 
 
 
 
 
 
 
  
The mathematical description of a knot was inspired by the polar decomposition theorem stating that the deformed state 
 of an infinitesimal vector
 of an infinitesimal vector 
 in a continuum can be decomposed into a stretch followed by a rotation [18],[20]:
 in a continuum can be decomposed into a stretch followed by a rotation [18],[20]:
|  | (43) | 
where 
 is the deformation gradient,
 is the deformation gradient, 
 is the rotation tensor and
 is the rotation tensor and 
 is the right stretch tensor. Applying this to a finite vector extending from the center of gravity of a knot
 is the right stretch tensor. Applying this to a finite vector extending from the center of gravity of a knot 
 to any expanded node
 to any expanded node 
 yields
 yields
|  | (44) | 
where 
 and
 and 
 are the deformation of the node and the deformation of the center of gravity, respectively. This can be rewritten as
 are the deformation of the node and the deformation of the center of gravity, respectively. This can be rewritten as
showing that the deformation of a node belonging to a knot can be decomposed in a translation of the knot's center of gravity followed by a stretch and a rotation of the connecting vector. Although this vector has finite dimensions, its size is usually small compared to the overall element length since it corresponds to the thickness of the shells or beams. In three dimensions 
 corresponds to a symmetric 3 x 3 matrix (6 degrees of freedom) and
 corresponds to a symmetric 3 x 3 matrix (6 degrees of freedom) and 
 to an orthogonal 3 x 3 matrix (3 degrees of freedom) yielding a total of 9 degrees of freedom. Notice that the stretch tensor can be written as a function of its principal values
 to an orthogonal 3 x 3 matrix (3 degrees of freedom) yielding a total of 9 degrees of freedom. Notice that the stretch tensor can be written as a function of its principal values  and principal directions
 and principal directions 
 as follows:
 as follows:
|  | (46) | 
 
 
 
 
 
 
