Title of Invention

"METHOD AND APPARATUS TO DETERMINE THE WIND SPEED AND DIRECTION EXPERIENCED BY A WIND TURBINE."

Abstract An apparatus and a method used to determine the speed and direction of the wind experienced by a wind turbine are provided. Said apparatus comprises at least one sensor fixed to the rotor of said wind turbine, an angular sensor to measure the angular position of the rotor of said wind turbine, and a circuit which converts the relationship between the output of said at least one sensor and the output of the angular sensor into the speed and direction of the wind experienced by the wind turbine. According to the invention, the sensing apparatus can measure the wind speed and direction in three dimensions. In addition, mounting the sensors directly to the rotor of the wind turbine results in a very simple and robust installation. Mounting the sensors directly to the rotor also eliminates the turbulence from the rotor and the nacelle of the wind turbine from affecting the sensors. Figs. 1 and 2
Full Text Method and apparatus to determine the wind speed and direction experienced by a wind turbine
Field of Invention
The present invention relates to an apparatus and a method used to determine the speed and direction of the wind experienced by a wind turbine.
Background of the Invention
The power output of a wind turbine and the loads exerted on the wind turbine by the wind are to a large extent dependent on the orientation of the wind turbine with respect to the wind. Therefore means are available on most wind turbines to adjust the orientation of the wind turbine such that the optimum orientation can be achieved. In addition, means are available on most wind turbines which allow the wind turbine to be adjusted, by for example changing the angle of attack of the blades dependent on the wind speed.
In order for the wind turbine to be optimally adjusted, the wind speed and direction need to be known. By adjusting the wind turbine more optimally, the power output of the wind turbine will be increased and the loads on the wind turbine will be decreased.
In addition, accurate measurement of the wind speed and direction allows the power performance of the wind turbine to be determined accurately. Accurate power performance data for a wind turbine is very important for proper adjustment and monitoring of wind turbines.
Description of the Prior Art

In the prior art, the most common solution used to measure the
speed and direction of the wind, is to place a cup anemometer
and a wind vane on the roof of the wind turbine's nacelle. The
problem with this approach is that the wind measurement is
placed behind the rotor. The rotor introduces turbulence and
therefore the wind measured by the wind sensor will be different
from the wind in front of the rotor. In addition, if the wind is
coming at an angle, either horizontally or vertically, the
nacelle of the wind turbine introduces vortices and boundary
layer effects which may heavily influence the wind sensors.
One solution for the purpose of power performance verification
is to place a mast with a wind speed and direction sensor at a
distance from the wind turbine. Typically, such a mast is placed
at a distance 2-3 rotor diameters away from the wind turbine.
This works well in areas where the wind is relatively the same
at the location of the mast and the location of the wind
turbine, flat on-land sites and offshore wind farms being good
examples. However, in many locations this is not the case. One
example is a wind turbine located on a mountainous site. In such
situations the wind will be different at the wind sensor and at
the wind turbine and it is therefore necessary to find the
correlation between the two positions. This is very costly
because another mast needs to be erected at the position of the
wind turbine.
Another common option is to place a wind sensor on a shaft,
which extends in front of the wind turbine coaxially with the
axis of rotation of the rotor. This puts the wind sensor in
front of the wind turbine, away from the turbulence caused by
the rotor or the wind turbine body. However, since the rotor is
spinning and the wind sensor needs to be kept stationary, a
complex mechanical system needs to be built into the rotor in
order to allow the rotor to spin about the stationary shaft
holding the wind sensor.
Other more advanced sensor systems are also available which can
directly measure the wind speed passing over each blade. One
such system is described in US 6,361,275. In this system, an
anemometer is mounted on each blade. If the rotation speed of
the rotor and the angle of attack of the blade are known, the
actual wind speed present at the blade can be determined.
Another advanced sensor system is presented in GB 2,067,247. The
system provided by this invention is comprised of two pressure
sensors located near the tip of the blade's profile. If the
rotation speed of the rotor and the angle of attack of the blade
are known, then the wind speed at the blade can be determined
based on the pressure readings. In addition, this system
describes a method of orienting the wind turbine until it is
facing directly into the wind. This is accomplished by comparing
the pressure readings when the rotor is at 90° and at 270°. If
the pressures are equal, then the rotor is facing directly into
the wind. If there is a difference, then the rotor position is
adjusted until the difference is zero.
Another document, EP 1,288,494, discloses a planar wind speed
and direction sensor, which has two pitot tubes mounted in a
plane at an angle to each other. This allows the sensor to
determine the wind speed and direction in a single plane. EP
1,288,494 also mentions that the sensor can be mounted to a
rotor of a wind turbine and that the sinusoidal output of the
pitot tubes can be used to orient the wind turbine. However, no
details are provided of how the sinusoidal output is used to
orient the wind turbine. It is assumed that a method is used
which is similar to the one described in GB 2,067,247.'
However, the three systems described above do not provide a
direct method of measuring the mean wind speed and direction
experienced by the centre of the wind turbine's rotor. The rotor
centre is typically used as a reference position for the wind
speed of a power curve. In addition, two of the above three
presented systems rely on sensors mounted in or on the blades.-
Sensors mounted in or on the blades are both difficult to
install and to maintain due to their position. Sensors mounted
on the blades also experience the problem that the air speed
over the blade is to a large extent a function of the blade
speed. Typically, the air speed due to the blade speed will be
much higher than the air speed due to the wind.
Furthermore, the three systems described above do not give any
information as to the flow inclination angle of the wind. The
flow inclination angle is the angle the wind makes to the
rotation axis of the wind turbine in a vertical plane. By
knowing the flow inclination angle, the loads on the wind
turbine can be determined more precisely.
Summary of the Present Invention
A first aspect of the current invention is to provide a wind
speed and direction sensing apparatus for wind turbines which
can be placed in front of the rotor and rigidly mounted to the
rotor.
A second aspect of the current invention is to provide a wind
speed and direction sensing apparatus and method for wind
turbines which can measure the wind speed and direction in three
dimensional space.
A third aspect of the current invention is to provide a wind
speed and direction sensing method for wind turbines which can
measure both wind speed and direction with a simple, robust and
low cost apparatus.
A fourth aspect of the current invention is to provide a wind
speed and direction sensing apparatus for wind turbines which
can be made with no moving parts.
A fifth aspect of the current invention is to provide a wind
speed and direction sensing method for wind turbines which in
certain embodiments demands low computing power.
The new and unique way in which the current invention fulfills
the above mentioned aspects is by presenting an apparatus as
mentioned in the opening paragraph comprising at least one
sensor fixed to the rotor of said wind turbine, an angular
sensor to measure the angular position of the rotor of said wind
turbine, and a circuit which converts the relationship between
the output of said at least one sensor and the output of the
angular sensor into the speed and direction of the wind
experienced by the wind turbine.
In this way, a sensing apparatus is provided which allows the
sensors to be placed in front of the rotor, thereby preventing
the air turbulence generated by the rotor and the nacelle from
affecting the output of the sensors. In addition, the mounting
of the sensors is very simple since the sensors are fixed
directly to the rotor. This results in a sensing apparatus which
is of low cost and low maintenance.
Depending on the type of sensor used, many possible embodiments
of the sensing apparatus can be made which have no moving parts.
In addition, certain types of sensors are especially well suited
to harsh temperatures and weather. In this way, the sensing
system can be made very robust.
Since the sensors rotate together with the rotor, the sensors
scan the wind as it rotates and is therefore able to determine
the wind speed and direction in three dimensional space.
In a preferred embodiment, the at least one sensor can be
mounted on the spinner or the hub of the wind turbine or on a
body fixed to the rotor of the wind turbine. In this way, if the
characteristics of the airflow around the spinner or the body
are known, these characteristics can be used to help determine
the wind speed and direction.
One preferred choice for the sensor is an air speed sensor. Many
different types of air speed sensors, such as sonic sensors, cup
anemometers, etc..., are available which are robust and low cost.
Another choice is a pressure sensor, the output of said pressure
sensor representing the surface pressure at a point on said
spinner or said body. The surface pressure is related to the
speed of the air flowing over the surface and can therefore also
be used to determine wind speed and direction.
In order to make the computing simpler, two sensors can be fixed
to the rotor, the two sensors placed symmetrically about the
rotation axis of the rotor and mounted on a plane encompassing
the rotation axis. In this way, the system can, at any rotation
angle of the rotor, find the angle that the wind makes to the
rotation axis in that plane. By recording the output of the two
sensors at two different angular positions, said two angular
•*•
positions being 90° from each other, the wind direction can be
specified in three dimensions.
Furthermore, by fixing three or more sensors to said rotor, said
three or more sensors placed with equidistant angles around the
rotation axis of said rotor, the wind speed and direction in
three dimensions can be determined at any angular position of
the rotor from a single recording at that position.
The current invention also provides for a method according to
the opening paragraph comprising the steps of rotating at least
one sensor about the rotation axis of the rotor of said wind
turbine, recording the output of said at least one sensor in at
least one angular position, and using the relationship between
said at least one recording and the at least one angular
position at which it was taken to calculate the wind speed and
direction. In this way a method is provided which is simple and
makes low demands on computing power.
There are many different sensing apparatuses which can be used
in the above method. It should be understood that the current
method is not limited to the apparatuses as described in this
document. It should also be understood that the number of
sensors and the number of angular positions at which recordings
are taken can vary. For example, in the case where three sensors
are spaced equidistantly on the. surface of the spinner the wind
speed and direction can be specified with one reading. In the
case where only one sensor is mounted on the surface of the
spinner, multiple recordings can be used to fully define the
wind speed and direction in three dimensional space.
In certain cases, said at least one sensor can be mounted to a
body fixed to the rotor of the wind turbine and the flow
characteristics of the airflow around said body can be used in
the calculation of the wind speed and direction. The body can
for example be the spinner of the rotor. Using the flow
characteristics of the airflow around such a body allows the
sensors to be mounted quite close to the body since the nonlinear
effects of the airflow around the body are taken into
consideration.
In another embodiment of the method, the output of said at least
one sensor can be recorded at multiple points during the
rotation of the rotor and the sinusoidal relationship between
the recordings and the angular position at which the recordings
were taken is used to determine the wind speed and direction.
Using statistics the fluctuations in the wind speed and
direction can be filtered out and the average wind speed and
direction found.
In yet another embodiment of the method, the phase and the
extreme values of the above described sinusoidal relationship
can be used to determine the speed and direction of the wind.
Using the phase and extreme values of the sinusoidal
relationship results in a simple method which requires low
computing power.
It should be obvious to the person skilled in the art, that the
above described embodiments are just a few of many apparatuses
and methods which can be implemented within the scope of the
current invention.
Brief Description of the Figures
The invention will be explained in greater detail below where
further advantageous properties and example embodiments are
described with reference to the drawings, in which
Fig. 1 is a schematic representation seen in perspective of a
wind turbine equipped with a first embodiment of a sensing
system according to the invention,
Fig. 2 shows a perspective detail view of the same,
Fig. 3 shows a side view of the same,
Fig. 4 shows a side detail view of the same,
Fig. 5 shows the theoretical streamlines of air flowing around a
sphere,
Fig. 6 shows the theoretical tangential speed of the airflow
around a sphere measured at different angles of O as defined in
Fig. 5,
Fig. 7 shows the definition of the angles used to describe the
wind direction in a first method according to the invention,
where a) shows the spinner typically seen from above, b) shows
the spinner typically seen from the front, and c) shows the
spinner typically seen from the side,
Fig. 8 shows the relationship between the angle of the wind and
the airspeed ratio measured by air speed sensors mounted to
opposite sides of the spinner of the wind turbine,
Fig. 9 shows a schematic representation seen in perspective of a
wind turbine equipped with a second embodiment of the sensing
system according to the invention,
Fig. 10 shows a perspective detail view of the same,
Fig. 11 shows the theoretical pressure difference between the
air pressure at different points on the surface of a sphere and
the air pressure at a large distance from the sphere,
Fig. 12 shows the angles used to define the wind direction in a
second method according to the invention,
Fig. 13 shows the relationship between the angle of the wind and
the air pressure difference ratio measured by pressure sensor
readings taken on opposite sides of the spinner of the wind
turbine,
Fig. 14 shows a schematic perspective view of a wind turbine
equipped with a third embodiment of the sensing apparatus
according to the invention,
Fig. 15 shows a detail view of the same,
Fig. 16 shows a schematic perspective view of a wind turbine
equipped with a fourth embodiment of the sensing apparatus
according to the invention,
Fig. 17 shows a detail view of the same,
Fig. 18 shows a side view of a fifth embodiment of a sensing
system according to the invention, and
10
Fig. 19 shows a detail view of the same.
Description of a Preferred Embodiment of the Invention
A first example embodiment 1 of an apparatus according to the
invention is shown in fig. 1-4. In this example, two onedimensional
(ID) air speed sensors 2 are mounted on the spinner
3 of a wind turbine 4 in a plane which includes the rotation
axis 5 of the spinner. As will be known to the person skilled in
the art, the rotor 6 is typically comprised of two or more
blades 7, which are joined together by the hub. A spinner 3 is
attached to the centre of the rotor to streamline the flow
around the hub. The hub is located inside the spinner and can
therefore not be seen in fig. 1-4.
The front half of the spinner is spherical in order to ensure
that the flow around the spinner is well described and smooth.
The two ID sensors 2 measure the component of the air velocity
above the boundary layer of the spinner, in the plane in which
the sensors lie and in a direction which is tangential to the
surface of the spherical spinner at the point where the sensors
are mounted.
In this example, one-dimensional sonic sensors are used. Each
sonic sensor comprises two sensor heads 8a,8b. The principle of
operation of sonic sensors is to measure the time it; takes for a
sound wave to travel between the two sensor heads 8a,8b. A sound
wave is being sent from the first sensor head 8a to the second
sensor head 8b. The second sensor head 8b receives the sound
wave, and a second sound wave is sent from the second sensor
head 8b to the first sensor head Sa. The air speed, in the
direction between the tips, can be determined by the difference
in the time it takes for the two sound waves to travel the
distance between the two sensor tips. These sensors have no
moving parts and are therefore very robust. They can also be
heated in order to prevent ice build-up in cold climates.
However, many other types of sensors can also be used in this
application, not just ID sonic sensors. Some examples (not
shown) are pitot tubes, Savonious rotors, propeller anemometers,
cup anemometers, etc. Some sensors, such as the 1D sonic
sensors, automatically compensate for the rotation of the
spinner, other sensors such as cup anemometers are affected by
the spinner rotation as well. In these cases, it is possible to
compensate for the spinner rotation by determining the rotation
speed of the spinner from the measurement of the rotor's
position over time.
Since the sensors are, in the current example, mounted directly
to the spinner, they can be mounted such that they are
accessible from inside the spinner. The spinner of many wind
turbines is so large that a maintenance person can crawl into
the spinner. The sensors can therefore be mounted from the
inside of the spinner such that the body of the sensor is on the
inside of the spinner and the sensing components protrude
through one or more small holes in the surface of the spinner.
In the example of a 1D sonic sensor, two small holes are drilled
in the surface of the spinner through which the sonic probes
protrude. The body of the sonic sensor with the signal
conditioning and electronics is bolted to the inside of the
spinner. Many other sensors can be mounted in this way, for
example Savonious rotors, two bladed propellers, pitot tubes,
etc...
In the current example, the wind speed and direction can be
determined from the two 1D sensors by using knowledge of how the
airflow speed is changed in two opposite directions around a
spherical object combined with the knowledge of the position of
the rotor relative to the horizon. Fig. 5 shows a schematic
representation of the theoretical flow around a spherical body
9. According to irrotational flow theory, the tangential
airspeed of the airflow around a sphere at a certain point 10
can be written as:
(1)
where vo is the velocity of the wind at a sufficient distance
from the spinner such that it is not influenced by the spinner,
O is the angle formed between a vector from the centre of the
sphere to the point of interest 10 and the wind direction
vector, R is the radius of the sphere, and r is the distance
from the centre of the sphere to the point of interest. Fig. 6
shows the tangential airspeed at different values of O for a
windspeed of lOm/s and an r/R ratio of 1.1.
In order to define the wind direction, two angles are used, ah
and av, as shown in fig. 7. The first angle ah, defines the
angle of the projection of the wind vector W in the XZ plane.
This plane is typically the horizontal plane. The angle is
defined to be positive, counter clockwise about the y-axis. The
second angle av defines the angle of the projection of the wind
vector W in the XY plane. This plane is typically the vertical
plane. Positive angles are defined as counter clockwise about
the z-axis.
The first angle, ah, is found by using the ratio of the wind
speeds measured by the two ID sensors 2 when they lie in the XZ
plane. The second angle av is found by using the ratio of the
wind speeds measured by the two ID sensors 2 when they lie in
the XY plane. Using av as an example and the formula (1) for
tangential wind speed as presented above we can calculate this
ratio to be:
F(av) = $L0-"J V»Sin(*~H1+2r3J sin(*-«w)
The angle, 9, is the angle at which the sensors are placed
relative to the rotation axis 5 of the spinner 3, see fig. 4. In
13
the current example, 6 is constant at 30°. As can be seen, the
ratio F, as presented in equation (2) is only a function of cu
and not of wind speed. Therefore, by measuring this ratio and
using the inverse of the above relationship, the angle ou can be
found. Fig. 8 shows the inverse of the above relationship. In
this example, a closed form solution to the above relationship
can also be found, see equation (3) , however, for more complex
spinner geometry, it might not be possible to find a closed form
solution.
a =arctan| F(av)tan0 (3)
The actual wind speed can be found by putting, for example, the
first measured airspeed, vi, and the calculated angle, cu, into
formula (1) and solving for Vo,. Equation (4) shows equation 1
solved for v*,.
(Figure Removed)
smlt/-
The calculations as presented above can be performed in some
sort of electronic circuit. This circuit could for example be a
micro-controller or a micro-processor (not shown). The circuit
could in another embodiment be an analog circuit, which outputs
analog signals which are proportional to the wind speed and
direction. The circuit could either be placed in the spinner
itself or in the nacelle 11. Signals can be transferred from the
spinner to the nacelle via one of the many forms of data
transmission known. In modern wind turbines, there are already
many signals, which are transferred from the spinner to the
nacelle.
In the example presented above, the outputs of the two air speed
sensors are recorded in two angular positions. The first is when
the air speed sensors lie in the horizontal plane and the second
is when the air speed sensors lie in the vertical plane. The
angular position of the air speed sensors can be detected in
many different ways. One example is to use an angular sensor
(not shown), which continuously measures the angular position of
the rotor 6. Since the air speed sensors 2 are fixed to the
rotor, the rotor's angular position and the air speed sensors'
angular position are fixed relative to each other. The output of
the air speed sensors can therefore be recorded when the angular
sensor detects the desired angular position of the rotor.
Multiple angular sensors can be used in certain cases to provide
redundancy in the case that one or more of the angular sensors
fail.
Another example (not shown) is to have some sort of trigger
mounted to the rotor of the wind turbine which triggers
measurements by the wind speed sensors each time the rotor
reaches a certain position. This trigger could for example be a
hall-effect sensor mounted on the rotor which gives a pulse each
time the hall-effect sensor passes a magnet placed on the
nacelle of the wind turbine. Four magnets could be embedded in
the nacelle spaced 90° from each other. This system could also
be described as a sort of angular sensor since it triggers at
certain angular positions.
Fig. 9-10 show a second embodiment 12 of an apparatus according
to the invention. In this embodiment, pressure readings from a
pressure sensor 13 mounted to the surface of the spinner 3 of a
wind turbine 4 are used to determine the wind speed and
direction experienced by the wind turbine. In this embodiment,
only one difference pressure sensor 13 is used, however, it will
be obvious to the person skilled in the art that additional
pressure sensors can be used to increase the performance of the
system. As an example, increasing the sensor count will increase
both the resolution and the bandwidth of the measurements.
As in the previous example, the wind turbine shown in fig. 9-10
has a spinner with a spherical front surface. In order to find
the pressure distribution we use the theoretical pressure
distribution of a fluid in the boundary layer around a sphere as
given by irrotational flow theory. The pressure distribution is
given by:
Cpl-lsin20 (5)
where O is the angle between a vector describing the direction
of the fluid in free stream and a vector between the centre of
the sphere and the point of interest on the surface. This is the
same angle as defined in fig. 5. CP is the pressure coefficient
and is defined as:

where p is the density of the fluid, p is the pressure at the
point of interest on the surface of the sphere, p , and v , are
the pressure and., airspeed respectively at a point located
outside the influence of the spinner, for example on a rod 14
mounted in front of the spinner. The density of the fluid, p,
can be determined from lookup tables if the pressure and
temperature of the fluid are known. Figure 11 shows the
theoretical pressure difference (p-p ) as a function of O at a
wind speed of lOm/s.
In the example embodiment as shown in figure 9 and 10, a first
pressure sensor 13 is mounted on the spherical surface of the
spinner at an angle of 30° to the axis of rotation of the
spinner. A second pressure sensor 15 is mounted on a rod 14
extending from the spinner on the axis of the rotor 5. The
average pressure as measured through holes 15 in the rod gives
the atmospheric pressure p and the pressure difference to the
pressure sensor on the spinner p-px- The rod also has a
temperature sensor (not seen) at its base surrounded by rings
in order to shield it from the sun. As the spinner rotates, the
pressure sensors 13,15 rotate with the spinner. This results in
the first pressure sensor 13 "scanning" the pressure on the
surface of the spinner. Depending on the angle between the wind
and the rotation axis of the spinner, the pressure readings will
change. In the special case where the wind direction and the
rotation axis are the same, the pressure reading will be
constant. However, as soon as the wind direction and the
rotation axis of the spinner are slightly different, the output
from the pressure sensor will in average have a sinusoidal
shape. This sinusoidal relationship can be used to find the wind
speed and direction.
It should be obvious to the reader that due to fluctuations in
the wind, the actual output of the sensor 13 will not be
perfectly sinusoidal. However, using statistical tools and/or
taking a number of measurements over time, the output of the
sensor can be fitted to a sinusoidal relationship. In addition,
for spinners having different shapes, it could be imagined that
the output of the sensor is not perfectly sinusoidal.
In this second example, a different coordinate system can be,
used to define the wind direction. This coordinate system is
shown in fig. 12. The first angle, p, defines the angle of a
plane A rotated about the rotation axis of the spinner. The
plane A is the plane in which the wind direction vector lies.
This plane rotates about the rotation axis of the spinner as the
wind direction changes. The second angle a, defines the angle,
in the plane A, between the wind direction vector and the
rotation axis of the spinner.
The angle P can be found by finding the angle at which the
maximum air pressure is measured by the pressure sensor. The
maximum air pressure will be found when the sensor is lying in
the same plane as the wind direction vector, that is to say on
the plane A as described in fig. 12. Therefore, the angle (3 can
be easily found by measuring the angle of the spinner and
recording the angle at which the maximum pressure occurs.
As in the previous example, the ratio between two sensor
readings can be used to find a. In this example, the ratio
between the minimum pressure reading and the maximum pressure
reading is used. For the spinner in the current example, the
minimum pressure reading occurs 180° from the maximum pressure
reading. As in the previous example, two sensors could be
mounted to the spinner 180° away from each other and the
readings from both sensors recorded at a single position.
However, in this example, only one sensor is used. Therefore,
once the maximum pressure reading is taken, the sensor is
rotated 180° further and the minimum pressure reading recorded
at this second position. In order to take into account the fact
that the wind speed and direction is, due to fluctuations in the
wind,' not the same at the time of the two pressure readings, the
pressure readings should be taken over a number of rotations in
order to average out the fluctuations in the wind.
By calculating the ratio, Pmin/Pmax, a can be determined. Fig.
13 shows the relationship between this ratio and a for the
theoretical pressure distribution used in this example and a
pressure sensor located at 30°. This relationship needs to be
determined theoretically or experimentally if a different
spinner type is used or if a different pressure sensor location
is used.
Once, a is known, it can be plugged into the pressure
distribution formulas and used to solve for the wind speed.
Equation (7) shows this relationship.
The procedure according to this second example could also be
used with the sensors as presented in the first example.
If two or more sensors are used, the sensors can be calibrated
using statistical tools. For example, consider that case where
two sensors, SI and S2, are mounted on a plane symmetrically
about the rotation axis of the spinner. This is the same as in
the first example. Due to this arrangement, for every half
rotation, or 180°, the spinner makes, the two sensors, SI and
52, swap places. This means that if the wind speed and direction
were constant, the reading from SI when the spinner is at 0°
should be the same as the reading from S2 when the spinner is at
180°. If the two readings as described above were different,
then the sensors could be calibrated such that the readings were
the same. Using statistical tools, it is possible to use the
readings from the sensors even though the wind speed and
direction are not constant.
In the two" examples presented above, the sensors were mounted
directly to a spherical spinner. However, it is not necessary
for the spinner to have a spherical shape. Other shapes such as
ellipsoid, parabolic, etc... are also acceptable. For the method
presented in this embodiment to work, the spinner needs to be
shaped such that the airflow around the surface of the spinner
can be relatively well defined and smooth.
In cases where the flow distribution of the air around the
spinner is not well defined or well known, or in cases where the
spinner is of a non-smooth shape, a well-defined body can be
rigidly mounted to the rotor. An example of this is shown in
fig. 14-15 which show a third embodiment 17 of an apparatus
according to the invention. In Fig. 14-15 a spherical body 18 is
attached directly to the rotor hub 19 via a shaft 20. One or
more pressure sensors 21 or airspeed sensors can then be placed
on this well-defined body and the distribution of the airflow
over the well defined body used in determining the wind speed
and direction.
For illustration purposes, the examples presented make use of
the theoretical airflow around a sphere. The theoretical airflow
used in these examples was derived from irrotational flow
theory. Since the airflow on spinners in the real world can be
different from theory, an experimentally measured airflow could
be used if more accuracy is required. A more accurate airflow
could also be determined via more advanced theory or
computational fluid dynamics (CFD) software, where also the
minor influence of blade roots, the nacelle and the tower can be
taken into account.
The presented examples made use of sensors placed at 30° to the
rotation axis of the spinner. The angle at which the sensors are
placed has an effect on the resolution of the sensing apparatus
as well as the range of wind directions it can measure.
Resolution is affected due to the non-linear nature of the
airflow. Taking the case for a pressure based solution, it can
be said that the highest resolution is achieved when the
gradient of the pressure distribution is high. In the pressure
distribution around a sphere, as shown in fig. 11, the gradient
is high at angles of around 45°. Therefore, in order to have the
best resolution, the sensors should be placed at an angle which
keeps the sensor at angles of close to 45°.
The range of wind directions measurable by the wind sensing
apparatus also depends on the placement of the sensors. At
angles of § past approximately 80°, depending on the velocity
and other characteristics of the wind, the flow can separate
from the surface of the spinner, thereby making the sensor
measurement unreliable. By placing the sensor at 30°, the wind
can come in at angles of ±50° to the rotation axis of. the
spinner without the angle of O going over 80°. Placing the
sensor within the range of 30° to 50° is a good compromise,
however, other angles are also possible.
Fig. 16 and 17 show a fourth embodiment 22 of an apparatus
according to the invention. In this case, two propeller
anemometers 23 are placed on a pole 24 rigidly connected to the
front of the spinner 3. The two sensors are angled at 30° to the
pole's axis. The pole places the sensors outside of the airflow
which is affected by the shape of the spinner. As the spinner
rotates, the pole and the propellers rotate with the spinner.
The propeller anemometers will therefore output an almost
sinusoidal signal as they rotate since the angle between the
rotation axis of the sensor and the wind vector will change. The
measurements from the propellers together with the measurement
of the rotor position can be used to find the wind speed - and
direction. In this example, it is not important to knew the
characteristics of the pressure or velocity distribution of the
airflow about the spinner because the sensors are exposed co the
wind at a location where there are no significant effects from
the spinner.
Instead of propeller anemometers, sonics or other types of wind
speed sensors that change their output with a variation of the
angle to the sensor can also be used together with the rotor
position measurement.
In this fourth embodiment, the sensor is placed at an angle to
the rotor axis in order to utilize the change in sensor output
with the changes in inflow angle during rotation in order to
determine the wind direction. This principle is similar ro the
principle described earlier, but with the difference that in
this case the change in sensor output with the change in inflow
angle during rotation is not due to the change in airspeed over
the spinner, but rather it is due to the sensor changing
orientation with respect to the wind.
Figures 18 and 19 show a fifth embodiment 25 according ro the
invention. This embodiment has been developed due to experiments
that showed that the output of the sensors can be made less
susceptible to sensor mounting errors and ice build-up on the
spinner by measuring the air speed over the spinner at an angle
to the tangential airflow. In the embodiment shown in figures 1
8, the sensors were arranged to measure the tangential airspeed
of the airflow over the spinner. By simulating the effect of ice
build-up on the spinner, it can be seen that ice build-up has a
rather large effect on the tangential air speed measurement.
However, by using the same simulation and measuring the airspeed
at an angle to the tangent vector of the spinner at the sensor
location, it can be seen that certain angles and certain sensor
locations are less sensitive to the effects of ice build-up and
mounting errors.
Figure 18 shows two sensors 26 mounted to the spinner 3 at an
angle of 0=±45° to the rotor's rotation axis 5. Figure 19 shows
a detailed view of one of the sensors 26. The sensors 26 are
arranged to measure the air speed at an angle of (3=26.3° to the
tangential airflow flowing over the spinner at the location of
the sensor. The tangent vector is shown in figure 19 with the
letter T, the radial vector is shown with the letter R, and the
measurement vector is shown with the letter M. The angles used
in this example are used as an example only and should not limit
the invention to these specific values.
The sensors 26 in this embodiment comprise a sensor body 27
which houses the electronics and signal processing means, a bent
rod 28, and two sonic sensor heads 29, 30 attached to the bent
rod 28. The bent rod 28 is arranged in such a way that the sonic
sensor heads are placed on the vector M as shown in figure 19.
The sensor body 27 is mounted to the inside of the spinner 3 and
the bent rod 28 and sonic sensor heads 29,30 protrude through a
hole 31 in the spinner 3. In this way, the sensor unit can
easily be exchanged from the inside of the spinner, by detaching
the sensor body 27 from the spinner and retracting the bent rod
28 and sonic sensor heads 29, 30 through the hole 31 in the
spinner 3.
in tnis embodiment, the spinner 3 has been divided into two
parts, a mounting part 32 and a sensor part 33. The mounting
part 32 is rigidly connected to the rotor 6 of the wind turbine.
The sensors 26 are attached to the sensor part 32. The sensor
part 33 can be detached from the mounting part 32 and mounted in
a wind tunnel for calibration and testing. When the sensor part
33 is calibrated it can be mounted back on the mounting part 32.
This solution would be especially useful for smaller wind
turbines where access to the inside of the spinner is not
possible, since exchanging the sensor part would be quicker and
easier than exchanging the individual sensors.
The arrangement of the sensor 26 as shown in figure 19 has the
additional advantage that the upstream sonic sensor 30 does not
disrupt the airflow through the sensor. This results in a more
accurate reading of the airflow over the spinner surface.
As will be obvious to the reader, the method according to the
current invention will not work if the wind is coming from
behind the wind turbine. In this situation,"" a traditional wind
vane will be useful to get the wind turbine oriented in the
general wind direction. Once the wind turbine is facing
relatively into the wind and the rotor has started rotating, the
wind direction and speed determining apparatus according to the
current invention can take over from the wind vane, and measure
the wind direction and speed with much higher accuracy.
For all embodiments of the current invention the wind speed
measured at the spinner or hub can be correlated to the free
wind that is unaffected by the wind turbine rotor. This can be
done with the use of a mast (not shown) positioned at a
sufficient distance from the wind turbine, and with a wind speed
sensor mounted at hub height. The correlation can be determined
for the entire wind speed range, as well as for eventual
different blade regulation control strategies.
In addition, as will be obvious to the person skilled in the
art, the above examples are not exhaustive. There are many
different ways of placing sensors on the rotor or the spinner of
a wind turbine which make use of the techniques employed by the
examples above. There are also many different mathematical
methods to convert the measurements taken by sensors mounted on
the rotor or the spinner of a wind turbine into the wind speed
and direction.





We Claim:
1. An apparatus (1;12;17;22;25) for determining the speed and direction of the wind
experienced by a wind turbine (4) comprising,
- at least one sensor (2;13,15;21;23;26) fixed to the rotor (6; 19) of said wind turbine (4), characterized by
- an angular sensor to measure the angular position of the rotor of said wind turbine (4), and
- a circuit which converts the relationship between the output of said at least one sensor (2,13,15,21,23;26) and the output of the angular sensor into the speed and direction of the wind experienced by the wind turbine (4).

2. An apparatus (1;12;22;25) as claimed in claim 1 characterized in that the at least one sensor (2;13,15;21;23;26) is mounted on the spinner (3) or the hub (19) of the wind turbine (4) or on a body (18) fixed to the rotor (3; 19) of the wind turbine (4).
3. An apparatus (26) as claimed in claims 1 or 2 characterized in that said at least one sensor (26) comprises at bent rod (28) mounted on the spinner (3) or the hub (19) of the wind turbine (4), two sonic sensor heads (29,30) attached to the bent rod (28) opposite each other, and a sensor body (27) with the circuit which converts the relationship between the output of said at least one sensor (26) and the output of the angular sensor into the speed and direction of the wind experienced by the wind turbine (4).
4. An apparatus (1) as claimed in claims 1 or 2 characterized in that said at least one sensor is an air speed sensor (2).
5. An apparatus (12;17;22) as claimed in claims 1 or 2 characterized in that said at least one sensor is a pressure sensor (13,15;21;23), the output of said pressure sensor (13,15;21;23) representing the surface pressure at a point on said spinner (3) or said body (18).
6. An apparatus (12) as claimed in any of claims 1-5 characterized in that two sensors (13,15) are fixed to said rotor (6), said two sensors (13,15) placed symmetrically about the rotation axis (5) of said rotor (6) and mounted on a plane encompassing the rotation axis (5).
7. An apparatus as claimed in claims 1-5 characterized in that at least three sensors are fixed to said rotor and placed with equidistant angles around the rotation axis (5) of said rotor (6).

8. A method for determining the speed and direction of the wind experienced by a wind
turbine (4) comprising the steps of:
- rotating at least one sensor (2;13,15;21;23;26) about the rotation axis (5) of the rotor (6) of said wind turbine (4),
- recording the output of said at least one sensor (2; 13,15,-21,-23,-26) in at least one angular position, and
- calculating the wind speed and direction with the relationship between said at least one recording and the at least one angular position at which it was taken.

9. A method as claimed in claim 8, characterized in that said at least one sensor (2;13,15;21;23;26) is mounted to a body (3;18) fixed to the rotor (6;19) of the wind turbine and that the flow characteristics of the airflow around said body (3; 18) are used in the calculation of the wind speed and direction.
10. A method as claimed in claims 8 or 9, characterized in that the output of said at least one sensor (2;13,15;21;23;26) is recorded at multiple points during the rotation of the rotor (6; 19) and the relationship between the recordings and the angular position at which the recordings were taken is used to determine the wind speed and direction.
11. A method as claimed in claim 10 characterized in that the phase and the extreme values of said relationship are used to determine the speed and direction of the wind.
12. A method as claimed in any one of claims 8 to 11 characterized in that said at least one sensor is at least one air speed sensor (2,) fixed to the rotor (6) of said wind turbine (4).
13. A method as claimed in any one of claims 8 to 11 characterized in that said at least one sensor is at least one pressure sensor (13,15;21;23) mounted to a rotating body (3;18) fixed to the rotor (6; 19) of said wind turbine (4).


Documents:

5469-DELNP-2006-Abstract-(11-08-2009).pdf

5469-delnp-2006-abstract.pdf

5469-delnp-2006-assignment.pdf

5469-DELNP-2006-Claims-(06-03-2012).pdf

5469-DELNP-2006-Claims-(11-08-2009).pdf

5469-delnp-2006-claims.pdf

5469-delnp-2006-Complete Specification Granted.pdf

5469-DELNP-2006-Correspondence Others-(05-03-2012).pdf

5469-DELNP-2006-Correspondence Others-(06-03-2012).pdf

5469-DELNP-2006-Correspondence-Others-(11-08-2009).pdf

5469-delnp-2006-correspondence-others.pdf

5469-DELNP-2006-Description (Complete)-(11-08-2009).pdf

5469-delnp-2006-description (complete).pdf

5469-DELNP-2006-Drawings-(11-08-2009).pdf

5469-delnp-2006-drawings.pdf

5469-DELNP-2006-Form-1-(06-03-2012).pdf

5469-delnp-2006-form-1.pdf

5469-delnp-2006-form-13.pdf

5469-delnp-2006-form-18.pdf

5469-DELNP-2006-Form-2-(06-03-2012).pdf

5469-delnp-2006-form-2.pdf

5469-DELNP-2006-Form-3-(05-03-2012).pdf

5469-DELNP-2006-Form-3-(06-03-2012).pdf

5469-delnp-2006-form-3.pdf

5469-DELNP-2006-Form-5-(06-03-2012).pdf

5469-delnp-2006-form-5.pdf

5469-delnp-2006-form-6.pdf

5469-DELNP-2006-GPA-(05-03-2012).pdf

5469-delnp-2006-gpa.pdf

5469-delnp-2006-pct-210.pdf

5469-delnp-2006-pct-304.pdf

5469-delnp-2006-pct-409.pdf

5469-delnp-2006-pct-416.pdf

5469-DELNP-2006-Petition-137-(06-03-2012).pdf

5469-DELNP-2006-Petition-137-(11-08-2009).pdf


Patent Number 251349
Indian Patent Application Number 5469/DELNP/2006
PG Journal Number 10/2012
Publication Date 09-Mar-2012
Grant Date 07-Mar-2012
Date of Filing 20-Sep-2006
Name of Patentee FORSKNINGSCENTER RISØ
Applicant Address FREDERIKSBORGVEJ 399, P.O. BOX 49, DK-4000 ROSKILDE DENMARK.
Inventors:
# Inventor's Name Inventor's Address
1 PEDERSEN TROELS FRIIS BØGEVEJ 4, DK-4000 ROSKILDE DENMARK.
PCT International Classification Number G01P 13/02
PCT International Application Number PCT/DK2005/000193
PCT International Filing date 2005-03-22
PCT Conventions:
# PCT Application Number Date of Convention Priority Country
1 PA 2004 00494 2004-03-26 Denmark