Rotor blade of a wind turbine and method for designing same

Information

  • Patent Grant
  • 11428204
  • Patent Number
    11,428,204
  • Date Filed
    Tuesday, October 23, 2018
    5 years ago
  • Date Issued
    Tuesday, August 30, 2022
    2 years ago
Abstract
A two-part or multi-part rotor blade and also to a method which is associated with it. The rotor blade is split into at least one rotor blade component which is close to the hub and one rotor blade component which is remote from the hub at a separation point in the longitudinal direction, wherein the rotor blade component which is close to the hub and the rotor blade component which is remote from the hub can be connected at the separation point for operation of the wind turbine. A ratio of profile thickness to profile depth, called relative thickness, at the separation point lies within a range of from 0.4 to 0.5. An improved two-part or multi-part rotor blade in spite of the unexpectedly high relative thicknesses.
Description
BACKGROUND
Technical Field

The present invention relates to a rotor blade of a wind turbine and to a method for designing a rotor blade of a wind turbine. The present invention relates, in particular, to a two-part or multi-part rotor blade and to a method which is associated with it.


Description of the Related Art

Rotor blades for wind turbines are known. In the past, one-piece, unsplit rotor blades were used for the most part but these are gradually reaching limits, in particular in respect of transportation, owing to ever-increasing dimensions.


For this reason, manufacture of split rotor blades, which are easier to transport than unsplit blades and are assembled by a fitter at the site of erection, has begun. Split rotor blades present some challenges in terms of design and construction of the rotor blades since, amongst other things, ease of assembly at the site of erection but also the blade dimensions, which are increased owing to the connection point, and therefore the additional loads to be expected on the turbine in comparison to a one-part design have to be taken into consideration.


BRIEF SUMMARY

Provided is a split rotor blade which may minimize the consequences of the known disadvantages and difficulties encountered with split rotor blades.


Provided is a rotor blade of a wind turbine, wherein the rotor blade is split into at least one rotor blade component which is close to the hub and one rotor blade component which is remote from the hub at a separation point in the longitudinal direction, wherein the rotor blade component which is close to the hub and the rotor blade component which is remote from the hub can be connected at the separation point for operation of the wind turbine, wherein a ratio of profile thickness to profile depth, called relative thickness, at the separation point lies within a range of from 0.4 to 0.5.


The relative thickness within a range of from 0.4 to 0.5 at the separation point constitutes an unexpectedly high value. An advantageous blade can ultimately be expected in spite of the high value of the relative thickness. From an aerodynamic point of view, profiles with high relative thicknesses are specifically disadvantageous since they firstly have poorer lift/drag ratios than profiles with a lower relative thickness and secondly also have lower lift coefficients in general. However, this effect, which is disadvantageous from an aerodynamic point of view, is compensated for in that the profiles with higher relative thicknesses are associated with structural advantages which allow, in particular, a lighter-weight construction of the rotor blade. A particularly advantageous combination of aerodynamically effective blade and comparatively low turbine loads for rotor blades which are split into two can be achieved owing to the range of from 0.4 to 0.5 selected.


The relative thickness at the separation point particularly preferably lies within a range of from 0.42 to 0.46. It has been found that particularly efficient rotor blades which are split into two can be realized within this range of values in particular.


In one embodiment, a sum of the lengths of the rotor blade component which is close to the hub and the rotor blade component which is remote from the hub, which rotor blade components are connected at the separation point, gives a blade length of the rotor blade, wherein the separation point is located in a region of from 25% to 38% of the blade length as viewed from the hub, in particular in a region of from 27% to 33% of the blade length as viewed from the hub.


The separation point is always associated with a higher local weight than the surrounding points of the rotor blade. For this reason, it would actually be desirable to place the separation point as close to the rotor hub as possible. However, as a result of this, the advantages of a two-part or multi-part rotor blade are canceled out, specifically the advantages in respect of transportation in particular. In the ideal case, this would mean providing the separation point in the region of 50% of the blade length. It has been found that providing the separation point in the narrow region between 25% and 38% of the blade length, in particular between 27% and 33% of the blade length, as a compromise between the mass distribution of the rotor blade that is established and the utilization of the advantages of a two-part or multi-part rotor blade is particularly effective.


In one embodiment, an absolute thickness of the rotor blade at the separation point is at least 1.70 m.


Since the absolute thickness of the rotor blade at the separation point is at least 1.70 m, it is possible for a fitter to reach the separation point within the rotor blade and to connect the two rotor blade components to one another at the separation point. The requirement in respect of the absolute thickness at the separation point together with the position of the separation point and the relative thickness at the separation point lead to a rotor blade which can be implemented within the generally known transportation limitations. In particular, a rotor blade which is designed in this way does not lead to a profile depth which is associated with difficulties in respect of transportation.


In one embodiment, a mean relative thickness between a first position of the relative blade length and a second position of the relative blade length is defined as a ratio of the definite integral of the relative thickness from the first position to the second position to a distance between the first position and the second position.


The mean relative thickness of from 20% to 30% of the relative blade length is preferably at least 0.460.


As an alternative or in addition, the mean relative thickness of from 20% to 50% of the relative blade length is preferably at least 0.390.


As an alternative or in addition, the mean relative thickness of from 20% to 70% of the relative blade length is preferably at least 0.33, in particular at least 0.35.


It has been found that, in particular, the region which is close to the hub of from 0% to 20% of the blade length can be designed substantially uninfluenced by the design as a two-part or multi-part rotor blade. However, in the region starting from 20%, in particular up to 30 or 50 or 70% of the relative blade length, the mean relative thickness assumes a considerably higher value than was the case in known rotor blades, in particular in known one-part rotor blades. In other words, the relative thickness, which is already excessively high at the separation point, in the range of from 0.4 to 0.5 is evident over a further region of the rotor blade, so that an extraordinarily high relative thickness prevails over further regions of the rotor blade.


An advantageous blade can ultimately be expected in spite of the high value of the relative thickness. From an aerodynamic point of view, profiles with high relative thicknesses are specifically disadvantageous since they firstly have poorer lift/drag ratios than profiles with a lower relative thickness and secondly also have lower lift coefficients in general. However, this effect, which is disadvantageous from an aerodynamic point of view, is compensated for in that the aerodynamic disadvantages which are associated with a higher relative thickness in rotor blades which are split into two are balanced out by the structural advantages which are obtained at the same time. This is achieved, in particular, in that the mass of the outer blade can be kept low owing to the higher relative thickness.


In one embodiment, a structural dimensionless parameter is defined as the definite integral of the relative thickness over a region of the relative blade length, wherein a lower limit of the integral is defined at a position of 20% of the blade length and the structural dimensionless parameter can be evaluated for any desired values of the upper limit.


The structural dimensionless parameter for an upper limit of 45% of the blade length is preferably at least 0.1.


As an alternative or in addition, the structural dimensionless parameter for an upper limit of 80% of the blade length is preferably at least 0.2.


As an alternative or in addition, the structural dimensionless parameter for the upper limit of 45% of the blade length is preferably at most 0.12.


As an alternative or in addition, the structural dimensionless parameter for the upper limit of 80% of the blade length is preferably at most 0.24.


The structural dimensionless parameter which is defined in this way has been found to be particularly suitable for compensating for the high mass of the inner blade, including the separation point, over the further blade course, without having a negative influence on the turbine loads. If the structural dimensionless parameter is kept within the preferred range when designing the rotor blade, a two-part or multi-part rotor blade of particularly optimum design is accordingly obtained as a result.


Provided is a wind turbine comprising at least one rotor blade according to the invention. The wind turbine is also improved owing to the use of the rotor blades according to the invention. In particular, the advantageous refinements of the rotor blades according to the invention can also be analogously applied to the wind turbine.


Provided is a wind farm comprising a plurality of wind turbines according to the invention. The plurality of wind turbines according to the invention assist in optimizing the wind farm. In particular, the advantageous refinements of the rotor blades and wind turbines according to the invention can also be analogously applied to the wind farm.


Provided is a method for designing a rotor blade of a wind turbine. The rotor blade is split into at least one rotor blade component which is close to the hub and one rotor blade component which is remote from the hub at a separation point in the longitudinal direction, wherein the rotor blade component which is close to the hub and the rotor blade component which is remote from the hub can be connected at the separation point for operation of the wind turbine. The method comprises a step of defining a ratio of profile thickness to profile depth, called relative thickness, at the separation point within a range of from 0.4 to 0.5, in particular within a range of from 0.42 to 0.46.


The method allows the same advantages to be achieved as are achieved by the rotor blade according to the invention. In particular, carrying out the method according to the invention leads to a rotor blade according to the invention. The preferred refinements of the embodiments of the rotor blade can also be transferred to the method in an analogous manner.


In one embodiment of the method, for the purpose of designing the rotor blade, a trade-off is made between a structurally necessary higher relative thickness at the separation point and an aerodynamically desired lower relative thickness at the separation point on the basis of a mean relative thickness, wherein the mean relative thickness between a first position of the relative blade length and a second position of the relative blade length is defined as a ratio of the definite integral of the relative thickness from the first position to the second position to a distance between the first position and the second position.


The mean relative thickness of from 20% to 30% of the relative blade length is preferably at least 0.460.


As an alternative or in addition, the mean relative thickness of from 20% to 50% of the relative blade length is preferably at least 0.390.


As an alternative or in addition, wherein the mean relative thickness of from 20% to 70% of the relative blade length is preferably at least 0.33, in particular at least 0.35.


In one embodiment of the method, for the purpose of designing the rotor blade, a trade-off is made between a structurally necessary higher relative thickness at the separation point and an aerodynamically desired lower relative thickness at the separation point on the basis of a structural dimensionless parameter, wherein the structural dimensionless parameter is defined as the definite integral of the relative thickness over a region of the relative blade length, wherein a lower limit of the integral is defined at a position of 20% of the blade length and the structural dimensionless parameter can be evaluated for any desired values of the upper limit.


The structural dimensionless parameter for an upper limit of 45% of the blade length is preferably at least 0.1.


As an alternative or in addition, the structural dimensionless parameter for an upper limit of 80% of the blade length is preferably at least 0.2.


As an alternative or in addition, the structural dimensionless parameter for the upper limit of 45% of the blade length is preferably at most 0.12.


As an alternative or in addition, the structural dimensionless parameter for the upper limit of 80% of the blade length is preferably at most 0.24.





BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS

Further advantages and preferred refinements will be described more precisely below with reference to the exemplary embodiments of the appended figures, in which:



FIG. 1 shows, schematically and by way of example, a wind turbine,



FIG. 2 shows, schematically and by way of example, curves of relative blade thicknesses of rotor blades,



FIG. 3 shows, schematically and by way of example, curves of a structural dimensionless parameter over the blade length, which is standardized with the maximum rotor blade length, of rotor blades, and



FIG. 4 shows, schematically and by way of example, curves of a mean relative thickness over the blade length, which is standardized with the maximum rotor blade length, of rotor blades.





DETAILED DESCRIPTION


FIG. 1 shows a wind turbine 100 comprising a tower 102 and a nacelle 104. A rotor 106 with three rotor blades 108 and a spinner 110 is arranged on the nacelle 104. During operation, the rotor 106 is set in rotary motion by the wind and thereby drives a generator in the nacelle 104. The spinner 110 encases a rotor hub (not shown) of the rotor 106.


The rotor blades 108 are each split into two and have a separation point 109 which separates a rotor blade component which is close to the hub from a rotor blade component which is remote from the hub. In other examples, rotor blades 108 which are split into more than two, for example, which are split into three or which are split into four, and have more than one separation point are equally conceivable.


Split rotor blades 108 are easier to transport than unsplit rotor blades 108 and furthermore also provide advantages with respect to production, for example, by using winding techniques. However, one known disadvantage of split rotor blades 108 is the generally higher blade mass than the unsplit rotor blades 108 of similar dimensions. The shown rotor blades 108, which are split into two, accordingly generally lead to higher loads on the wind turbine 100.


For assembly purposes, the rotor blade component, which is close to the hub and the rotor blade component, which is remote from the hub are, for example, screwed together at the separation point 109 on the inside of the blade at the site of erection. In order that this can be ensured by a fitter, the thickness of the rotor blade 108 at the separation point 109 is, for example, at least 1.70 m. Other connection concepts can accordingly be provided given smaller thicknesses at the separation point 109.


For optimum distribution of the loads, the separation point 109 would have a cylindrical profile with a relative thickness in the region of 1. However, since the separation point 109 lies in a region of the rotor blade 108, in particular in a region of from 25 to 38% of the blade length, at which considerable effects on the yield can already be detected, profiling should be performed. Accordingly, for aerodynamic reasons, the relative thickness of the profiling at the separation point 109, that is to say the ratio of blade thickness to blade depth at the separation point 109, should be as low as possible. However, a low relative thickness in the region of the separation point 109 would, as directly follows from the definition of the relative blade thickness, lead to high blade depths at the separation point 109, which would in turn have a disadvantageous effect both on turbine loads and on the transportation of the rotor blades 108.


It has been found to be particularly preferable to define the separation point at a relative thickness in the range of from 0.4 to 0.5, in particular of from 0.42 to 0.46. This allows a rotor blade to be obtained which takes into account both the loads to be expected and the aerodynamic efficiency but also the mass of the rotor blade 108 as a whole in an appropriate manner.


In comparison to one-part rotor blades, this results, in particular owing to the separation point 109, in relatively high thicknesses in that region of the rotor blade 108 which is close to the hub.



FIG. 2 shows, schematically and by way of example, a curve 210 of the relative blade thickness of a rotor blade 108 which is split into two. For comparison, the same figure illustrates a curve 220 of the relative blade thickness of a known one-part rotor blade as a line. It can be seen that the relative thickness curve 210 lies above the relative thickness curve 220 over a wide course of the rotor blade length. This means that the rotor blade 108 which is split into two has a higher relative thickness than known rotor blades over a wide course in order to keep the mass of the outer blade low and thereby to compensate for the high mass of the inner blade, including the separation point 109, as far as possible and to keep the total mass of the rotor blade 108 in respect of the turbine loads as low as possible.


A region of the separation point 109 is indicated by an arrow 230. In the region of the rotor hub, which region is identified by an arrow 240, the known thickness curve 220 has a circular-cylindrical profile which can be established from the relative thickness of 1. Further profile curves 220, which do not have a circular-cylindrical shape in the hub region 240, are likewise known. However, in comparison to the rotor blade 108, all of the known rotor blades and, respectively, their thickness curves 220 have, in the region of the separation point 230, that is to say particularly between 25% and 38% of the rotor blade length, relative thicknesses which lie considerably below the thickness curve 210.


In FIG. 2 and also further FIGS. 3 and 4, the standardized rotor blade radius, that is to say a position in the longitudinal direction of the rotor blade starting from the hub, which position has been standardized with the length of the rotor blade, is plotted on the horizontal axis.


Therefore, balancing out the aerodynamically critical profiles with high relative thicknesses in relation to the structurally advantageous thickness profiles is achieved. This is particularly difficult owing to the separation point 109, in particular in the case of rotor blades 108 which are split into two or more parts. To achieve this, provided is a dimensionless parameter F which corresponds substantially to an integral of the relative thickness:






F
=




x

1


x

2





d
t


d

x






Here, d is the thickness of the rotor blade 108 at a relative position






x
=

r
R






and t is the local profile depth at the point x.


The curve of the dimensionless parameter F is schematically shown for several different rotor blades in FIG. 3. Here, the value 0.2 has proven particularly advantageous as the lower integral limit x1. Here, a curve 310 of the dimensionless parameter F corresponds to the curve which is calculated for a rotor blade 108, while a curve 320 corresponds to a comparison curve of a known one-part rotor blade. It can be seen that the dimensionless parameter F for the rotor blade 108 assumes a higher value than is the case for the known one-part rotor blades. It should be noted that only relative variables which are not provided with units are then used for calculating the dimensionless parameter. It goes without saying that other dimensionless parameters which take into account the characteristic curve of the rotor blades 108 can also be used as an alternative.


A further example is shown in FIG. 4 in which the mean relative thickness for various rotor blades is plotted with respect to the relative blade position. Here, a curve 410 likewise corresponds to an exemplary curve of the mean relative thickness of a rotor blade 108, while a curve 420 represents a known, one-part rotor blade by way of example. The mean relative thickness of the rotor blade lies considerably above the curve 420 of the known rotor blades over the entire plotted region. In other words, the curve 410 is always higher than the curve 420 of the known one-part rotor blade designs in the middle region of the blade between 0.2 and 0.8 of the relative blade length.


In this example, the mean relative blade thickness for the region starting from 0.2 of the relative blade radius is determined. That is to say, the range of from 0.2 up to the value which is plotted on the horizontal is determined. For calculation purposes, for example, the dimensionless parameter F can be formed with the lower limit x1=0.2 and the result can be divided by the distance of the examined value from 0.2. It goes without saying that other ranges which do not necessarily begin at 0.2 can also be used for assessing the mean relative thickness. Therefore, for example, a range from 0.1 or else from 0.3 of the relative blade radius can also be examined.

Claims
  • 1. A rotor blade of a wind turbine, comprising: a first rotor blade component that is close to a hub when mounted on a wind turbine, and a second rotor blade component that is remote from the hub, wherein the first and second rotor blade components are separable at a separation point in a longitudinal direction of the rotor blade,wherein a ratio of a profile thickness to a profile depth, called relative thickness, at the separation point is within a range from 0.4 to 0.5,wherein a sum of lengths of the first rotor blade component and the second rotor blade component provides a total blade length of the rotor blade, andwherein the separation point is located in a region from 25% to 38% of the total blade length as referenced from the hub.
  • 2. The rotor blade as claimed in claim 1, wherein an absolute thickness of the rotor blade at the separation point is at least 1.7 meters.
  • 3. The rotor blade as claimed in claim 1, wherein a mean relative thickness between a first position of a relative blade length and a second position of the relative blade length is defined as a ratio of a definite integral of the relative thickness from the first position to the second position to a distance between the first position and the second position, wherein the mean relative thickness from 20% to 30% of the relative blade length is at least 0.460.
  • 4. The rotor blade as claimed in claim 1, wherein: a structural dimensionless parameter is defined as a definite integral of a relative thickness over a region of a relative blade length, wherein a lower limit of the integral is defined at a position of 20% of the total blade length and the structural dimensionless parameter is evaluated for any desired values of an upper limit, andthe structural dimensionless parameter for an upper limit of 45% of the total blade length is at least 0.1.
  • 5. The rotor blade as claimed in claim 4, wherein the structural dimensionless parameter for the upper limit of 45% of the blade length is at most 0.12.
  • 6. A wind turbine comprising: a hub; andat least one rotor blade as claimed in claim 1, wherein the first rotor blade component of the at least one rotor blade is coupled to the hub.
  • 7. A wind farm comprising a plurality of wind turbines as claimed in claim 6.
  • 8. A method of forming a rotor blade of a wind turbine, the method comprising: coupling a first rotor blade component to a second rotor blade component at a connection point, wherein the first rotor blade component is close to a hub when the rotor blade is mounted to the wind turbine, wherein the second rotor blade component is remote from the hub, wherein the connection point is at a separation point in a longitudinal direction of the rotor blade,wherein a ratio of a profile thickness to a profile depth, called relative thickness, at the separation point is defined within a range of from 0.4 to 0.5,wherein a sum of lengths of the first rotor blade component and the second rotor blade component provides a total blade length of the rotor blade, andwherein the separation point is located in a region from 25% to 38% of the total blade length as referenced from the hub.
  • 9. The method as claimed in claim 8, wherein: a mean relative thickness between a first position of the relative blade length and a second position of a relative blade length is defined as a ratio of a definite integral of the relative thickness from the first position to the second position to a distance between the first position and the second position, andthe mean relative thickness of from 20% to 30% of the relative blade length is at least 0.460.
  • 10. The method as claimed in claim 8 wherein: a structural dimensionless parameter is defined as a definite integral of the relative thickness over a region of a relative blade length, wherein a lower limit of the integral is defined at a position of 20% of the total blade length and the structural dimensionless parameter is evaluated for any desired values of an upper limit, andthe structural dimensionless parameter for an upper limit of 45% of the total blade length is at least 0.1.
  • 11. The method as claimed in claim 10, wherein the structural dimensionless parameter for the upper limit of 45% of the total blade length is at most 0.12.
  • 12. The method as claimed in claim 11, wherein the structural dimensionless parameter for an upper limit of 80% of the total blade length is at most 0.24.
  • 13. The method as claimed in claim 9, wherein a mean relative thickness from 20% to 50% of the relative blade length is at least 0.390.
  • 14. The method as claimed in claim 8, wherein the ratio at the separation point is within a range from 0.42 to 0.46.
  • 15. The rotor blade as claimed in claim 1, wherein the ratio at the separation point is within a range from 0.42 to 0.46.
  • 16. The rotor blade as claimed in claim 1, wherein the separation point is located in a region from 27% to 33% of the total blade length.
  • 17. The rotor blade as claimed in claim 3, wherein a mean relative thickness of from 20% to 50% of the relative blade length is at least 0.390.
  • 18. The rotor blade as claimed in claim 4, wherein the structural dimensionless parameter for an upper limit of 80% of the total blade length is at least 0.2.
  • 19. The rotor blade as claimed in claim 18, wherein the structural dimensionless parameter for the upper limit of 80% is at most 0.24.
Priority Claims (1)
Number Date Country Kind
10 2017 124 861.7 Oct 2017 DE national
PCT Information
Filing Document Filing Date Country Kind
PCT/EP2018/079039 10/23/2018 WO
Publishing Document Publishing Date Country Kind
WO2019/081510 5/2/2019 WO A
US Referenced Citations (81)
Number Name Date Kind
1403069 Burne Jan 1922 A
2400388 Campbell May 1946 A
2428936 Hunter Oct 1947 A
2442783 Senn Jun 1948 A
2453403 Bogardus Nov 1948 A
2465007 Bragdon et al. Mar 1949 A
2485543 Andreau Oct 1949 A
2616509 Thomas Nov 1952 A
2622686 Chevreau et al. Dec 1952 A
2934150 Fink Apr 1960 A
3184187 Isaac May 1965 A
3463420 Butler et al. Aug 1969 A
3874816 Sweeny et al. Apr 1975 A
3987984 Fischer Oct 1976 A
4247253 Seki et al. Jan 1981 A
4274011 Garfinkle Jun 1981 A
4408958 Schacle Oct 1983 A
4419053 Swearingen, Jr. Dec 1983 A
4498017 Parkins Feb 1985 A
4519746 Wainauski et al. May 1985 A
4613760 Law Sep 1986 A
4668169 Perry May 1987 A
4692095 Lawson-Tancred Sep 1987 A
4699568 Harlamert et al. Oct 1987 A
4732542 Hahn et al. Mar 1988 A
4773824 Kiss Sep 1988 A
4773825 Rodde et al. Sep 1988 A
4830574 Wainauski et al. May 1989 A
4858852 Henne Aug 1989 A
4976587 Johnston et al. Dec 1990 A
5096378 Jamieson Mar 1992 A
5106265 Holzem Apr 1992 A
5320491 Coleman et al. Jun 1994 A
5417548 Tangier et al. May 1995 A
5474415 Becker et al. Dec 1995 A
5474425 Lawlor Dec 1995 A
5527151 Coleman et al. Jun 1996 A
5562420 Tangler et al. Oct 1996 A
5570859 Quandt Nov 1996 A
5570997 Pratt Nov 1996 A
6015115 Dorsett et al. Jan 2000 A
6068446 Tangier et al. May 2000 A
6133716 Schutten Oct 2000 A
6420795 Mikhail et al. Jul 2002 B1
6465902 Beauchamp et al. Oct 2002 B1
6503058 Selig et al. Jan 2003 B1
6523781 Ragner Feb 2003 B2
6682302 Noble Jan 2004 B2
6899523 Wobben May 2005 B2
6951443 Blakemore Oct 2005 B1
7204674 Wobben Apr 2007 B2
7357624 Wobben Apr 2008 B2
D584686 Gudewer Jan 2009 S
7708530 Wobben May 2010 B2
7946803 Wobben May 2011 B2
8172539 Kootstra May 2012 B2
8348622 Bech Jan 2013 B2
8403642 Carroll et al. Mar 2013 B2
8668462 Fischer et al. Mar 2014 B2
8678770 Enevoldsen Mar 2014 B2
8777573 Hibbard et al. Jul 2014 B2
8814525 Petsche et al. Aug 2014 B2
8894374 Fuglsang Nov 2014 B2
8911214 Fukami Dec 2014 B2
9759185 Bohlen Sep 2017 B2
9932960 Petsche et al. Apr 2018 B2
10125741 Hayden Nov 2018 B2
20030099546 Stiesdal et al. May 2003 A1
20040105752 Wobben Jun 2004 A1
20040115057 Wobben Jun 2004 A1
20070297896 Wobben Dec 2007 A1
20070297909 Wobben Dec 2007 A1
20080069699 Bech Mar 2008 A1
20100196166 Enevoldsen et al. Aug 2010 A1
20110135486 Bendel Jun 2011 A1
20110150664 Mickeler et al. Jun 2011 A1
20110293432 Hibbard et al. Dec 2011 A1
20120020803 Lees Jan 2012 A1
20120280509 Fukami Nov 2012 A1
20130115098 Madsen et al. May 2013 A1
20150064017 Bohlen Mar 2015 A1
Foreign Referenced Citations (46)
Number Date Country
2778548 Dec 2012 CA
101059119 Oct 2007 CN
102003332 Apr 2011 CN
103168172 Jun 2013 CN
3126677 Jan 1983 DE
3913505 Nov 1989 DE
4002972 Aug 1991 DE
4428731 Feb 1996 DE
4435606 Apr 1996 DE
19719221 Oct 1998 DE
69415292 Jul 1999 DE
69513871 Jul 2000 DE
19963086 Jun 2001 DE
10307682 Jan 2004 DE
10319246 Dec 2004 DE
102008033411 Mar 2009 DE
102008052858 Apr 2010 DE
102011050901 Dec 2011 DE
102012109170 Mar 2013 DE
102012206109 Sep 2013 DE
102013202666 Aug 2014 DE
0283730 Sep 1988 EP
0375382 Jun 1990 EP
1978245 Oct 2008 EP
2339171 Jun 2011 EP
2366891 Sep 2011 EP
908631 Apr 1946 FR
2290585 Jun 1976 FR
2587675 Mar 1987 FR
2311978 Oct 1997 GB
55-153870 Dec 1980 JP
S61140181 Aug 1986 JP
5-180146 Jul 1993 JP
2359151 Jun 2009 RU
577300 Nov 1977 SU
1539378 Jan 1990 SU
0073651 Dec 2000 WO
0155590 Aug 2001 WO
0183983 Nov 2001 WO
02051730 Jul 2002 WO
03104646 Dec 2003 WO
2010048958 May 2010 WO
2010086297 Aug 2010 WO
2012007058 Jan 2012 WO
2012164305 Dec 2012 WO
WO-2013075718 May 2013 WO
Non-Patent Literature Citations (3)
Entry
Björck, A., “Coordinates and Calculations for the FFA-W1-xxx, FFA-W2-xxx and FFA-W3-xxx Series of Airfoils for Horizontal Axis Wind Turbines,” The Aeronautical Research Institute of Sweden, 1990, 150 pages, Stockholm, Sweden.
Timmer et al., “Thick Airfoils for HAWTs,” Journal of Wind Engineering and Industrial Aerodynamics, vol. 39, Amsterdam, Netherlands, 1992, pp. 151-160.
“Wortmann FX 77-W-343(FX77W343,Contour Data)”, Nihon University Aero Student Group, NASG Airfoil Database, XP002253850, http://www.nasg.com/afdb/show-airfoil-e.phtml?id=338, download date of Oct. 2, 2006.
Related Publications (1)
Number Date Country
20200248671 A1 Aug 2020 US