G. Cheron et al., Kinematics invariance in multi-directional complex movements in free space: effect of changing initial direction, CLIN NEU, 110(4), 1999, pp. 757-764
We investigated in normal human subjects the effect of changing the initial
direction on the kinematic properties of figure '8' movement performed as
fast as possible by the right arm extended in free space. To this end, the
motion of the index finger was monitored by the ELITE system. The figure '8
' movement was characterized by a complex tangential velocity profile (Vt)
presenting 5 bell-shaped components. It was found that the temporal segment
ation following Vt was not significantly different, whatever the initial di
rection of the movement. The decomposition of Vt into different velocity pr
ofiles with respect to vertical (3 phases, Iy-IIIy) and horizontal (5 phase
s, Iz-Vz) directions showed a significant relationship between the amplitud
e and the maximal velocity for all the different phases (except the IIy pha
se), which demonstrated a good conservation of the Isochrony Principle. How
ever, we showed that the transition between the clockwise and counterclockw
ise loop (inflection point) induced greater variability in the vertical vel
ocity profile than in the horizontal one. Moreover, some parameters such as
the maximal velocity of Iy and the movement amplitude of the last phases (
IIIy and Vz) showed significant changes depending on the initial direction.
A highly significant positive correlation was observed between the instant
aneous curvature and angular velocity. This was expressed by a power law si
milar to that previously describe for other types of movement. Furthermore,
it was found that this covariation between geometrical and kinematic prope
rties of the trajectory is not dependent on the initial direction of moveme
nt. In conclusion, these results support the idea that the fast execution i
n different directions of a figure '8' movement is mainly controlled by two
types of invariant commands. The first one is reflected in the 2/3 power l
aw between angular velocity and curvature and the second one is represented
by a segmented tangential velocity profile. (C) 1999 Elsevier Science Irel
and Ltd. All rights reserved.