FIELD OF THE INVENTION
The invention relates to methods and apparatus for reducing aerodynamic loads on wind turbine blades, and particularly to reducing negative lift during gusts.
BACKGROUND OF THE INVENTION
Negative lift is produced by a wind turbine blade airfoil at negative angles of attack. When the blade is operating at a low or zero positive angle of attack, gusts can abruptly alternate the lift between negative and positive, resulting in high stress and fatigue on the blade, rotor, and tower. When this occurs on the radially outer portion of the blade it can cause rapidly alternating flexing of the blade, especially when operating in maximum winds with turbulence. One way to reduce or eliminate negative lift is to stall the pressure side of the blade at negative angles of attack using a pressure side stall strip, as taught in U.S. Pat. No. 8,602,739 issued to the present assignee. However, a stall strip can add undesirable drag under some operating conditions. This is addressed by the present invention.
BRIEF DESCRIPTION OF THE DRAWINGS
The invention is explained in the following description in view of the drawings that show:
FIG. 1 is a transverse sectional profile of a prior art wind turbine blade airfoil.
FIG. 2 is a partial transverse profile of a wind turbine blade airfoil with a pressure side stall strip in an incident wind stagnation zone.
FIG. 3 shows the apparatus of FIG. 2 close to zero angle of attack.
FIG. 4 shows of the apparatus of FIG. 2 at a negative angle of attack.
FIG. 5 shows the apparatus of FIG. 2 at increased positive angle of attack.
FIG. 6 shows a stall strip with forward and aft concave sides.
FIG. 7 shows a stall strip with forward concave side and aft convex side.
FIG. 8 is a graph of coefficient of lift versus angle of attack, with and without a pressure side stall strip.
FIG. 9 is a profile of a pressure side of a radially outer portion of a wind turbine blade.
FIG. 10 shows an exemplary transverse sectional profile of a stall strip.
DETAILED DESCRIPTION OF THE INVENTION
FIG. 1 shows a transverse sectional profile of a wind turbine blade 20 with a leading edge LE, trailing edge TE, pressure side PS, and suction side SS. The blade rotates in a rotation direction R in a plane of rotation 21, which results in a relative wind vector RW if the ambient wind is zero. Adding the ambient wind vector AW produces a resultant incident wind vector IW, which defines an angle of attack a between the incident wind vector and the chord line CL. The pitch angle θ is set such that the rotor rotates at a desired blade tip speed and angle of attack suitable for the wind conditions. During normal operation, the incident wind impinges on a forward portion of the pressure side of the airfoil near the leading edge and spreads forward and aft from the line of impingement. This creates a stagnation zone 22 along the line of impingement.
FIG. 2 shows a partial airfoil profile 20 with a stall strip 24A in the stagnation zone 22 that occurs at the angle of attack a resulting from a predetermined nominal operating condition. This angle of attack may provide a desired blade tip speed ratio for an operating condition such as 5 to 10% below maximum power or at a minimum ambient condition for rated power. Locating the stall strip 24A in the stagnation zone eliminates drag from the stall strip in this operating condition. The chordwise position of the stagnation zone may vary over the span of the blade. This position can be determined with computational fluid dynamics for a given blade design. The stall strip may be positioned and aligned to stay within the stagnation zone at the predetermined nominal operating condition. Since there is no drag penalty, the stall strip can be taller than in the prior art, and thus more effective at stalling the pressure side of the airfoil at negative angles of attack.
FIG. 3 shows the airfoil 20 with a reduced angle of attack, for example close to zero angle of attack during operation at higher than nominal wind speeds. In this condition, the stall strip 24A is aft of the stagnation zone 22. A stable bubble of recirculating flow 26 forms behind the stall strip. This does not cause flow separation from the pressure side of the airfoil. Instead it provides a fairing effect that enables the flow to continue without separating. Drag caused by the stall strip in such high wind condition can be beneficial in limiting the blade rotation speed.
FIG. 4 shows the airfoil 20 at a negative angle of attack at which the angle of airflow over the stall strip has burst the recirculation bubble of FIG. 3, causing separation 27 of the airflow over the pressure side, and thus reducing negative lift. The angle of attack at which this instability occurs is controllable by the position, size, and sectional shape of the stall strip as later described.
FIG. 5 shows the airfoil 20 with an increase in angle of attack over FIG. 2. The stagnation zone 22 is now aft of the stall strip 24A. The stall strip may be positioned and shaped to contain a bubble of recirculating air flow 28 on a forward side of the stall strip at angles of attack greater than the nominal angle of attack at the predetermined operating condition up to a maximum operating angle of attack or up to another predetermined angle of attack such as 15 degrees. The forward flow over the stall strip flows over the recirculation bubble 28 and re-attaches to the airfoil boundary layer.
FIG. 6 shows a stall strip 24B with concave sides. A concave side aids in forming and maintaining a stable recirculation bubble 28. This shape may be beneficial on either or both of the forward and aft sides of the stall strip to maintain laminar flow except when the angle of attack is below a desired minimum, below which the aft recirculation bubble 26 (FIG. 3) bursts, reducing negative lift. This reduces alternating flapwise strains in gusty conditions. “Flapwise” means bending in a plane normal to the chord and normal to the span of the blade.
FIG. 7 shows a stall strip 24C with a concave forward side and a convex aft side. A concave forward side aids in forming and maintaining a stable forward recirculation bubble 28 under the conditions shown. The convex aft side encourages aft vortex shedding when the stagnation point moves forward of the strip. Vortices and waves shed by the stall strips herein are unlike the vortices created by vortex generators designed to delay flow separation. Vortices shed by stall strips are oriented spanwise. They encourage flow separation, while vortex generators create vortices that are oriented chordwise.
FIG. 8 is a graph that compares function curves of lift coefficient CL versus angle of attack a for an unmodified airfoil 32 and a modified airfoil 34 with a pressure side stall strip as taught herein for an exemplary wind turbine blade design. The stall strip may be positioned and shaped to create airflow separation at a particular negative angle of attack 36 or negative lift coefficient 38.
FIG. 9 illustrates a stall strip 24 disposed on a pressure side PS of a wind turbine blade airfoil 20. The stall strip may stay within the stagnation zone over at least 15% of the span of the blade for example. The chordwise position of the stagnation zone may vary along the span 39 of the stall strip. For example the chordwise position of the stall strip may vary within a range of 1%-25% of the chord, for example between 1% and 5%, along most of the outer 30% of the blade span. “Blade span” means the distance from the blade root to tip 40. “Chordwise position” means the distance from the leading edge along the chord line as a percentage of the chord length. In the example shown, the chordwise position of the stagnation zone increases with radial position along the outer 30% of the blade. The stagnation zone may follow a line or curve, depending on the particular blade design and the chosen nominal operation condition.
FIG. 10 illustrates a triangular cross section of a stall strip having a height H, a base B, an apex angle Ø, and optionally an axis of symmetry 42. Exemplary sectional profiles may be triangular or substantially triangular in some embodiments. For example, the triangle height may be 1-20 mm, and the included angle may be 45-150 degrees. Other shapes such as concave/convex triangles as previously shown, fences, or other forms may be used.
In a method of the invention, a nominal operating condition is selected, such as one that produces less than maximum power, and a stall strip is placed within the pressure side stagnation zone that occurs during that condition. This placement eliminates drag from the stall strip at the nominal operating condition. By sizing and shaping the stall strip as described herein, a bubble of recirculating airflow is maintained on the forward and aft sides of the stall strip under respectively greater and lesser angles of attack until a predetermined negative angle of attack or negative coefficient of lift is reached. Then the stall strip separates the airflow on the pressure side of the airfoil. This reduces structural fatigue and maximum stress on the blade, the rotor shaft, and the tower, with no significant performance penalty.
While various embodiments of the present invention have been shown and described herein, it will be obvious that such embodiments are provided by way of example only. Numerous variations, changes and substitutions may be made without departing from the invention herein. Accordingly, it is intended that the invention be limited only by the spirit and scope of the appended claims.