 
 
 
 
 
   
Figure 2 illustrates the coordinate system of a blade.
The origin of the coordinate system is at the center of rotation in
the blade hub.  The  -axis is coincides with the rotor's axis or
rotation.  For simplicity, we assume that there is no coning (i.e., the blades
are perpendicular to the axis of rotation).  Thus, the
-axis is coincides with the rotor's axis or
rotation.  For simplicity, we assume that there is no coning (i.e., the blades
are perpendicular to the axis of rotation).  Thus, the  -axis points
through the blade.  In fact, the locus of spar midpoints is on the
-axis points
through the blade.  In fact, the locus of spar midpoints is on the
 -axis.  The
-axis.  The  -axis points towards the back of the blade.
-axis points towards the back of the blade.
Figure 3 illustrates a cross-section of the blade.
The  - and
- and  -axes are as described above.  The
-axes are as described above.  The  -axis points out
of the paper.  This figure also illustrates the surface coordinate
system for the single-celled beam that the blade is modeled as. The
-axis points out
of the paper.  This figure also illustrates the surface coordinate
system for the single-celled beam that the blade is modeled as. The
 -axis starts at the trailing edge and loops around as shown.  For simplicity,
the front edge of the blade is not considered, because it would
require a multicelled analysis.
-axis starts at the trailing edge and loops around as shown.  For simplicity,
the front edge of the blade is not considered, because it would
require a multicelled analysis.
There is one subtlety.  Due to blade twisting, the local coordinate
system of the cross-section is slightly different than the blade
coordinate system.  In the cross-section coordinate system, the
 -axis points through the trailing edge, regardless of the
angle-of-attack.
-axis points through the trailing edge, regardless of the
angle-of-attack.
 
 
 
 
