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Fig. 7 Limiting case of
q max = π, short microtubules.
( a ) Pole force function.
( b ) Spindle force function.
( c ) Equilibrium
conformation. L = 0.8 R ,
S = 0.65 R . For clarity, only
few microtubule forms are
plotted. These microtubules
lie in the ( x , y ) plane that
passes through the spindle
axis. Their values of q are
sampled uniformly between 0
and q max . Reproduced from
Maly ( 2012 ) under the
Creative Commons
Attribution License
The positioning of an isolated complete aster with comparatively long microtu-
bules in three dimensions was considered in the previous section (Figs. 2 and 3 ). In
this case, considered now as a model for an isolated spindle pole, the pole force func-
tion has a root at approximately x p = 2( L R ): A more centrally positioned pole is
attracted to the cell margin, whereas a more eccentrically positioned one is repelled.
Considering a spindle with such an aster at each pole, one can observe that the pres-
ence of the root does not affect the stability of symmetry. Even though the pole force
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