In this
post, I’m going to discuss the different methods and ideas to get a uniform
torque through the whole revolution (cycle) of Savonius or any drag type VAWT.
Some of these methods can be applied and the other may be only theoretical.
Consider the following relations to extract all
the available methods to obtain a
1. Using
helical (twisted) profile Savonius
The common
two-bladed Savonius wind turbine with 180 degrees angle of twist (like helix®
wind turbine) will produce a uniform torque through the whole cycle. This
method is the best method –till now- to smoothen torque. This method looks like
placing a large (infinite) number of conventional Savonius turbines with infinitesimal
height one above another, and each turbine is angularly-shifted (rotated about
axis of rotation). Theoretically (as I claim, and neglecting the effect of top
and bottom tips), a general relation which relates number of blades with angle
of twist may be used:
Considering a Savonius
bucket (semi-circular) element with infinitesimal height, the previous relation
(formula) came from the fact that we want -at any angular position of the
turbine- to find buckets with phase angles ranging from 0 to 360 degrees. Or more
precisely, and in other words, for any angular position of the turbine we want
to find blade patterns ranging from 0 to 360.
Note: increasing number
of blades has certain limits. Performance of wind turbine deteriorates at high
number of blades. Also, the geometry of the blade constrains the maximum number
of blades.
2. Variable
radius (force arm)
In this
method, the blade will slide out/in from/to the center of rotation in order to
compensate decrease/increase of aerodynamic force to get a uniform torque through
the whole cycle. In fact this method is completely idiot because it has
the following disadvantages:
§
This method will work properly –theoretically- for only
one wind direction (and its opposite direction), and so the main advantage of
VAWT of receiving wind from any direction with the same performance is no more
available
§
Sliding motion in and out is going to change the
primary gap between inner blade tips which affects heavily the performance and
noise level of the turbine
§
This method requires a complex mechanism (based on the
mathematical model of the aerodynamic force) to give a variable radius. In most
cases, aerodynamic force does not change linearly with angular position.
§
The use of certain mechanism will limit the RPM of the
turbine and make it more noisy and difficult to maintain.
3. Variable
drag (projected) area
As a
concept, it looks like the previous method. In this method we increase/decrease
the area of the blade (in drag type VAWT) as the torque arm
decreases/increases. This method also has the same disadvantages of the
previous method. When drag area increases/decreases in a radial direction,
torque radius also is going to increase/decrease and this is how two methods
can be combined in one.
4. Variable
blade profile
It is some
kind of foolish to think about this method, but it is just an option to
imagine. In this method we change blade profile and so drag coefficient as the
blade rotates. Blade profiles with high drag coefficients will be used at
smaller torque radii, and vise versa. In addition to the disadvantages of
methods 2 and 3, a changing blade profile may be considered as a science
fiction as it is impossible to achieve.
5. Controlling
inlet wind speed
In fact,
inlet wind speed can be controlled with different methods based on the
imagination of the designer, but I’m going to assume that a flat shield plate
is used to do this job. Controlling the angle of this shield plate is going to
affect and control air speed over the advancing blade. The control of shield
plate angle may be achieved by using stepper/servo motor or by linking the
shield plate with the rotor by a mechanism to update plate angle passively
without the need of external control. This method requires some setup for a
given (fixed) wind direction, and this makes the turbine no more useful when
wind comes from another directions.
6. Controlling
rotational speed of the wind
By controlling
rotational speed of the turbine at different angular positions, we can control
the relative velocity of air with respect to blades. At positions of high
torque values increase turbine’s rpm, and at the positions of low torque values
decrease turbine’s rpm.
7. Changing
inlet wind direction with time
When blade
rotates, deviate the direction of inlet air keeping its speed the same.
As the
turbine revolves, change the inlet wind direction in order to make the turbine
exposed to the same aerodynamic force for the whole cycle.
8. Controlling
inlet air density
This method
also is just an imagination in a science fiction movie. In this method
increase/decrease air density when torque arm decreases/increases. Air density
may be controlled by spraying a water mist in the inlet air (just imagine).
9. Array of
Savonius wind turbines with angular (phase) shift
Imagine a linear array of simple Savonius wind
turbines that are connected (linked) using a large belt or sprocket chain, and
this belt drives a central generator. Also, imagine that those turbines have
different phase angles for a given wind direction. Although this method
requires a farm of wind turbines, and has many disadvantages like the use of
belts or chains, positioning problems of these turbines, and not-operating with
the same performance for all wind directions, but it conceptually works.
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