the sub-blade D2 modulating wings 21 relative to the wings 22 of the collecting blade G2 and the blade G3d2 of the present invention.
  • Figure 9 is an enlarged view of ⁇ 3 in Figures 5b and 6c, showing a schematic view of the orientation of the sub-blade D3 modulating wings 32 relative to the wings 33 of the blade G3 and the blade G4d3 of the present invention.
  • Figure 10 is an enlarged view of ⁇ 4 in Figures 5c and 6d, which is a schematic illustration of the orientation of the blade G4 and the blade G5d4 of the present invention in which the sub-blade D4 modulates the wing 43 relative to the wing 44.
  • Fig. l la and Fig. 1 ib are respectively a schematic diagram of the position of the blade Gndm modulation collecting wing C of the present invention relative to the wing ml of the sub-blade Dm and the orientation of the modulation wing mi relative to the wing mj.
  • Figure 12 is a schematic illustration of the orientation of the blade Gn modulation wing ni relative to the wing nj of the present invention.
  • Figure 13 is a schematic view showing a configuration of a single-wing blade formed by the sub-blades D1 of the blade G2dl of the present invention.
  • Fig. 14a and Fig. 14b are schematic views showing a configuration of the outer contour of the blade G4d3 neutron blade D3 and the outer contour of the blade G4d3 constructed by a certain wing A by the wing B of the present invention.
  • Fig. 14c is an enlarged view of ⁇ in Fig. 14b as an example, showing a schematic diagram of constructing a blade G4d3 in the shape of a certain wing A.
  • Figures 14d, 14e, and 14f are schematic views of a stepwise construction blade G4d3.
  • Fig. 15 is a view showing changes in Cp of the blades G2dl, G3d2, G4d3 and D1 according to the present invention as a function of the angle ⁇ .
  • FIG 16 is a flow diagram showing the computational fluid dynamics (CFD) of the blade G2dl of the present invention.
  • Figure 17 is a schematic illustration of a three-dimensional blade formed by the blade G2dl of the present invention.
  • Figure 18 is a schematic illustration of another three-dimensional blade formed by the blade G2dl of the present invention.
  • Figure 19 is a schematic illustration of a three-dimensional blade formed by the blade G3 of the present invention.
  • Figure 20 is a schematic illustration of a three-dimensional blade formed by the blade G4 of the present invention.
  • Figures 21a and 21b are schematic views of two three-dimensional spiral type blades formed by the blade G2dl of the present invention.
  • Figures 22a and 22b are schematic views of two three-dimensional ⁇ -type blades formed by the blade G2dl of the present invention.
  • the present invention provides a multi-wing collecting blade for efficient use of wind energy, comprising a domain formed between at least two wings and at least one adjacent wing, by designing the shape of each of said wings and said domain, Enabling adjacent wings to create a current collecting effect on fluid flowing through the domains therebetween, and enhancing the current collecting effect by increasing the relative orientation between the adjacent wings
  • the kinetic energy of the fluid of the domain increases the lift of the wing behind the domain, thereby increasing the wind energy utilization coefficient Cp of the multi-wing blade as a whole; the construction points of the multi-wing collecting blade described above, one is designed
  • the criterion is that each of the wings and the domain formed by the configuration must be such that the fluid flowing through the domain flows in a tangential direction to the upper surface of the adjacent wing behind the domain, such that the shape of the domain must be a space between the rear concave surface of the front adjacent wing and the front convex surface of the rear adjacent wing, and a common feature of both the
  • the shape of the wing is composed of a streamlined curve, and the streamlined curve does not have a corresponding mathematical function analytical expression describing the law of variation of the parameter, which can only be described by the numerical value of the coordinate point, due to the wing and the
  • the mutual matching between the shapes of the domain is relative, so the shape of the wing and the domain conforming to the design criterion structure is not unique, and the description method of the coordinate point value cannot summarize the construction result of the design technique of the present invention. The whole picture.
  • the above two criteria for the design goal are the key techniques for constructing the multi-wing collecting blade, under the guidance of the two criteria, design
  • the steps are construction ⁇ forming ⁇ detection ⁇ analysis ⁇ reconstruction ⁇ reshaping ⁇ in detection ⁇ reanalysis ⁇ ... ⁇ until the wind energy utilization coefficient Cp is constructed to the average value of the corner ⁇ is the maximum value ⁇ Cp> ma X corresponding shape ⁇ 25. 25 ⁇ 0. 25 ⁇
  • the present invention has a configuration of the multi-wing collector blade, at a wind speed of 10 m / sec, more than a dozen multi-wing collecting blade ⁇ Cp> ma X reaches 0. 20 ⁇ 0. 25
  • the maximum value Cpmax reaches 0. 35 ⁇ 0. 40, but the shape of the wing and the domain to which they belong and the relative orientation between the adjacent wings are different.
  • the blade Gn of the present invention has a relatively high Cp performance and a function of controlling power, and thus accommodates a wider range of wind speeds.
  • the tangential direction provides more fluid kinetic energy to the boundary layer of the upper surface of the wing mj to reduce the laminar flow separation and increase the lift of the wing mj, thereby increasing the Cp of the blade Gndm;
  • the orientation of the wing ml and the orientation of the wing mi relative to the wing mj can control the lift values of the wings ml and mj, and thus the power of the blade Gndm can be controlled.
  • a method for designing the multi-wing collecting blade is such that the shape of a certain single wing A is the outer contour of the multi-wing collecting blade, and at least two are connected between the upper and lower surfaces of the single wing A.
  • the strip streamline curve forms at least one slit-shaped space, the convex surfaces of the two streamlined curves are oriented in the upwardly forward direction, and the joint between the two streamlined curves and the upper and lower surfaces of the single wing A is smooth Excessive streamlined configuration, and then removing the portion of the single wing A between the two streamlined curves formed after the fluent structure, the slit space thus formed is the shape of the domain, and the two sides of the domain are retained
  • the portion of the single wing A forms a shape formed by at least two closed streamline curves, each closed streamline curve shape being each of the wings formed by the design; in the design, the criterion for determining the shape is each of the configurations
  • the shape of the wing and the domain enables fluid flowing through the domain to flow in
  • the wings are n, in turn by the wing nl, the domain fl2, the wing n2, the wing ni, the domain fij, the wing nj,
  • n_l constitutes a blade Gn
  • the shape of a certain single wing A is the outer contour of the blade Gn, on the single wing A, a streamlined curve connecting the 2 (n-1) strips with the convex surface toward the upper front direction to form n-1 slit-shaped spaces, and two streamline curves forming each of the slit-shaped spaces and the
  • n_l n parts of the single-wing A remaining on both sides of the domain fij form n
  • the shape of a certain single wing A is the outer contour of the blade Gndm
  • the shape of a certain single wing B is the outer contour of the sub-blade Dm in the blade Gndm
  • the current is constructed.
  • FIGS. 1a, 1b, and 1c which respectively include two wings 21, 22, three wings 31, 32, 33 and four wings 41, 42, 43, 44, the fields between adjacent wings are fl2, fl2, f23 and fl2, f23, f34, the shape design of each wing, the streamline matching between the wings and the relative orientation, must be convective Fluid passing through the domains between adjacent wings creates a current collecting effect that increases the kinetic energy of the fluid flowing through the domain to increase the lift of the wings behind the field, thereby increasing the wind energy utilization factor of the overall blade.
  • the wing C of the head has special characteristics, whether it is a few wing collecting blades, the head
  • the wing C shape features are the same, only the current collecting function, the lift of its own can not be improved.
  • the remaining wings act as the power wing characters of the blades, they and
  • the domains between the adjacent wings form sub-blades D2, D3 and D4 having the same characteristics as the corresponding blades in Fig. 1, and also include the case where the sub-blades are one wing D1.
  • the domain between the collecting wing C and the sub-blades D1, D2, D3, D4 is named the collecting basin F.
  • the sub-blade D is changed to d here to emphasize that such a blade is still one of the multi-wing collecting blades of the present invention.
  • the collecting wings C in the blades only serve as a current collecting, which gives the power blades a sub-blade Dm with a larger chord space.
  • FIG. 3 and 4 are schematic views of the blade Gn and the blade Gndm of the present invention, respectively, wherein the dotted line shape represents the contour formed by the domain components between the wings and the wing represented by "", and does not represent the shape of a certain wing.
  • the blade Gn consists of the wing nl, the domain fl2, the wing n2, the wing ni, the domain fij, the wing nj, the wing n (n-1), the domain f(n_l) n and the wing nn constitute "and" the blade Gndm is set by
  • the outer contour of the blade shown in Figure 5 is constructed in a certain wing A shape
  • Figure 6 The outer contour of the sub-blades in the blade is constructed according to a certain wing B shape.
  • the airfoil of the sub-blade D1 is an option of the wing B, wherein some wing A.
  • Some kind of wing B can be some existing airfoil, or it can be some kind of airfoil with better performance in the future.
  • the configuration of the blades shown in Figures 1 and 2 does not require such an outer profile, and the resistance is relatively greater than that of the outer profile winged configuration.
  • FIG. 7 sequentially show enlarged views of the ⁇ 1, ⁇ 2, ⁇ 3, and ⁇ 4 portions of the blade shown in Figs. 5 and 6, respectively.
  • the blade G2dl shown in Fig. 6 is composed of the collecting wing C and the wing 11 (i.e., the sub-blade D1).
  • the position of the collecting wing C relative to the wing 11 is adjusted (shown by a broken line in Fig.
  • the flow rate which in turn changes the kinetic energy and flow direction of the fluid flowing to the upper surface of the wing 22, causes laminar flow separation of the upper surface of the wing 22 and changes in the lift value of the wing 22, thereby modulating the Cp of G2 and G3d2 for the purpose of controlling power.
  • the orientation of the modulation wing 32 relative to the wing 33 changes the flux and flow rate of the fluid flowing through the field f23, and The kinetic energy and flow direction of the fluid flowing to the upper surface of the wing 33 are changed, so that the laminar flow separation of the upper surface of the wing 33 and the lift value of the wing 33 are changed, so that the Cp of G3 and G4d3 can be modulated to achieve the purpose of controlling the power.
  • the orientation of the current collecting wing C relative to the wing 21, the wing 31, the wing 41, the orientation of the modulation wing 31 relative to the wing 32, the orientation of the modulation wing 41 relative to the wing 42 and the modulation wing 42 are relative.
  • the above-mentioned mechanism for acting on the wing 11, the wing 22, the wing 33 and the wing 44 can also achieve the purpose of controlling power.
  • FIG. 1a, 1b and 12 respectively show a schematic view of the general orientation of the modulation of the blade Gndm and the blade Gn, the change of the orientation of the modulation collecting wing C with respect to the wing ml is indicated by the dashed line in Fig. 11a
  • the change in the orientation of the modulation wing mi relative to the wing mj is indicated by the dashed line in FIG. 1 ib
  • the change in the orientation of the modulation wing ni relative to the wing nj is indicated by the dashed line in FIG.
  • Shown in Figure 13 is a single wing blade Dl for comparison.
  • the outer contours of both the sub-blades D3 and the blades G4d3 shown in Figs. 14a and 14b are respectively configured in a certain wing B shape and in a certain wing A shape.
  • the streamlined curve from the convex surface indicated by the broken line toward the upper front direction forms three slit-shaped spaces indicated by the hatched areas of the horizontal line, and the streamlined curves on both sides of each of the horizontally shaded areas formed are formed on the wing A
  • the joint portion of the lower surface is fluently streamlined, and the portion indicated by the hatched area is formed, and the three spaces formed by the portions of the wing A in the shaded area and the hatched area are removed.
  • the shape of the watershed F, the domain f 12 and the domain f23 of the sub-blade D3 shown in Fig. 14b is in turn, and the remaining portions of the wing A are in turn the set shown in Fig. 14b.
  • the shape of the flow wing (:, the wing 31 of the sub-blade D3, the wing 32, and the wing 33.
  • the point of the shape configuration of the above-mentioned horizontally shaded area is to determine the flow direction of the fluid in the formation domain to conform to the configuration, the shaded area is
  • the structure is formed a plurality of times, that is, the lower surface of the collecting wing C, the front convex surface of the wing 31, and the rear
  • the concave surface, the front convex surface and the rear concave surface of the wing 32, and the front convex surface of the wing 33 are formed in a plurality of configurations, and the finally formed collecting wing C, the wing 31 of the sub-blade D3 and the wing 32 will pass through the collecting basin F
  • the fluid flow flowing in the domains f 12 and F23 of the sub-blades D3 flows toward the tangential direction of the upper surfaces of the wings 31, the wings 32 and the wings 33, and the watershed F, the domain 2 and the domain f23 of the sub-blades D3 are narrow or narrow or
  • the relative orientation between their adjacent wings is a significant
  • FIG. 14d A design method for respectively constructing the wing and the domain to which the blade G4d3 belongs is shown in Fig. 14d, Fig. 14e, and Fig. 14f, and the first step shown in Fig. 14d is to use the single wing A as the outer contour to construct a corresponding ⁇ Cp>ma X
  • the second step shown in Fig. 14e is to determine the sub-blade D1' as the outer contour (similar to the wing B of Fig.
  • the wing 2 and the domain 2 determined in the second step cooperate to construct a blade G4d3 corresponding to ⁇ [>111£ ⁇ , and the wing 2 is the determined wing 31.
  • the advantage of this step-by-step construction of the wing and domain approach is that it facilitates the analysis of the relationship between shape and orientation and performance.
  • the two-wing, three- and four-wing collecting blades G2d1, G3d2 and G4d3 shown in Fig. 6 and the single-winged blade D1 shown in Fig. 13 are used as an embodiment, and a large number of Computational fluid dynamics simulation and experiment, the results show that the Cp of the multi-wing collecting blade has a significant improvement compared with the chord-long single-wing blade D1, especially in the middle and low wind speed range.
  • the Cp of the blades D1, G2dl, G3d2, and G4d3 is sequentially increased, and the maximum value of Cp is increased toward the direction of the large corner angle with the number of blade-forming wings.
  • Fig. 15 the two-wing, three- and four-wing collecting blades G2d1, G3d2 and G4d3 shown in Fig. 6 and the single-winged blade D1 shown in Fig. 13 are used as an embodiment, and a large number of Computational fluid dynamics simulation and experiment, the results show that the Cp of the multi
  • the streamline density in the collection basin F is increased, the color is brighter (indicating that the flow velocity is faster) and continues to a length of the upper surface of the downstream wing; this phenomenon embodies that the collector wing C will collect the basin F
  • the kinetic energy of the inner fluid is increased and directed to the tangential direction of the upper surface of the downstream wing.
  • the blade of the present invention is named as a multi-wing collecting blade.
  • FIG. 17, 18, 21a, 21b and 22a, 22b are schematic views of three-dimensional vanes of the blade G2dl of the present invention
  • Figs. 19 and 20 are schematic views of three-dimensional vanes of the vane G3 and the vane G4 of the present invention, respectively.
  • the blades shown in Figures 17, 19 and 20 can be applied as blades of vertical shaft (also known as vertical axis) wind turbines in the form of "H", "Y”, " ⁇ " and “ ⁇ ”shapes;
  • the concave surface of the blade shown in Fig. 21a faces outward, and the concave surface of the blade shown in Fig.
  • FIG. 21b faces inward, they can be applied as A blade of a vertical axis wind turbine like a spiral pattern;
  • the concave surface of the blade shown in Fig. 22a faces inward, and the concave surface of the blade shown in Fig. 22b faces outward, they can be applied as blades of a vertical axis wind turbine like a " ⁇ "shape;
  • Fig. 18 The blade shown can be applied as a blade for a horizontal axis wind turbine.
  • the value range of n or m is preferably 2 n 30, l ⁇ m ⁇ 29, in principle, in the range of 16 n 30, 15 m 29
  • the blade of the present invention is more suitable for the blade of the high-power wind turbine; in the range of 6 n 15 , 5 ⁇ m ⁇ l4 , the blade of the invention is more suitable for the blade of the large medium-power wind turbine; In the range of 10, 3 m 9 , the blade of the present invention is suitable for the blade of the medium power wind turbine; when in the range of 2 n 5 , l ⁇ m ⁇ 4, the blade of the invention is suitable for low power and below Blades of power wind turbines. This also embodies the cost-effective selectivity advantages of the inventive blade.

Abstract

A multi-airfoil collecting blade capable of utilizing wind power efficiently comprises at least two airfoils and at least one zone formed between the adjacent airfoils. By designing the shape of each airfoil and zone, the adjacent airfoils are enabled to generate a collecting effect on the fluid flowing through the zone between the adjacent airfoils. The zone is a space formed between a rear concave surface of an adjacent air foil in front of the zone and a front convex surface of an adjacent airfoil behind the zone, and the rear concave surface and the front convex surface of the adjacent airfoils are upward and front-biased. The relative orientation of the adjacent airfoils is arranged to enhance the collecting effect, so that the kinetic energy of the fluid flowing through the zone is increased and hence the lifting force of the adjacent airfoil behind the zone is increased, thereby improving the rotor power coefficient of the whole multi-airfoil collecting blade formed by the airfoils and zones.

Description

一种高效利用风能的多翼集流叶片 技术领域 本发明属于风力机 (亦称风车或风机)技术领域, 具体涉及一种能够高效利用 风能的风力机叶片。  BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to the technical field of wind turbines (also known as windmills or wind turbines), and in particular to a wind turbine blade capable of efficiently utilizing wind energy.
背景技术 叶片的风能利用系数 (表示为 Cp, 又称风能利用效率)是叶片性能的体现, 叶 片的 Cp 与空气流过叶片翼型产生的升力有关, 而翼型产生的升力由构造翼型流线型的形 状确定, 因此叶片的 Cp性能由其构成的翼型形状确定。 提高叶片的 Cp是研发高性能风电 技术中最根本的技术。 现有的风力发电产品的叶片均是单翼片, 翼片的翼型有飞机用的 NACA系列, 风轮叶片专用的 SERI系列、 NREL系列、 RIS O_A系列、 G0E系列和 FFA-W系 列等。 由这些翼型构成的单翼叶片由于自身没有集流效应, 不能提高风能利用效率, 这也 是造成单翼叶片在中低风速范围性能欠佳的原因之一。 BACKGROUND OF THE INVENTION The wind energy utilization coefficient of a blade (expressed as Cp, also known as wind energy utilization efficiency) is a manifestation of blade performance. The Cp of the blade is related to the lift generated by the air flowing through the blade airfoil, and the lift generated by the airfoil is streamlined by the structural airfoil. The shape is determined so that the Cp properties of the blade are determined by the shape of the airfoil formed. Increasing the Cp of the blade is the most fundamental technology in the development of high performance wind power technology. The blades of existing wind power products are single-winged, and the airfoil of the airfoil is NACA series for aircraft, SERI series for wind wheel blades, NREL series, RIS O_A series, G0E series and FFA-W series. The single-wing blades composed of these airfoils cannot improve the wind energy utilization efficiency because they have no current collecting effect, which is one of the reasons for the poor performance of the single-wing blades in the middle and low wind speed range.
发明内容 本发明的目的在于提供一种与单翼叶片相比具有相对高 Cp的多翼集流叶片。 SUMMARY OF THE INVENTION It is an object of the present invention to provide a multi-wing collecting blade having a relatively high Cp compared to a single wing blade.
本发明描述中使用的相关术语释义:  Interpretation of related terms used in the description of the present invention:
翼型 (aerofoil)是指由符合某种空气动力学特性的流线型曲线构成的二维形状。 例 如,沿机翼之展向的每一个垂向切面都被称为翼型。翼型有种类和大小之分,例如 NACA4412 和 NACA0015是两个翼型、 也是两种翼型, 两个不同弦长的 NACA4412是两个翼型、 但是一 种翼型。  Aerofoil refers to a two-dimensional shape consisting of a streamlined curve that conforms to certain aerodynamic properties. For example, each vertical section along the span of the wing is referred to as an airfoil. There are types and sizes of airfoils. For example, the NACA4412 and NACA0015 are two airfoils and two airfoils. The two different chord lengths of the NACA4412 are two airfoils, but one airfoil.
翼片 (airfoil)是指由符合某种空气动力学特性的流线型曲面构成的三维形状。 例如, 机翼、 翼型在空间排布的包络面形成的三维体。 由一个翼型形成的翼片是等宽的、 一种翼 型形成的翼片不定是等宽的。  An airfoil is a three-dimensional shape consisting of a streamlined surface that conforms to certain aerodynamic properties. For example, a three-dimensional body formed by an envelope surface of a wing and an airfoil. The fins formed by one airfoil are of equal width, and the fins formed by one airfoil are of equal width.
叶片 (blade)是指风力机吸收风能的基本单元, 若干该单元均匀分布在轮毂的圆周上。 本发明中所述的叶片是指由至少两个翼片构成的叶片, 它仍然是风力机吸收风能的基本单 元。  Blade refers to the basic unit of wind turbines that absorbs wind energy. Several of the units are evenly distributed on the circumference of the hub. The blade referred to in the present invention refers to a blade composed of at least two fins, which is still a basic unit for wind turbines to absorb wind energy.
在二维空间里, 翼片映现为翼型, 因此在三维空间里描述的翼片, 在二维空间里就应 该描述为翼型。 为避开描述上的羁绊, 翼片和翼型均简称翼, 在三维空间里指翼片、 在二 维空间里指翼型。  In a two-dimensional space, the fins are reflected as airfoils, so the fins described in three dimensions should be described as airfoils in a two-dimensional space. In order to avoid the flaws in the description, the fins and the airfoil are referred to as wings, in the three-dimensional space, the fins, and in the two-dimensional space.
方位是指相邻翼之间的相对方向与位置。  Azimuth refers to the relative direction and position between adjacent wings.
域是相邻翼之间形成的流体流动空间的简称。 本发明多翼集流叶片的表示方法: A domain is an abbreviation for a fluid flow space formed between adjacent wings. The representation method of the multi-wing collecting blade of the invention:
字母 G代表多翼集流叶片、 数字 n (n 2)代表翼的数目、 数字 i (i=l,2,……,n)代表 头部起始的第 i个翼的编号、 字母 f代表两个翼之间的域, ni代表 n个翼中的第 i个翼、 fij代表第 i个翼与第 j个翼之间的域。 例如, G3代表由翼 31、 域 2、 翼 32、 域 f23 和翼 33构成的三翼集流叶片, Gn代表由翼 nl、 域 f 12、 翼 n2、 、 翼 ni、 域 fij、 翼 nj、 ……、 翼 n (n-l)、 域 f (n_l) n和翼 nn构成的多翼集流叶片。  The letter G represents the multi-wing collecting blade, the number n (n 2) represents the number of wings, the number i (i = l, 2, ..., n) represents the number of the i-th wing starting from the head, and the letter f represents The domain between the two wings, ni represents the i-th wing of the n wings, and fij represents the domain between the i-th wing and the j-th wing. For example, G3 represents a three-wing collecting blade composed of a wing 31, a domain 2, a wing 32, a domain f23 and a wing 33, and Gn represents a wing n1, a domain f 12, a wing n2, a wing ni, a domain fij, a wing nj, ..., multi-wing collecting blades composed of wing n (nl), domain f (n_l) n and wing nn.
本发明的目的可以通过采取以下技术方案来实现:  The object of the present invention can be achieved by adopting the following technical solutions:
一种高效利用风能的多翼集流叶片, 它包括至少两个翼和至少一个相邻翼之间形成的 域, 通过对每个所述翼和所述域的形状设计, 使相邻的所述翼对流过其间所述域的流体产 生一种集流效应, 所述域是其前面相邻翼的后凹面与后面相邻翼的前凸面之间形成的空 间, 并且所述的相邻翼后凹面、 前凸面是朝向上偏前方向; 通过设置所述相邻翼之间的相 对方位以增强所述集流效应, 增大流过所述域的流体的动能而提高所述域后面相邻翼的升 力, 从而提高由所述翼和所述域组成的整体多翼叶片的风能利用系数。  A multi-wing collecting blade for efficiently utilizing wind energy, comprising a domain formed between at least two wings and at least one adjacent wing, by arranging the shape of each of said wings and said domain to make adjacent The wing produces a current collecting effect on the fluid flowing through the domain therebetween, the domain being the space formed between the rear concave surface of the front adjacent wing and the front convex surface of the adjacent adjacent wing, and the adjacent wing The rear concave surface, the front convex surface is oriented upwardly; the relative orientation between the adjacent wings is set to enhance the current collecting effect, and the kinetic energy of the fluid flowing through the domain is increased to increase the phase behind the domain The lift of the adjacent wing thereby increasing the wind energy utilization factor of the overall multi-blade blade comprised of the wing and the domain.
所述的翼为 n个, 由 n个翼 ni (n 2、 i=l, 2, , n)和 n_l个由翼 ni与翼 nj之间的 域 fij (j=i+l n、 i=l, 2, , n_l)构成多翼叶片 Gn, 通过所述 n个翼 ni和所述 n_l个 翼 ni与翼 nj之间的所述域 fi j的形状设计、 以及所述 n-1个翼 ni与翼 nj之间相对方位 的设置,所述域 fij是翼 ni的后凹面与翼 nj的前凸面之间形成的空间,并且所述后凹面、 前凸面是朝向上偏前方向; 使所述翼 ni将通过所述域 fij的流体聚集流向所述翼 nj上表 面的切线方向, 给所述翼 nj 上表面的边界层提供更大的流体动能, 来减小层流分离而使 所述翼 nj的升力增大, 从而提高了所述多翼叶片 Gn的风能利用系数 Cp; 通过调制所述翼 ni与所述翼 nj之间的相对方位, 控制所述翼 nj的升力值, 进而控制所述多翼叶片 Gn的 功率。  The wing is n, consisting of n wings ni (n 2, i=l, 2, , n) and n_l by the domain fij between the wing ni and the wing nj (j=i+ln, i=l , 2, , n_l) constitute a multi-blade blade Gn, the shape design of the domain fi j between the n wings ni and the n-1 wings ni and the wing nj, and the n-1 wings ni a setting of a relative orientation with the wing nj, the field fij being a space formed between the rear concave surface of the wing ni and the front convex surface of the wing nj, and the rear concave surface and the front convex surface are oriented upwardly forward; The wing ni will flow through the fluid of the domain fij to the tangential direction of the upper surface of the wing nj, providing greater fluid kinetic energy to the boundary layer of the upper surface of the wing nj to reduce laminar flow separation and make the wing The lift of nj is increased, thereby increasing the wind energy utilization coefficient Cp of the multi-blade blade Gn; by modulating the relative orientation between the wing ni and the wing nj, controlling the lift value of the wing nj, thereby controlling the The power of the multi-blade blade Gn.
所述的翼为 n个, 排头的翼 nl界定为集流翼 C, 其余的翼 ni (i=2,……,n)构成子叶 片 Dm (m=n-1), 集流域 F是集流翼 C与子叶片 Dm之间的域, 它由集流翼 C的下表面和子叶 片 Dm前缘上部之间的空间形成, 由集流翼(:、 集流域 F和子叶片 Dm (m=n_l)构成多翼叶片 The wings are n, the wing n1 of the head is defined as the collecting wing C, and the remaining wings ni (i=2, . . . , n) constitute the sub-blade Dm (m=n-1), and the collecting basin F is a set. The domain between the flow wing C and the sub-blade Dm, which is formed by the space between the lower surface of the collecting wing C and the upper portion of the leading edge of the sub-blade Dm, by the collecting wing (:, the collecting basin F and the sub-blade Dm (m=n_l ) constitute a multi-blade blade
Gndm, 其中所述子叶片 Dm由 m个翼 mi (m=n_l ^ l、 i=l, 2, , m)和 m_l个翼 mi与翼 mj 之间的域 fij (j=i+l m、 i=l,2,……,m_l)构成, 通过所述集流翼 C形状设计、 m个所述 翼 mi形状设计和所述集流域 F和 m-1个翼 mi与翼 mj之间的所述域 fi j的形状设计, 以 及所述集流翼 C与翼 ml之间的相对方位、翼 mi与翼 mj之间的相对方位设置, 所述域 fi j 是所述翼 mi的后凹面与所述翼 mj的前凸面之间形成的空间, 并且所述后凹面、 前凸面是 朝向上偏前方向, 使集流翼 C将通过集流域 F的流体聚集流向翼 ml上表面的切线方向、 翼 mi将通过域 fi j的流体聚集流向翼 mj上表面的切线方向, 给翼 mi上表面的边界层提 供更大的流体动能, 来减小层流分离而使翼 mi的升力增大, 从而提高了叶片 Gndm的风能 利用系数 Cp; 通过调制集流翼 C相对于翼 ml所处的方位、翼 mi相对于翼 mj所处的方位, 控制翼 mi的升力值, 进而控制叶片 Gndm的功率。 Gndm, wherein the sub-blade Dm consists of m wings mi (m=n_l ^ l, i=l, 2, m) and m_l between the wing mi and the wing mj (j=i+lm, i =l, 2, ..., m_l) constitutes, through the collector wing C shape design, m of the wing mi shape design and between the collection basin F and m-1 wings mi and the wing mj The shape of the domain fi j is designed to And the relative orientation between the collecting wing C and the wing ml, the relative orientation between the wing mi and the wing mj, the domain fij being the rear concave surface of the wing mi and the front convex surface of the wing mj a space formed therebetween, and the rear concave surface and the front convex surface are oriented in an upwardly forward direction, so that the collecting wing C flows the fluid passing through the collecting basin F to the tangential direction of the upper surface of the wing ml, and the wing mi will pass through the domain fi The fluid accumulation flows to the tangential direction of the upper surface of the wing mj, providing greater fluid kinetic energy to the boundary layer of the upper surface of the wing mi, thereby reducing the laminar flow separation and increasing the lift of the wing mi, thereby increasing the wind energy utilization coefficient of the blade Gndm. Cp; Controls the lift value of the wing mi by controlling the orientation of the collector wing C relative to the wing ml and the orientation of the wing mi relative to the wing mj, thereby controlling the power of the blade Gndm.
以某种单翼 A的形状作为所述多翼叶片 Gn或 Gndm的外轮廓,其效果是能减小叶片 Gn 的阻力。  The shape of a certain type of single wing A is used as the outer contour of the multi-blade blade Gn or Gndm, and the effect is to reduce the resistance of the blade Gn.
以某种单翼 B的形状作为所述多翼叶片 Gndm中的子叶片 Dm的外轮廓, 其效果是能减 小子叶片 Dm (m 2)的阻力。  The outer contour of the sub-blade Dm in the multi-blade blade Gndm is formed in the shape of a certain one-wing B, and the effect is to reduce the resistance of the sub-blade Dm (m 2).
本发明提供的上述高效利用风能的多翼集流叶片, 充分利用了伯努利 (Bernoul l i effect ) 效应, 设计更趋合理, 该叶片能够对流过所述域的流体产生集流效应, 从而提高 所述多翼叶片的风能利用系数 Cp。  The above-mentioned multi-wing collecting blade with high efficiency utilizing wind energy fully utilizes the Bernoul li effect effect, and the design is more reasonable, and the blade can generate a collecting effect on the fluid flowing through the domain, thereby improving The wind energy utilization coefficient Cp of the multi-blade blade.
附图说明 DRAWINGS
图 la、 图 lb、 图 lc分别是本发明双翼、 三翼和四翼集流叶片 G2、 G3和 G4的一种构 形示意图。  Figures la, lb, and lc are schematic views of a configuration of the two-wing, three-wing, and four-wing collecting blades G2, G3, and G4 of the present invention, respectively.
图 2a、 图 2b、 图 2c、 图 2d分别是本发明双翼、 三翼、 四翼和五翼集流叶片 G2dl、 G3d2、 G4d3和 G5d4的一种构形示意图。  2a, 2b, 2c, and 2d are schematic views showing a configuration of the two-wing, three-wing, four-wing, and five-wing collecting blades G2dl, G3d2, G4d3, and G5d4 of the present invention, respectively.
图 3是本发明多翼集流叶片 Gn的构型通式示意图。  Fig. 3 is a schematic view showing the configuration of the multi-wing collecting blade Gn of the present invention.
图 4是本发明多翼集流叶片 Gndm的构型通式示意图。  Fig. 4 is a schematic view showing the configuration of the multi-wing collecting blade Gndm of the present invention.
图 5a、 图 5b、 图 5c分别是本发明由某种翼 A构造集流叶片 G2、 G3和 G4外轮廓的一 种构形示意图。  Figures 5a, 5b, and 5c are schematic views of a configuration of the outer contours of the collecting blades G2, G3 and G4 of the present invention by a certain wing A, respectively.
图 6a是本发明叶片 G2dl的一种构形示意图, 其中子叶片 D1为单翼子叶片。 图 6b、 图 6c、 图 6d分别是本发明以图 6a中子叶片 D1为翼 B构造子叶片 D2、 D3和 D4外轮廓的 的集流叶片 G3d2、 G4d3和 G5d4中的一种构形示意图。  Fig. 6a is a schematic view showing a configuration of the blade G2dl of the present invention, wherein the sub-blades D1 are single-wing sub-blades. Fig. 6b, Fig. 6c, and Fig. 6d are respectively schematic views showing one of the collecting blades G3d2, G4d3 and G5d4 of the outer contour of the sub-blades D2, D3 and D4 of the sub-blade D1 of Fig. 6a.
图 7是图 6a中 1的放大图、 是本发明集流叶片 G2dl调制集流翼 C相对于翼 11 (即 子叶片 D1)所处方位的一种示意图。 图 8是图 5a和图 6b中 Ψ 2的放大图、 是本发明集流叶片 G2和叶片 G3d2中子叶片 D2 调制翼 21相对于翼 22所处方位的一种示意图。 Fig. 7 is an enlarged view of 1 in Fig. 6a, which is a schematic view showing the orientation of the collecting vane G2dl of the present invention with respect to the wing 11 (i.e., the sub-blade D1). Figure 8 is an enlarged view of Ψ 2 in Figures 5a and 6b, showing a schematic view of the orientation of the sub-blade D2 modulating wings 21 relative to the wings 22 of the collecting blade G2 and the blade G3d2 of the present invention.
图 9是图 5b和图 6c中 Ψ 3的放大图、是本发明叶片 G3和叶片 G4d3中子叶片 D3调制 翼 32相对于翼 33所处方位的一种示意图。  Figure 9 is an enlarged view of Ψ 3 in Figures 5b and 6c, showing a schematic view of the orientation of the sub-blade D3 modulating wings 32 relative to the wings 33 of the blade G3 and the blade G4d3 of the present invention.
图 10是图 5c和图 6d中 Ψ4的放大图、 是本发明叶片 G4和叶片 G5d4中子叶片 D4调 制翼 43相对于翼 44所处方位的一种示意图。  Figure 10 is an enlarged view of Ψ4 in Figures 5c and 6d, which is a schematic illustration of the orientation of the blade G4 and the blade G5d4 of the present invention in which the sub-blade D4 modulates the wing 43 relative to the wing 44.
图 l la、图 l ib分别是本发明叶片 Gndm调制集流翼 C相对于子叶片 Dm的翼 ml所处方 位和调制翼 mi相对于翼 mj所处方位的一种示意图。  Fig. l la and Fig. 1 ib are respectively a schematic diagram of the position of the blade Gndm modulation collecting wing C of the present invention relative to the wing ml of the sub-blade Dm and the orientation of the modulation wing mi relative to the wing mj.
图 12是本发明叶片 Gn调制翼 ni相对于翼 nj所处方位的一种示意图。  Figure 12 is a schematic illustration of the orientation of the blade Gn modulation wing ni relative to the wing nj of the present invention.
图 13是本发明由叶片 G2dl的子叶片 D1形成的一种单翼叶片构形示意图。  Figure 13 is a schematic view showing a configuration of a single-wing blade formed by the sub-blades D1 of the blade G2dl of the present invention.
图 14a、 图 14b分别是本发明由某种翼 B构造一种叶片 G4d3中子叶片 D3的外轮廓和 由某种翼 A构造叶片 G4d3的外轮廓的一种构形示意图。  Fig. 14a and Fig. 14b are schematic views showing a configuration of the outer contour of the blade G4d3 neutron blade D3 and the outer contour of the blade G4d3 constructed by a certain wing A by the wing B of the present invention.
图 14c是以图 14b中 Ω的放大图为例, 说明按某种翼 A的形状构造一种叶片 G4d3的 示意图。  Fig. 14c is an enlarged view of Ω in Fig. 14b as an example, showing a schematic diagram of constructing a blade G4d3 in the shape of a certain wing A.
图 14d、 图 14e、 图 14f是一种分步骤构造叶片 G4d3的示意图。  Figures 14d, 14e, and 14f are schematic views of a stepwise construction blade G4d3.
图 15是本发明叶片 G2dl、 G3d2、 G4d3和 D1的 Cp随转角 Θ变化的示意图。  Fig. 15 is a view showing changes in Cp of the blades G2dl, G3d2, G4d3 and D1 according to the present invention as a function of the angle Θ.
图 16是本发明叶片 G2dl的计算流体动力学 (CFD)的流场示意图。  Figure 16 is a flow diagram showing the computational fluid dynamics (CFD) of the blade G2dl of the present invention.
图 17是由本发明叶片 G2dl形成的一种三维叶片示意图。  Figure 17 is a schematic illustration of a three-dimensional blade formed by the blade G2dl of the present invention.
图 18是由本发明叶片 G2dl形成的另一种三维叶片示意图。  Figure 18 is a schematic illustration of another three-dimensional blade formed by the blade G2dl of the present invention.
图 19是由本发明叶片 G3形成的一种三维叶片示意图。  Figure 19 is a schematic illustration of a three-dimensional blade formed by the blade G3 of the present invention.
图 20是由本发明叶片 G4形成的一种三维叶片示意图。  Figure 20 is a schematic illustration of a three-dimensional blade formed by the blade G4 of the present invention.
图 21a、 图 21b是由本发明叶片 G2dl形成的两种三维螺旋型叶片示意图。  Figures 21a and 21b are schematic views of two three-dimensional spiral type blades formed by the blade G2dl of the present invention.
图 22a、 图 22b是由本发明叶片 G2dl形成的两种三维 Φ型叶片示意图。  Figures 22a and 22b are schematic views of two three-dimensional Φ-type blades formed by the blade G2dl of the present invention.
具体实施方式 本发明提供的高效利用风能的多翼集流叶片, 包括至少两个翼和至少一 个相邻翼之间形成的域, 通过对每个所述翼和所述域的形状设计, 要能使相邻的所述翼对 流过其间所述域的流体产生一种集流效应, 并且通过设置所述相邻翼之间的相对方位以增 强所述集流效应、 增大流过所述域的流体的动能而提高所述域后面的所述翼的升力, 从而 提高整体所述多翼叶片的风能利用系数 Cp; 上述的多翼集流叶片的构造要点, 一是设计的 判据是构造形成的每个所述翼和所述域的形状必须能使流过所述域的流体流向所述域后 面相邻翼上表面的切线方向, 这样所述域的形状必须由其前面相邻翼的后凹面和后面相邻 翼的前凸面之间的空间构成、 并且所述后凹面和前凸面上部两者的共同特征是朝向上偏前 方向的流线型曲线, 所述域的形状与其两边相邻的所述翼的形状之间有相互的匹配性; 二 是所述相邻翼之间相对方位设置的判据是对流过所述域的流体产生的集流效应能最大程 度地提高所述域后面相邻翼的升力。在空气动力学领域,翼的形状是由流线型曲线构成的, 而流线型曲线没有对应的描述参量变化规律的数学函数解析表达式、 只能用坐标点数值描 述, 由于本发明的所述翼和所述域的形状之间相互的匹配性是相对的, 因此符合设计判据 构造的所述翼和所述域的形状不具有唯一性, 坐标点数值的描述方法不能概括本发明设计 技术构造结果的全貌。 在本发明所述翼和所述域的形状设计中, 针对设计目标制定的上述 两个判据是构造所述多翼集流叶片的关键技术, 在所述两个判据的指引下, 设计步骤是构 造→成形→检测→分析→再构造→再成形→在检测→再分析→……→直到构造出风能利 用系数 Cp对转角 Θ的平均值为极大值〈Cp〉maX对应的形状和方位为止,本发明构造了近百 个所述多翼集流叶片, 在 10米 /秒风速下, 有十几个多翼集流叶片的〈Cp〉maX达到 0. 20〜 0. 25、最大值 Cpmax达到 0. 35〜0. 40, 但它们所属的所述翼和所述域的形状以及所述相邻 翼之间的相对方位是不同的。 DETAILED DESCRIPTION OF THE INVENTION The present invention provides a multi-wing collecting blade for efficient use of wind energy, comprising a domain formed between at least two wings and at least one adjacent wing, by designing the shape of each of said wings and said domain, Enabling adjacent wings to create a current collecting effect on fluid flowing through the domains therebetween, and enhancing the current collecting effect by increasing the relative orientation between the adjacent wings The kinetic energy of the fluid of the domain increases the lift of the wing behind the domain, thereby increasing the wind energy utilization coefficient Cp of the multi-wing blade as a whole; the construction points of the multi-wing collecting blade described above, one is designed The criterion is that each of the wings and the domain formed by the configuration must be such that the fluid flowing through the domain flows in a tangential direction to the upper surface of the adjacent wing behind the domain, such that the shape of the domain must be a space between the rear concave surface of the front adjacent wing and the front convex surface of the rear adjacent wing, and a common feature of both the rear concave surface and the front convex surface portion is a streamlined curve toward the upper front direction, the shape of the domain There is mutual matching between the shapes of the wings adjacent to the two sides; the second is that the relative orientation between the adjacent wings is set to a maximum value for the current collecting effect on the fluid flowing through the domains. Raise the lift of adjacent wings behind the field. In the field of aerodynamics, the shape of the wing is composed of a streamlined curve, and the streamlined curve does not have a corresponding mathematical function analytical expression describing the law of variation of the parameter, which can only be described by the numerical value of the coordinate point, due to the wing and the The mutual matching between the shapes of the domain is relative, so the shape of the wing and the domain conforming to the design criterion structure is not unique, and the description method of the coordinate point value cannot summarize the construction result of the design technique of the present invention. The whole picture. In the shape design of the wing and the domain of the present invention, the above two criteria for the design goal are the key techniques for constructing the multi-wing collecting blade, under the guidance of the two criteria, design The steps are construction → forming → detection → analysis → reconstruction → reshaping → in detection → reanalysis → ... → until the wind energy utilization coefficient Cp is constructed to the average value of the corner Θ is the maximum value <Cp> ma X corresponding shape 〜 25. 25〜 0. 25。 The present invention has a configuration of the multi-wing collector blade, at a wind speed of 10 m / sec, more than a dozen multi-wing collecting blade <Cp> ma X reaches 0. 20~ 0. 25 The maximum value Cpmax reaches 0. 35~0. 40, but the shape of the wing and the domain to which they belong and the relative orientation between the adjacent wings are different.
所述的翼为 n个, 依次由翼 nl、 域 fl2、 翼 n2、 、 翼 ni、 域 fij、 翼 nj、 、 翼 n (n-l)、 域 f (n-l) n和翼 nn构成叶片 Gn, 即由 n个翼 ni (n 2、 i=l, 2, ,n)和 n_l 个由翼 ni与翼 nj之间的域 fij (j=i+l n、 i=l, 2,……,n_l)构成叶片 Gn, 通过所述 n个 翼 ni (n 2、 i=l, 2, , η)和所述 η_1 个翼 ni 与翼 nj 之间的所述域 fij (j=i+l n、 i=l,2,……,n-l)的形状设计、 以及所述 n-1个翼 ni与翼 nj之间相对方位的设置, 所述 域 fij 由所述翼 ni 的后凹面和所述翼 nj 的前凸面上部之间的空间形成、 并且所述翼 ni 的后凹面和所述翼 nj的前凸面上部两者都是凸面朝向上偏前方向的流线型, 使所述翼 ni 将通过所述域 fij的流体聚集流向所述翼 nj上表面的切线方向, 给所述翼 nj上表面的边 界层提供更多的流体动能, 来减小层流分离而使所述翼 nj 的升力增大, 从而提高了所述 叶片 Gn的风能利用系数 Cp; 通过调制所述翼 ni相对于所述翼 nj所处的方位而能控制所 述翼 nj的升力值, 进而就能控制所述叶片 Gn的功率。 可见, 本发明的叶片 Gn具有相对 高的 Cp性能和控制功率的功能, 因此适应更宽的风速范围。 所述的翼为 n个, 排头的翼 nl界定为集流翼 C, 其余的翼 ni (i=2,……, n) 构成子叶 片 Dm (m=n-1), 集流域 F是集流翼 C与子叶片 Dm之间的域、 由集流翼 C的下表面和子叶片 Dm前缘上部之间的空间形成, 由集流翼(:、 集流域 F和子叶片 Dm (m=n-1)构成叶片 Gndm, 其中的所述子叶片 Dm由翼 ml、域 f 12、翼 m2、 、翼 mi、域 fi j、翼 mj、 、翼 m (m- 1)、 域 f (m-l) m和翼 mm构成, 即由 m个翼 mi (m=n_l ^ l、 i=l, 2, , m)和 m_l个翼 mi与翼 mj之间的域 f i j ( j=i+l m、 i=l, 2,……, m)构成,通过所述集流翼 C和 m个所述翼 mi (m=n_l i=l, 2,…, m)以及所述集流域 F和 m-1个翼 mi与翼 mj之间的所述域 f i j (j=i+l m、 i=l, 2,……, m-1)的形状设计、 所述集流翼 C和 m个所述翼 mi (m=n-l l、 i=l, 2,… )之 间的相对方位设置, 所述域 fij由所述翼 mi的后凹面和所述翼 mj的前凸面之间的空间形 成、 并且所述翼 mi的后凹面和所述翼 mj的前凸面上部两者是凸面朝向上偏前方向的流线 型, 使集流翼 C将通过集流域 F的流体聚集流向翼 ml上表面的切线方向、 翼 mi将通过域 fij的流体聚集流向翼 mj上表面的切线方向, 给翼 mj上表面的边界层提供更多的流体动 能, 来减小层流分离而导致翼 mj的升力增大, 从而提高了叶片 Gndm的 Cp; 通过调制集流 翼 C相对于翼 ml所处的方位、 翼 mi相对于翼 mj所处的方位, 而能控制翼翼 ml、 mj的升 力值, 进而就能控制叶片 Gndm的功率, 当!11^ 2时, 子叶片 Dm与所述叶片 Gn的特征完全 相同。 The wings are n, and in turn, the blade N1, the domain fl1, the wing n2, the wing ni, the domain fij, the wing nj, the wing n (nl), the domain f (nl) n and the wing nn constitute the blade Gn, ie From n wings ni (n 2, i=l, 2, , n) and n_l are the domains fij between the wing ni and the wing nj (j=i+ln, i=l, 2, ..., n_l) Forming a blade Gn through the field fij between the n wings ni (n 2, i=l, 2, , η) and the η_1 wing ni and the wing nj (j=i+ln, i= a shape design of l, 2, ..., nl), and a relative orientation between the n-1 wings ni and the wing nj, the domain fij being defined by the rear concave surface of the wing ni and the wing nj A space between the front convex surface portions is formed, and both the rear concave surface of the wing ni and the front convex surface portion of the wing nj are streamlined in which the convex surface faces the upper front direction, so that the wing ni will pass through the domain The fluid accumulation of fij flows to the tangential direction of the upper surface of the wing nj, providing more fluid kinetic energy to the boundary layer of the upper surface of the wing nj to reduce the laminar flow separation and increase the lift of the wing nj, thereby Increasing the wind energy utilization coefficient Cp of the blade Gn; by modulating the wing ni phase The lift value of the wing nj can be controlled for the orientation in which the wing nj is located, thereby controlling the power of the blade Gn. It can be seen that the blade Gn of the present invention has a relatively high Cp performance and a function of controlling power, and thus accommodates a wider range of wind speeds. The wings are n, the wing n1 of the head is defined as the collecting wing C, and the remaining wings ni (i=2, . . . , n) constitute the sub-blade Dm (m=n-1), and the collecting basin F is a set. The domain between the flow wing C and the sub-blade Dm is formed by the space between the lower surface of the collecting wing C and the upper portion of the leading edge of the sub-blade Dm, by the collecting wing (:, the collecting basin F and the sub-blade Dm (m=n- 1) constituting a blade Gndm, wherein the sub-blade Dm is composed of a wing ml, a domain f 12, a wing m2, a wing mi, a domain fi j, a wing mj, a wing m (m-1), a domain f (ml) m And wing mm, that is, the domain fij between m wings mi (m=n_l ^ l, i=l, 2, m) and m_l wings mi and wing mj ( j=i+lm, i=l , 2, ..., m) constituted by the collecting wing C and m of the wings mi (m=n_l i=l, 2,..., m) and the collecting basin F and m-1 wings Shape design of the domain fij (j=i+lm, i=l, 2, . . . , m-1) between mi and wing mj, the collector wing C and m of the wings mi (m a relative orientation setting between =nl l, i=l, 2,...), the field fij being formed by the space between the rear concave surface of the wing mi and the front convex surface of the wing mj, and the wing mi Back concave surface and front convex surface of said wing mj Both of them are streamlined with the convex surface facing the upper direction, so that the collecting wing C will concentrate the fluid flowing through the collecting basin F to the tangential direction of the upper surface of the wing ml, and the wing mi will concentrate the fluid passing through the domain fij to the upper surface of the wing mj. The tangential direction provides more fluid kinetic energy to the boundary layer of the upper surface of the wing mj to reduce the laminar flow separation and increase the lift of the wing mj, thereby increasing the Cp of the blade Gndm; The orientation of the wing ml and the orientation of the wing mi relative to the wing mj can control the lift values of the wings ml and mj, and thus the power of the blade Gndm can be controlled. When !11^2, the sub-blade Dm and the The characteristics of the blade Gn are identical.
一种设计所述多翼集流叶片的方法,是以某种单翼 A的形状为所述多翼集流叶片的外 轮廓, 在所述单翼 A的上、 下表面之间连接至少两条流线型曲线形成至少一个缝形空间, 所述两条流线型曲线的凸面朝向上偏前的方向, 并在所述两条流线型曲线与所述单翼 A的 上、 下表面的结合部进行流畅性过度的流线型构造, 再去掉流畅性构造后形成的所述两条 流线型曲线之间的所述单翼 A的部分, 这样构成的缝形空间就是所述域的形状, 所述域两 边保留的所述单翼 A的部分形成至少由两个闭合流线型曲线构成的形状, 每个闭合的流线 型曲线形状就是设计形成的每个所述翼; 设计中, 形状的判别标准是构造的每个所述翼和 所述域的形状能使流过所述域的流体流向所述域后面的所述翼上表面的切线方向; 所述域 宽窄尺度的判别标准是对流过所述域的流体产生的集流效应能最大程度地提高所述域后 面的所述翼的升力, 从而提高整体所述多翼叶片的风能利用系数 Cp。 以某种单翼 A的形状 为所述多翼集流叶片的外轮廓形状的设计方法的效果是能减小多翼集流叶片的阻力。  A method for designing the multi-wing collecting blade is such that the shape of a certain single wing A is the outer contour of the multi-wing collecting blade, and at least two are connected between the upper and lower surfaces of the single wing A. The strip streamline curve forms at least one slit-shaped space, the convex surfaces of the two streamlined curves are oriented in the upwardly forward direction, and the joint between the two streamlined curves and the upper and lower surfaces of the single wing A is smooth Excessive streamlined configuration, and then removing the portion of the single wing A between the two streamlined curves formed after the fluent structure, the slit space thus formed is the shape of the domain, and the two sides of the domain are retained The portion of the single wing A forms a shape formed by at least two closed streamline curves, each closed streamline curve shape being each of the wings formed by the design; in the design, the criterion for determining the shape is each of the configurations The shape of the wing and the domain enables fluid flowing through the domain to flow in a tangential direction to the upper surface of the wing behind the domain; the criterion for the narrowness of the domain width is the flow through the domain Collecting effect produced can be improved later in the domain maximally lift of the wing, thereby improving the overall power coefficient of the plurality of blades of Cp. The effect of the design method of the shape of the outer contour of the multi-wing collecting blade in the shape of a certain type of single wing A is to reduce the resistance of the multi-wing collecting blade.
所述的翼为 n个, 依次由翼 nl、 域 fl2、 翼 n2、 、 翼 ni、 域 fij、 翼 nj、 、 翼 n (n-l)、 域 f (n-l) n和翼 nn构成叶片 Gn, 即由 n个翼 ni (n 2、 i=l, 2, ,n)和 n_l 个由翼 ni与翼 nj之间的域 fij (j=i+l n、 i=l, 2,……,n_l)构成叶片 Gn, 以某种单翼 A 的形状为所述叶片 Gn的外轮廓, 在所述单翼 A的上、 下表面之间连接 2 (n-1)条其凸面朝 向上偏前方向的流线型曲线形成 n-1个缝形空间, 并在形成每个所述缝形空间的两条流线 型曲线与所述单翼 A上、 下表面的各两个结合部进行流畅性过度的流线型构造, 再去掉流 畅性构造后形成的 n-1个缝形空间内的所述单翼 A的部分, 这样构成的空间就是 n-1个所 述域 fij (j=i+l n、 i=l, 2,……, n_l)的形状, n_l个所述域 fij两边保留的所述单翼 A 的部分形成 n 个由闭合流线型曲线构成的形状, 就是设计形成的 n 个所述翼 ni (n 2、 i=l, 2,……, n), 设计所述翼 ni和所述域 fi j形状的判别标准以及所述域 fij宽窄尺度的 判别标准是所述翼 ni将通过所述域 fi j的流体聚集流向所述翼 nj上表面的切线方向, 给 所述翼 nj上表面的边界层提供更多的流体动能, 来减小层流分离而使所述翼 nj的升力增 大, 从而提高了所述叶片 Gn的风能利用系数 Cp。 The wings are n, in turn by the wing nl, the domain fl2, the wing n2, the wing ni, the domain fij, the wing nj, The wing n (nl), the domain f (nl) n and the wing nn constitute the blade Gn, that is, between n wings ni (n 2, i = l, 2, , n) and n_l between the wing ni and the wing nj The field fij (j=i+ln, i=l, 2, . . . , n_l) constitutes a blade Gn, and the shape of a certain single wing A is the outer contour of the blade Gn, on the single wing A, a streamlined curve connecting the 2 (n-1) strips with the convex surface toward the upper front direction to form n-1 slit-shaped spaces, and two streamline curves forming each of the slit-shaped spaces and the The two joint portions on the upper and lower surfaces of the single wing A are subjected to a streamlined structure with excessive fluency, and the portion of the single wing A in the n-1 slit-shaped spaces formed by the fluent structure is removed, and the space thus constituted Is the shape of n-1 of the domains fij (j=i+ln, i=l, 2, . . . , n_l), and n parts of the single-wing A remaining on both sides of the domain fij form n The shape formed by the closed streamline curve is the n said wings ni (n 2, i=l, 2, ..., n), and the criterion for designing the shape of the wing ni and the domain fi j and the The criterion for judging the width and narrowness of the domain fij is that the wing ni will The condensed flow of the domain fi j to the tangential direction of the upper surface of the wing nj provides more fluid kinetic energy to the boundary layer of the upper surface of the wing nj to reduce laminar flow separation and make the wing nj The lift is increased, thereby increasing the wind energy utilization coefficient Cp of the blade Gn.
用同样的设计方法, 以某种单翼 B的形状为所述叶片 Gndm中的子叶片 Dm的外轮廓, 构造子叶片 Dm 的 m个所述翼 mi (m 2、 i=l, , m)和 m_l 个所述域 fij (j=i+l m、 i=l, 2,……, m-1)的形状和所述的方位。  With the same design method, the shape of the single wing B is the outer contour of the sub-blade Dm in the blade Gndm, and the m wings mi of the sub-blade Dm are constructed (m 2, i=l, , m) And m_l the shape of the domain fij (j=i+lm, i=l, 2, . . . , m-1) and the orientation described.
用同样的设计方法, 即以某种单翼 A的形状为所述叶片 Gndm的外轮廓, 又以某种单 翼 B的形状为所述叶片 Gndm中的子叶片 Dm的外轮廓, 构造集流翼 C和子叶片 Dm的 m个 所述翼 mi (m 2、 i=l, , m)和 m_l个所述域 fij (j=i+l m、 i=l, 2, , m-1)的形状和 所述的方位。  By the same design method, that is, the shape of a certain single wing A is the outer contour of the blade Gndm, and the shape of a certain single wing B is the outer contour of the sub-blade Dm in the blade Gndm, the current is constructed. The shapes of the m wings mi (m 2, i=l, , m) of the wing C and the sub-blade Dm and m_l of the domain fij (j=i+lm, i=l, 2, , m-1) And the orientation described.
下面结合附图和实施例对本发明作进一步描述。  The invention is further described below in conjunction with the drawings and embodiments.
如图 la、 图 lb、 图 lc所示的双翼 G2、 三翼 G3和四翼 G4集流叶片, 它们分别包括两 个翼 21、 22, 三个翼 31、 32、 33和四个翼 41、 42、 43、 44, 相邻翼之间的域分别为 fl2, fl2、 f23及 fl2、 f23、 f34, 每个翼的形状设计、 翼之间彼此的流线型匹配和相对方位的 设置, 须能对流过相邻翼之间域的流体产生一种集流效应, 增大流过所述域流体的动能而 提高所述域后面的所述翼的升力, 从而提高整体叶片的风能利用系数。  a two-wing G2, a three-wing G3 and a four-wing G4 collecting blade as shown in FIGS. 1a, 1b, and 1c, which respectively include two wings 21, 22, three wings 31, 32, 33 and four wings 41, 42, 43, 44, the fields between adjacent wings are fl2, fl2, f23 and fl2, f23, f34, the shape design of each wing, the streamline matching between the wings and the relative orientation, must be convective Fluid passing through the domains between adjacent wings creates a current collecting effect that increases the kinetic energy of the fluid flowing through the domain to increase the lift of the wings behind the field, thereby increasing the wind energy utilization factor of the overall blade.
如图 2a、 图 2b、 图 2c、 图 2d所示的双翼 G2dl、 三翼 G3d2、 四翼 G4d3和五翼 G5d4 集流叶片, 排头的翼 C具有特殊性, 无论是几翼集流叶片, 排头的翼 C形状特征都是相同 的, 只起集流作用, 自身的升力不能提高。 而其余的翼担当叶片的动力翼角色, 它们和相 邻翼之间的域形成与图 1中对应叶片有相同特征的子叶片 D2、 D3 和 D4, 还包括子叶片为 一翼 D1的情况。 集流翼 C与子叶片 Dl、 D2、 D3、 D4之间的域命名为集流域 F。 此处将 子叶片 D变为 d强调了此类叶片仍然是本发明多翼集流叶片的一种。 叶片中的集流翼 C仅 起集流作用, 这给起动力翼作用的子叶片 Dm有更大弦长的空间。 As shown in Figure 2a, Figure 2b, Figure 2c, Figure 2d, the two-wing G2dl, three-wing G3d2, four-wing G4d3 and five-wing G5d4 collecting blades, the wing C of the head has special characteristics, whether it is a few wing collecting blades, the head The wing C shape features are the same, only the current collecting function, the lift of its own can not be improved. And the remaining wings act as the power wing characters of the blades, they and The domains between the adjacent wings form sub-blades D2, D3 and D4 having the same characteristics as the corresponding blades in Fig. 1, and also include the case where the sub-blades are one wing D1. The domain between the collecting wing C and the sub-blades D1, D2, D3, D4 is named the collecting basin F. The sub-blade D is changed to d here to emphasize that such a blade is still one of the multi-wing collecting blades of the present invention. The collecting wings C in the blades only serve as a current collecting, which gives the power blades a sub-blade Dm with a larger chord space.
图 3和图 4分别是本发明叶片 Gn和叶片 Gndm的示意图,其中虚线形状代表由 "…… " 表示的诸翼和翼之间域构成部分形成的轮廓、 并不代表某个翼的形状, "叶片 Gn由翼 nl、 域 fl2、 翼 n2、 、 翼 ni、 域 fij、 翼 nj、 、 翼 n (n- 1)、 域 f (n_l) n和翼 nn构成" 和 "叶片 Gndm是由集流翼 (、 集流翼 C与子叶片之间的域 F、 子叶片 Dm (m=n_l)由翼 ml、 3 and 4 are schematic views of the blade Gn and the blade Gndm of the present invention, respectively, wherein the dotted line shape represents the contour formed by the domain components between the wings and the wing represented by "...", and does not represent the shape of a certain wing. "The blade Gn consists of the wing nl, the domain fl2, the wing n2, the wing ni, the domain fij, the wing nj, the wing n (n-1), the domain f(n_l) n and the wing nn constitute "and" the blade Gndm is set by The flow wing (the domain F between the collecting wing C and the sub-blades, the sub-blade Dm (m=n_l) is composed of the wing ml,
± ¾ fl2、 翼 m2、 、 翼 mi、 ± ¾ fij、 翼 mj、 、 翼 m (m_l)、 ±或 f (m_l) m禾口翼隱构成" 的通用表述对应的通用意义上的示意图, 叶片 Gndm是一种有更大 Cp的叶片 Gn。 Schematic diagram of the general sense corresponding to the general expression of ± 3⁄4 fl2, wing m2, wing mi, ± 3⁄4 fij, wing mj, wing m (m_l), ± or f (m_l) m Gndm is a leaf Gn with a larger Cp.
图 5、 图 6所示的本发明实施例与图 1和图 2所示的本发明实施例之间的不同在于: 图 5所示叶片的外轮廓按某种翼 A形状构造, 图 6所示叶片中的子叶片外轮廓按某种翼 B 形状构造, 在 m=l时, 子叶片 D1是单翼叶片, 子叶片 D1的翼型作为所述翼 B的一种选择, 其中某种翼 A、 某种翼 B可以是现有的某种翼型, 也可以是未来性能更佳的某种翼型。 而 图 1和图 2所示叶片的构造没有这种外轮廓的要求, 其阻力相对大于外轮廓有翼的形状规 范构造叶片的。  The difference between the embodiment of the present invention shown in Figures 5 and 6 and the embodiment of the present invention shown in Figures 1 and 2 is that the outer contour of the blade shown in Figure 5 is constructed in a certain wing A shape, Figure 6 The outer contour of the sub-blades in the blade is constructed according to a certain wing B shape. When m=l, the sub-blade D1 is a single-wing blade, and the airfoil of the sub-blade D1 is an option of the wing B, wherein some wing A. Some kind of wing B can be some existing airfoil, or it can be some kind of airfoil with better performance in the future. The configuration of the blades shown in Figures 1 and 2 does not require such an outer profile, and the resistance is relatively greater than that of the outer profile winged configuration.
图 7、 图 8、 图 9和图 10分别依次显示图 5和图 6所示的所述叶片的 Ψ 1、 Ψ2、 Ψ3 和 Ψ4部位的放大图。 图 6£1所示叶片 G2dl由集流翼 C和翼 11 (即子叶片 D1)构成, 当调制 集流翼 C相对于翼 11所处方位时(图 7中的虚线所示), 就能改变流过集流域 F流体的通 量和流速、 继而改变流到翼 11上表面流体的动能和流向, 致使翼 11上表面的层流分离和 翼 11的升力值出现变化, 因而能调制 G2dl的 Cp, 达到控制功率的目的。 同理, 在图 5a 和图 6b所示叶片 G2和 G3d2中, 调制翼 21相对于翼 22所处的方位(图 8中的虚线所示), 就能改变流过域 2流体的通量和流速、 继而改变流到翼 22上表面流体的动能和流向, 致使翼 22上表面的层流分离和翼 22的升力值出现变化, 因而能调制 G2和 G3d2的 Cp, 达 到控制功率的目的。 在图 5b和图 6c所示叶片 G3和 G4d3中, 调制翼 32相对于翼 33所处 的方位(图 9中的虚线所示), 就能改变流过域 f23流体的通量和流速、继而改变流到翼 33 上表面流体的动能和流向, 致使翼 33上表面的层流分离和翼 33的升力值出现变化, 因而 能调制 G3和 G4d3的 Cp, 达到控制功率的目的。 在图 5c和图 6d所示叶片 G4和 G5d4中, 调制翼 43相对于翼 44所处的方位(图 10中的虚线所示), 就能改变流过域 f34流体的通 量和流速、 继而改变流到翼 44上表面流体的动能和流向, 致使翼 44上表面的层流分离和 翼 44的升力值出现变化, 因而能调制 G4和 G5d4的 Cp, 达到控制功率的目的。 用同样的 方法, 调制集流翼 C相对于翼 21、 翼 31、 翼 41所处方位、 调制翼 31相对于翼 32所处方 位、 调制翼 41相对于翼 42所处方位和调制翼 42相对于翼 43所处方位时, 均能以上述对 翼 11、 翼 22、 翼 33和翼 44产生作用的机理, 同样达到控制功率的目的。 7, 8, 9, and 10 sequentially show enlarged views of the Ψ 1, Ψ 2, Ψ 3, and Ψ 4 portions of the blade shown in Figs. 5 and 6, respectively. The blade G2dl shown in Fig. 6 is composed of the collecting wing C and the wing 11 (i.e., the sub-blade D1). When the position of the collecting wing C relative to the wing 11 is adjusted (shown by a broken line in Fig. 7), Varying the flux and flow rate of the fluid flowing through the header F, and then changing the kinetic energy and flow direction of the fluid flowing to the upper surface of the wing 11, causing the laminar flow separation of the upper surface of the wing 11 and the lift value of the wing 11 to change, thereby modulating the G2dl Cp, to achieve the purpose of controlling power. Similarly, in the blades G2 and G3d2 shown in Figures 5a and 6b, the modulation wing 21 is oriented relative to the orientation of the wing 22 (shown in phantom in Figure 8), and the flux flowing through the domain 2 fluid can be varied. The flow rate, which in turn changes the kinetic energy and flow direction of the fluid flowing to the upper surface of the wing 22, causes laminar flow separation of the upper surface of the wing 22 and changes in the lift value of the wing 22, thereby modulating the Cp of G2 and G3d2 for the purpose of controlling power. In the blades G3 and G4d3 shown in Figures 5b and 6c, the orientation of the modulation wing 32 relative to the wing 33 (shown in phantom in Figure 9) changes the flux and flow rate of the fluid flowing through the field f23, and The kinetic energy and flow direction of the fluid flowing to the upper surface of the wing 33 are changed, so that the laminar flow separation of the upper surface of the wing 33 and the lift value of the wing 33 are changed, so that the Cp of G3 and G4d3 can be modulated to achieve the purpose of controlling the power. In the blades G4 and G5d4 shown in Figures 5c and 6d, The orientation of the modulation wing 43 relative to the wing 44 (shown in phantom in Figure 10) changes the flux and flow rate of the fluid flowing through the field f34, and in turn changes the kinetic energy and flow of the fluid flowing to the upper surface of the wing 44, resulting in The laminar flow separation of the upper surface of the wing 44 and the lift value of the wing 44 are varied, so that the Cp of G4 and G5d4 can be modulated to achieve the purpose of controlling power. In the same manner, the orientation of the current collecting wing C relative to the wing 21, the wing 31, the wing 41, the orientation of the modulation wing 31 relative to the wing 32, the orientation of the modulation wing 41 relative to the wing 42 and the modulation wing 42 are relative. At the same position as the wing 43, the above-mentioned mechanism for acting on the wing 11, the wing 22, the wing 33 and the wing 44 can also achieve the purpose of controlling power.
图 l la、图 l ib和图 12分别示出对叶片 Gndm和叶片 Gn调制方位的通用意义上的示意 图, 调制集流翼 C相对于翼 ml所处方位的变化由图 11a中的虚线所示、 调制翼 mi相对于 翼 mj所处方位的变化由图 l ib中的虚线所示、 调制翼 ni相对于翼 nj所处方位的变化由 图 12中的虚线所示。  1a, 1b and 12 respectively show a schematic view of the general orientation of the modulation of the blade Gndm and the blade Gn, the change of the orientation of the modulation collecting wing C with respect to the wing ml is indicated by the dashed line in Fig. 11a The change in the orientation of the modulation wing mi relative to the wing mj is indicated by the dashed line in FIG. 1 ib, and the change in the orientation of the modulation wing ni relative to the wing nj is indicated by the dashed line in FIG.
如图 13所示的是用于对比的单翼叶片 Dl。  Shown in Figure 13 is a single wing blade Dl for comparison.
图 14a、 图 14b所示子叶片 D3和叶片 G4d3两者的外轮廓分别按某种翼 B形状和按某 种翼 A形状构造。  The outer contours of both the sub-blades D3 and the blades G4d3 shown in Figs. 14a and 14b are respectively configured in a certain wing B shape and in a certain wing A shape.
图 14c是在图 14b中 Ω的放大图中, 以所述翼 A的形状为构造 G4d3的外轮廓, 在所 述单翼 A的上、 下表面之间连接 2 (4-1) =6条由虚线所示的凸面朝向上偏前方向的流线型 曲线形成了 3个由横线阴影区域所示的缝形空间, 在形成的每个横线阴影区域两边的流线 型曲线与所述翼 A上、 下表面的结合部进行流畅性过度的流线型构造, 又形成了由斜线阴 影区域所示的部分, 去掉由横线和斜线阴影区域内的所述翼 A的部分形成的 3个空间, 从 所述翼 A的前缘起始, 依次就是图 14b所示的集流域 F、子叶片 D3的域 f 12和域 f23的形 状, 保留的所述翼 A的部分依次就是图 14b所示的集流翼 (:、 子叶片 D3的翼 31、 翼 32和 翼 33 的形状。 上述横线阴影区域的形状构造的要点是确定形成域中流体的流向符合构形 的判据, 斜线阴影区域是多次构造成形的, 即集流翼 C的下表面、 翼 31 的前凸面和后凹 面、 翼 32的前凸面和后凹面以及翼 33的前凸面是多次构造成形的, 最终形成的所述集流 翼 C、 子叶片 D3的翼 31和翼 32将通过所述集流域 F、 子叶片 D3的域 f 12和域 f23中流 过的流体聚集流向所述翼 31、 翼 32和翼 33上表面的切线方向, 所述集流域 F、 子叶片 D3 的域 2和域 f23宽窄尺度或它们相邻翼之间相对方位是在与图 16所示相邻翼之间类似 的区域中流体有显著的集流效应; 这样给所述子叶片 D3的翼 31、 翼 32和翼 33上表面的 边界层提供更多的流体动能, 来减小层流分离而使所述翼 31、 翼 32和翼 33的升力增大, 最终确定的叶片 G4d3构形是一系列构造的集流翼 (:、 子叶片 D3的翼 31、 翼 32和翼 33及 其相对方位中对应叶片 G4d3的风能利用系数 Cp对转角 Θ的平均值为极大值〈Cp〉maX的形 状和方位。 Figure 14c is an enlarged view of Ω in Figure 14b, with the shape of the wing A as the outer contour of the configuration G4d3, connecting 2 (4-1) = 6 between the upper and lower surfaces of the single wing A The streamlined curve from the convex surface indicated by the broken line toward the upper front direction forms three slit-shaped spaces indicated by the hatched areas of the horizontal line, and the streamlined curves on both sides of each of the horizontally shaded areas formed are formed on the wing A The joint portion of the lower surface is fluently streamlined, and the portion indicated by the hatched area is formed, and the three spaces formed by the portions of the wing A in the shaded area and the hatched area are removed. Starting from the leading edge of the wing A, the shape of the watershed F, the domain f 12 and the domain f23 of the sub-blade D3 shown in Fig. 14b is in turn, and the remaining portions of the wing A are in turn the set shown in Fig. 14b. The shape of the flow wing (:, the wing 31 of the sub-blade D3, the wing 32, and the wing 33. The point of the shape configuration of the above-mentioned horizontally shaded area is to determine the flow direction of the fluid in the formation domain to conform to the configuration, the shaded area is The structure is formed a plurality of times, that is, the lower surface of the collecting wing C, the front convex surface of the wing 31, and the rear The concave surface, the front convex surface and the rear concave surface of the wing 32, and the front convex surface of the wing 33 are formed in a plurality of configurations, and the finally formed collecting wing C, the wing 31 of the sub-blade D3 and the wing 32 will pass through the collecting basin F, The fluid flow flowing in the domains f 12 and F23 of the sub-blades D3 flows toward the tangential direction of the upper surfaces of the wings 31, the wings 32 and the wings 33, and the watershed F, the domain 2 and the domain f23 of the sub-blades D3 are narrow or narrow or The relative orientation between their adjacent wings is a significant current collecting effect in the region similar to that between the adjacent wings shown in Figure 16; thus giving the wings 31, wings 32 and the upper surface of the wings 33 of the sub-blades D3 The boundary layer provides more fluid kinetic energy to reduce laminar flow separation and increase the lift of the wings 31, wings 32 and wings 33, The final determined blade G4d3 configuration is the average of the wind angle utilization factor of the wind energy utilization coefficient Cp of the series of configured collecting wings (:, the wing 31, the wing 32 and the wing 33 of the sub-blade D3 and the corresponding blade G4d3 in the relative orientation is The shape and orientation of the maximum value <Cp>ma X.
一种分别构造叶片 G4d3所属翼和域的设计方法由图 14d、图 14e、图 14f所示, 图 14d 所示的第一步是以单翼 A为外轮廓, 构造出对应〈Cp〉maXl的叶片 G2dl ' 的集流翼 C、集流 域 F和子叶片 D1 ' 的形状和方位;图 14e所示的第二步是以确定的子叶片 D1 ' 为外轮廓 (类 似图 6b的翼 B)构造子叶片 D2 ' 的翼 2 、 域 2和翼 22 ' , 它们与第一步确定的集流 翼 C和集流域 F配合构造出对应〈〔 〉111£^2的叶片 G3d2 ' 中子叶片 D2 ' 的翼 2 、 域 f 12 和翼 22 ' 的形状和方位;图 14f所示的第三步是以翼 22 ' 为外轮廓构造子叶片 D3的翼 32、 域 f23和翼 33, 它们与第一步确定的集流翼 C和集流域?、 第二步确定的翼 2 和域 2 配合构造出对应〈〔 〉111£^的叶片 G4d3, 翼 2 就是确定的翼 31。 这种分步逐个构造翼和 域方法的优点是利于分析形状和方位与性能之间的关系。 A design method for respectively constructing the wing and the domain to which the blade G4d3 belongs is shown in Fig. 14d, Fig. 14e, and Fig. 14f, and the first step shown in Fig. 14d is to use the single wing A as the outer contour to construct a corresponding <Cp>ma X The shape and orientation of the collecting wing C, the collecting basin F and the sub-blade D1 ' of the blade G2dl '; the second step shown in Fig. 14e is to determine the sub-blade D1' as the outer contour (similar to the wing B of Fig. 6b) Constructing the wing 2, the domain 2 and the wing 22' of the sub-blade D2', which cooperate with the collecting wing C and the collecting basin F determined in the first step to construct the blade G3d2' neutron blade D2 corresponding to <[>111£^2 The shape and orientation of 'wing 2, domain f 12 and wing 22'; the third step shown in Fig. 14f is to construct the wing 32, the domain f23 and the wing 33 of the sub-blade D3 with the outer contour of the wing 22', which are the same as the One-step determination of the collector wing C and the collection basin? The wing 2 and the domain 2 determined in the second step cooperate to construct a blade G4d3 corresponding to <[>111£^, and the wing 2 is the determined wing 31. The advantage of this step-by-step construction of the wing and domain approach is that it facilitates the analysis of the relationship between shape and orientation and performance.
如图 15、 图 16所示, 以图 6所示的双翼、 三翼和四翼集流叶片 G2dl、 G3d2 G4d3以 及图 13所示的用于对比的单翼叶片 D1为实施例, 进行了大量的计算流体动力学仿真模拟 和试验, 研究结果表明上述的多翼集流叶片的 Cp相比同弦长单翼叶片 D1有显著提高, 特 别是在中低风速区间其 Cp有大幅的提高。 由图 15所示, 叶片 Dl、 G2dl、 G3d2和 G4d3的 Cp依次提高、 并且 Cp的最大值随叶片构成翼的数量增加移向大转角 Θ角的方向。 由图 16 所示, 集流域 F内的流线密度加大、 颜色变亮 (表示流速变快)并延续到下游翼上表面的一 段长度上; 这个现象体现了集流翼 C将集流域 F内流体的动能提高、 并导向下游翼上表面 的切线方向。 综合图 15和图 16所示的研究结果, 说明在本发明设计的多翼叶片构形中, 构成叶片的各翼之间, 相对流体流动的方向而言, 上游翼对下游翼有聚集流体和导向流动 方向、 并给下游翼提供更大动能流体的作用, 致使下游翼上表面的层流分离出现在更大转 角处而提高了下游翼的升力。 这就在理论上解释了图 15 所示的现象, 证明了上述的上游 翼与下游翼配合能对流体生产一种集流效应。 因此, 本发明的叶片起名为多翼集流叶片。  As shown in Fig. 15 and Fig. 16, the two-wing, three- and four-wing collecting blades G2d1, G3d2 and G4d3 shown in Fig. 6 and the single-winged blade D1 shown in Fig. 13 are used as an embodiment, and a large number of Computational fluid dynamics simulation and experiment, the results show that the Cp of the multi-wing collecting blade has a significant improvement compared with the chord-long single-wing blade D1, especially in the middle and low wind speed range. As shown in Fig. 15, the Cp of the blades D1, G2dl, G3d2, and G4d3 is sequentially increased, and the maximum value of Cp is increased toward the direction of the large corner angle with the number of blade-forming wings. As shown in Fig. 16, the streamline density in the collection basin F is increased, the color is brighter (indicating that the flow velocity is faster) and continues to a length of the upper surface of the downstream wing; this phenomenon embodies that the collector wing C will collect the basin F The kinetic energy of the inner fluid is increased and directed to the tangential direction of the upper surface of the downstream wing. Combining the results of the research shown in Fig. 15 and Fig. 16, it is shown that in the multi-blade configuration of the present invention, between the wings constituting the blade, the upstream wing has a collecting fluid to the downstream wing with respect to the direction of fluid flow. The direction of flow is directed and the downstream wing is provided with a larger kinetic energy fluid, causing laminar separation of the upper surface of the downstream wing to occur at a larger corner and increasing the lift of the downstream wing. This theoretically explains the phenomenon shown in Fig. 15, which proves that the above-mentioned upstream wing and downstream wing can produce a current collecting effect on the fluid. Therefore, the blade of the present invention is named as a multi-wing collecting blade.
图 17、 图 18、 图 21a、 21b和图 22a、 图 22b是本发明叶片 G2dl的三维叶片示意图, 图 19和图 20分别是本发明叶片 G3和叶片 G4的三维叶片示意图。 图 17、 图 19和图 20所 示的叶片能应用作为像 "H"形、 "Y"形、 " Δ "形和 "◊"形样式的立轴(又称垂直轴)风 力机的叶片; 图 21a所示叶片的凹面朝外、 图 21b所示叶片的凹面朝内, 它们能应用作为 像螺旋形样式的立轴风力机的叶片; 图 22a所示叶片的凹面朝内、 图 22b所示叶片的凹面 朝外, 它们能应用作为像 " Φ"形样式的立轴风力机的叶片; 图 18 所示的叶片能应用作 为水平轴风力机的叶片。 17, 18, 21a, 21b and 22a, 22b are schematic views of three-dimensional vanes of the blade G2dl of the present invention, and Figs. 19 and 20 are schematic views of three-dimensional vanes of the vane G3 and the vane G4 of the present invention, respectively. The blades shown in Figures 17, 19 and 20 can be applied as blades of vertical shaft (also known as vertical axis) wind turbines in the form of "H", "Y", "Δ" and "◊"shapes; The concave surface of the blade shown in Fig. 21a faces outward, and the concave surface of the blade shown in Fig. 21b faces inward, they can be applied as A blade of a vertical axis wind turbine like a spiral pattern; the concave surface of the blade shown in Fig. 22a faces inward, and the concave surface of the blade shown in Fig. 22b faces outward, they can be applied as blades of a vertical axis wind turbine like a "Φ"shape; Fig. 18 The blade shown can be applied as a blade for a horizontal axis wind turbine.
以上仅列举了本发明的三种叶片的应用, 对本发明叶片 Gn和叶片 Gndm, 当取 n或 m 为不同值时, 能形成的叶片种类很多, 都能应用到包括上述风力机类型在内的众多风力机 类型上。 综合考虑风力机功率和叶片的制造、 运输和安装成本等因素, 所述 n或 m的取值 范围优选 2 n 30、 l^m^29, 原则上, 在 16 n 30、 15 m 29的范围时, 本发明的 叶片较适于担当大功率风力机的叶片; 在 6 n 15、 5^m^l4 的范围时, 本发明的叶片 较适于担当大中功率风力机的叶片; 在 4 n 10、 3 m 9的范围时, 本发明的叶片适于 担当中功率风力机的叶片; 当在 2 n 5、 l^m^4 的范围时, 本发明的叶片适于担当小 功率及其以下功率风力机的叶片。 这也体现本发明叶片有性价比的选择性优势。  The above only enumerates the application of the three types of blades of the present invention. When the blade Gn and the blade Gndm of the present invention have different values of n or m, many types of blades can be formed, which can be applied to the types including the above-mentioned wind turbines. Many types of wind turbines. Considering factors such as wind turbine power and blade manufacturing, transportation and installation costs, the value range of n or m is preferably 2 n 30, l^m^29, in principle, in the range of 16 n 30, 15 m 29 When the blade of the present invention is more suitable for the blade of the high-power wind turbine; in the range of 6 n 15 , 5 ^ m ^ l4 , the blade of the invention is more suitable for the blade of the large medium-power wind turbine; In the range of 10, 3 m 9 , the blade of the present invention is suitable for the blade of the medium power wind turbine; when in the range of 2 n 5 , l^m^4, the blade of the invention is suitable for low power and below Blades of power wind turbines. This also embodies the cost-effective selectivity advantages of the inventive blade.

Claims

权利要求 Rights request
1. 一种高效利用风能的多翼集流叶片, 其特征是它包括至少两个翼和至少一个相邻翼之 间形成的域, 通过对每个所述翼和所述域的形状设计, 使相邻的所述翼对流过其间所 述域的流体产生一种集流效应, 所述域是其前面相邻翼的后凹面与后面相邻翼的前凸 面之间形成的空间, 并且所述相邻翼的后凹面、 前凸面是朝向上偏前方向; 通过设置 所述相邻翼之间的相对方位以增强所述集流效应, 增大流过所述域的流体的动能而提 高所述域后面相邻翼的升力, 从而提高由所述翼和所述域组成的整体多翼叶片的风能 利用系数。  A multi-wing collecting blade for efficiently utilizing wind energy, characterized in that it comprises a domain formed between at least two wings and at least one adjacent wing, by designing the shape of each of said wings and said domain, Having an adjacent pair of said wings create a current collecting effect on the fluid flowing through said domain therebetween, said domain being the space formed between the rear concave surface of the front adjacent wing and the front convex surface of the adjacent adjacent wing, and The rear concave surface and the front convex surface of the adjacent wings are oriented in an upwardly forward direction; the relative azimuth between the adjacent wings is provided to enhance the current collecting effect, and the kinetic energy of the fluid flowing through the domain is increased to increase The lift of adjacent wings behind the domain, thereby increasing the wind energy utilization factor of the overall multi-blade blade comprised of the wing and the domain.
2. 根据权利要求 1所述的多翼集流叶片, 其特征是所述的翼为 n个, 由 n个翼 ni (n 2、 i=l, 2, , η)和 η-1个由翼 ni与翼 nj之间的域 fij (j=i+l n、 i=l, 2, , n_l)构 成多翼叶片 Gn,通过所述 n个翼 ni和所述 n_l个翼 ni与翼 nj之间的所述域 fi j的形 状设计、 以及所述 n-1个翼 ni与翼 nj之间相对方位的设置, 所述域 f i j是翼 ni的后 凹面与翼 nj的前凸面之间形成的空间, 并且所述相邻翼的后凹面、 前凸面是朝向上偏 前方向; 使所述翼 ni将通过所述域 fi j的流体聚集流向所述翼 nj上表面的切线方向, 给所述翼 nj上表面的边界层提供更大的流体动能, 来减小层流分离而使所述翼 nj 的 升力增大, 从而提高了所述多翼叶片 Gn的风能利用系数 Cp; 通过调制所述翼 ni与所 述翼 nj之间的相对方位,控制所述翼 nj的升力值,进而控制所述多翼叶片 Gn的功率。 2. The multi-wing collecting blade according to claim 1, wherein said wings are n, and n wings ni (n 2, i = l, 2, , η) and η-1 The domain fij (j=i+ln, i=l, 2, , n_l) between the wing ni and the wing nj constitutes a multi-wing blade Gn through which the n wings ni and the n_l wings ni and the wing nj The shape design of the field fi j and the relative orientation between the n-1 wings ni and the wing nj, which is formed between the back concave surface of the wing ni and the front convex surface of the wing nj a space, and the rear concave surface and the front convex surface of the adjacent wing are oriented in an upwardly forward direction; causing the wing ni to concentrate fluid flow through the domain fi j to a tangential direction of the upper surface of the wing nj, The boundary layer of the upper surface of the wing nj provides greater fluid kinetic energy to reduce laminar flow separation and increase the lift of the wing nj, thereby increasing the wind energy utilization coefficient Cp of the multi-blade blade Gn; The relative orientation between the wing ni and the wing nj controls the lift value of the wing nj, thereby controlling the power of the multi-blade Gn.
3. 根据权利要求 1所述的多翼集流叶片, 其特征是所述的翼为 n个, 排头的翼 nl界定为 集流翼 C, 其余的翼 ni (i=2,……,n)构成子叶片 Dm (m=n-1), 集流域 F是集流翼 C与子 叶片 Dm之间的域, 它由集流翼 C的下表面和子叶片 Dm前缘上部之间的空间形成, 由 集流翼 C、 集流域 F和子叶片 Dm (m=n-1)构成多翼叶片 Gndm, 其中所述子叶片 Dm由 m 个翼 mi (m=n-l l、 i=l, 2, ,m)和 m_l个翼 mi与翼 mj之间的域 fij (j=i+l m、 i=l, 2,……, m-1)构成, 通过所述集流翼 C形状设计、 m个所述翼 mi形状设计和所述集 流域 F和 m-1个翼 mi与翼 mj之间的所述域 f i j的形状设计, 以及所述集流翼 C与翼 ml之间的相对方位、翼 mi与翼 mj之间的相对方位设置, 所述域 fi j是所述翼 mi的后 凹面与所述翼 mj的前凸面之间形成的空间, 并且所述相邻翼的后凹面、 前凸面是朝向 上偏前方向, 使集流翼 C将通过集流域 F的流体聚集流向翼 ml上表面的切线方向、 翼 mi将通过域 fij的流体聚集流向翼 mj上表面的切线方向, 给翼 mj上表面的边界层提 供更大的流体动能, 来减小层流分离而使翼 mj 的升力增大, 从而提高了叶片 Gndm的 风能利用系数 Cp; 通过调制集流翼 C相对于翼 ml所处的方位、翼 mi相对于翼 mj所处 的方位, 控制翼 mj的升力值, 进而控制叶片 Gndm的功率。 3. The multi-wing collecting blade according to claim 1, wherein said wing is n, the wing n1 of the head is defined as a collecting wing C, and the remaining wings ni (i=2, ..., n The sub-blade Dm (m=n-1) is formed, and the collecting basin F is a domain between the collecting wing C and the sub-blade Dm, which is formed by the space between the lower surface of the collecting wing C and the upper portion of the leading edge of the sub-blade Dm. , the multi-wing blade Gndm is constituted by the collecting wing C, the collecting basin F and the sub-blade Dm (m=n-1), wherein the sub-blade Dm is composed of m wings mi (m=nl l, i=l, 2, , m) and the domain fij (j=i+lm, i=l, 2, ..., m-1) between the m_l wing mi and the wing mj, through the shape of the collecting wing C, m The wing mi shape design and the shape design of the domain fij between the header F and m-1 wings mi and the wing mj, and the relative orientation between the collector wing C and the wing ml, the wing mi With respect to the relative orientation between the wings mj, the field fi j is a space formed between the rear concave surface of the wing mi and the front convex surface of the wing mj, and the rear concave surface and the front convex surface of the adjacent wing are Oriented In the upper direction, the collecting wing C flows the fluid through the collecting basin F to the tangential direction of the upper surface of the wing ml, and the wing mi flows the fluid passing through the domain fij to the tangential direction of the upper surface of the wing mj to the upper surface of the wing mj. The boundary layer provides greater fluid kinetic energy to reduce laminar flow separation and increase the lift of the wing mj, thereby increasing the wind energy utilization coefficient Cp of the blade Gndm; by modulating the orientation of the collecting wing C relative to the wing ml The direction of the wing mi relative to the wing mj controls the lift value of the wing mj, thereby controlling the power of the blade Gndm.
4. 根据权利要求 2或 3所述的多翼集流叶片, 其特征是以某种单翼 A的形状作为所述多 翼叶片 Gn或 Gndm的外轮廓。  The multi-wing collecting blade according to claim 2 or 3, characterized in that the shape of a certain single wing A is taken as the outer contour of the multi-blade blade Gn or Gndm.
5. 根据权利要求 3所述的多翼集流叶片, 其特征是以某种单翼 B的形状作为所述多翼叶 片 Gndm中的子叶片 Dm的外轮廓。  The multi-wing collecting blade according to claim 3, characterized in that the shape of a certain single wing B is taken as the outer contour of the sub-blade Dm in the multi-blade blade Gndm.
6. 根据权利要求 2或 4所述的多翼集流叶片, 其特征是所述多翼叶片 Gn中的所述 n个翼 的取值范围为 2 n 30。  The multi-wing collecting blade according to claim 2 or 4, characterized in that the n wings of the multi-blade Gn have a value range of 2 n 30 .
7. 根据权利要求 6所述的多翼集流叶片, 其特征是所述多翼叶片 Gn中的所述 n个翼的取 值范围为 2 n 5。  7. The multi-wing collecting blade according to claim 6, wherein said n wings of said multi-wing blade Gn have a value ranging from 2 n 5 .
8. 根据权利要求 3至 5任一所述的多翼集流叶片, 其特征是所述多翼叶片 Gndm中的所述 n个翼的取值范围为 2 n 5、 l m 4。  The multi-wing collecting blade according to any one of claims 3 to 5, characterized in that the n wings of the multi-wing blade Gndm have a value ranging from 2 n 5 to 1 m 4 .
9. 根据权利要求 3至 5任一所述的多翼集流叶片, 其特征是所述多翼叶片 Gndm中的所述 n个翼的取值范围为 6 n 15、 5 m 14。  9. A multi-wing collecting blade according to any one of claims 3 to 5, characterized in that said n wings of said multi-wing blade Gndm have a value in the range of 6 n 15 , 5 m 14 .
10.根据权利要求 3至 5任一所述的多翼集流叶片, 其特征是所述多翼叶片 Gndm中的所述 n个翼的取值范围为 16 n 30、 15 m 29。  The multi-wing collecting blade according to any one of claims 3 to 5, characterized in that said n wings of said multi-wing blade Gndm have a value ranging from 16 n 30 to 15 m 29 .
PCT/CN2012/076024 2012-05-17 2012-05-24 Multi-airfoil collecting blade capable of utilizing wind power efficiently WO2013170497A1 (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
CN201210152431.0 2012-05-17
CN201210152431.0A CN102661239B (en) 2012-05-17 2012-05-17 Multi-wing collecting vane capable of utilizing wind power efficiently

Publications (1)

Publication Number Publication Date
WO2013170497A1 true WO2013170497A1 (en) 2013-11-21

Family

ID=46770794

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/CN2012/076024 WO2013170497A1 (en) 2012-05-17 2012-05-24 Multi-airfoil collecting blade capable of utilizing wind power efficiently

Country Status (2)

Country Link
CN (1) CN102661239B (en)
WO (1) WO2013170497A1 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2548330A (en) * 2016-03-06 2017-09-20 Ian Pollington Bruce Vertical axis wind turbine
US10253753B2 (en) 2014-09-25 2019-04-09 Winfoor Ab Rotor blade for wind turbine
SE2050686A1 (en) * 2020-06-10 2021-12-11 Carlson Bjoern Vertical wind turbine

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR3011285B1 (en) 2013-09-30 2018-03-16 Electricfil Automotive ROTOR FOR WIND TURBINE IN PARTICULAR VERTICAL AXIS
CN106837684B (en) * 2015-12-10 2019-08-20 李亦博 Efficient vertical axis wind energy conversion system
CN106870277A (en) 2015-12-10 2017-06-20 李亦博 Efficiently using the blade and its manufacture method of low velocity fluid
WO2017097229A1 (en) * 2015-12-10 2017-06-15 李亦博 Blade capable of efficiently utilizing low velocity fluid, and application of blade
CN111188731B (en) * 2020-01-15 2021-06-04 河南科技大学 Vertical axis wind wheel with separation wing type lift-drag fusion of fish gill and fish belly cavity

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101400891A (en) * 2006-03-14 2009-04-01 泰克西斯先进技术及体系有限公司 Multi-element blade with aerodynamic profiles
US20100143152A1 (en) * 2009-06-30 2010-06-10 Balaji Subramanian Method and apparatus for increasing lift on wind turbine blade
CN101892945A (en) * 2010-07-13 2010-11-24 中国农业大学 Wind turbine blade
CN102116252A (en) * 2009-12-30 2011-07-06 通用电气公司 Method and apparatus for increasing lift on wind turbine blade
CN202065123U (en) * 2011-06-03 2011-12-07 秦皇岛风日和科技有限公司 Combined efficient vertical axis wind driven generator

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE2908761A1 (en) * 1979-03-06 1980-09-18 Hans Mueller Blade for wind-powered motor - has auxiliary pivoted flap, secondary blade or internal flow passages
GB2227286A (en) * 1989-01-17 1990-07-25 Howden Wind Turbines Limited Control of a wind turbine and adjustable blade therefor
DE4201457C1 (en) * 1992-01-21 1993-04-08 Alfred 4460 Nordhorn De Frohnert Wind converter vane with flow gap at nose - has gap controlled by centrifugal slider within vane front edge

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN101400891A (en) * 2006-03-14 2009-04-01 泰克西斯先进技术及体系有限公司 Multi-element blade with aerodynamic profiles
US20100143152A1 (en) * 2009-06-30 2010-06-10 Balaji Subramanian Method and apparatus for increasing lift on wind turbine blade
CN102116252A (en) * 2009-12-30 2011-07-06 通用电气公司 Method and apparatus for increasing lift on wind turbine blade
CN101892945A (en) * 2010-07-13 2010-11-24 中国农业大学 Wind turbine blade
CN202065123U (en) * 2011-06-03 2011-12-07 秦皇岛风日和科技有限公司 Combined efficient vertical axis wind driven generator

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10253753B2 (en) 2014-09-25 2019-04-09 Winfoor Ab Rotor blade for wind turbine
GB2548330A (en) * 2016-03-06 2017-09-20 Ian Pollington Bruce Vertical axis wind turbine
SE2050686A1 (en) * 2020-06-10 2021-12-11 Carlson Bjoern Vertical wind turbine
EP3922839A1 (en) * 2020-06-10 2021-12-15 Carlson, Björn Vertical wind power plant
SE544250C2 (en) * 2020-06-10 2022-03-15 Carlson Bjoern Vertical wind turbine

Also Published As

Publication number Publication date
CN102661239A (en) 2012-09-12
CN102661239B (en) 2014-09-24

Similar Documents

Publication Publication Date Title
WO2013170497A1 (en) Multi-airfoil collecting blade capable of utilizing wind power efficiently
Sagharichi et al. Effect of solidity on the performance of variable-pitch vertical axis wind turbine
Baker Features to aid or enable self starting of fixed pitch low solidity vertical axis wind turbines
US10443562B2 (en) Vortex generator for a wind turbine
CN103270296B (en) Wind turbine blade, wind power generation device provided with same, and design method for wind turbine blade
CN103089536B (en) Aileron surface on the stall fence on wind turbine blade
Yan et al. Aerodynamic performance improvements of a vertical axis wind turbine by leading-edge protuberance
EP2129908A2 (en) Wind turbine blades with vortex generators
CN104704233A (en) Swallow tail airfoil
CN104564804B (en) The design method of wind wheel blade and tubular wine wheel and wind wheel blade
CN207420779U (en) A kind of new blade of wind-driven generator vortex generator for being beneficial to installation
Mazarbhuiya et al. Low wind speed aerodynamics of asymmetric blade H-Darrieus wind turbine-its desired blade pitch for performance improvement in the built environment
Wang et al. Development of small domestic wind turbine with scoop and prediction of its annual power output
Ren et al. Influences of winglets on the hydrodynamic performance of horizontal axis current turbines
Mostafa et al. Quantitative impact of a micro-cylinder as a passive flow control on a horizontal axis wind turbine performance
CN104097770B (en) A kind of Helicopter Main rotor fin
Chen et al. Bionic coupling design and aerodynamic analysis of horizontal axis wind turbine blades
CN209192204U (en) Propeller and unmanned plane
Gui et al. Study on aerodynamic performance of mine air duct horizontal axis wind turbine based on breeze power generation
Frunzulica et al. Numerical investigations of passive flow control elements for vertical axis wind turbine
CN111502907B (en) Vortex generator, fan blade and wind driven generator comprising same
Manerikar et al. Horizontal axis wind turbines passive flow control methods: a review
Frunzulica et al. Numerical investigations of dynamic stall control
CN205858578U (en) A kind of R aerofoil profile root case blade construction design for promoting Wind turbines power
Radi et al. Optimal design of an horizontal axis wind turbine using blade element momentum theory

Legal Events

Date Code Title Description
121 Ep: the epo has been informed by wipo that ep was designated in this application

Ref document number: 12876799

Country of ref document: EP

Kind code of ref document: A1

NENP Non-entry into the national phase

Ref country code: DE

122 Ep: pct application non-entry in european phase

Ref document number: 12876799

Country of ref document: EP

Kind code of ref document: A1