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Chapter 2. Prehension

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<strong>Chapter</strong> 5 - Movsrnent Before Contact 163<br />

transport component. In contrast, there were obvious differences in<br />

anticipatory hand posturing between the egg-like object and the spheri-<br />

cal one. On perturbed trials, when the sphere suddenly expanded to<br />

appear egg-like, the fmt evidence for alterations in hand configuration<br />

occured at least 500 ms after perturbation onset. He noted this time<br />

required elaboration of new commands, and the configuration of a<br />

new, appropriate grip pattern before the beginning of fiiger closure.<br />

Thus, in contrast to the short times for compensation to visual<br />

perturbation of extrinsic characteristics, it appears that perturbing in-<br />

trinsic object characteristics requires a longer time to reconfigure the<br />

opposition space parameters. In a larger experiment (more subjects,<br />

more trials with a computerized motion analysis system), with pertur-<br />

bations to obiect size both grasp and transport components were af-<br />

fected (Paulignan, Jeannerod, MacKenzie, 8z Marteniuk, 199 1).<br />

Using pad opposition, subjects grasped one of two, nested dowels,<br />

placed 35 cm away. The inner, ‘small’ dowel was 10 cm high and 1.5<br />

cm in diameter; the outer, ‘large’ dowel was 6 cm high and 6 cm in<br />

diameter. On 20% perturbed trials one of the two translucent dowels<br />

would be illuminated, then at movement onset, the illumination would<br />

suddenly switch to the larger (S->L) or smaller (L->S) dowel, giving<br />

the impression of an expanding or shrinking dowel respectively.<br />

Results showed that movement time for S->L trials, requiring a<br />

change in direction of planned aperture size (i.e., a reopening,<br />

compared to initial selection), increased by 175 ms, whereas L->S<br />

trials, requiring a change in magnitude of planned aperture size (ie.,<br />

greater closing), increased by only 98 ms. Compared to control, un-<br />

perturbed trials, none of the kinematic landmarks up to peak decelera-<br />

tion were affected by the perturbation; all changes to the transport<br />

kinematics occurred after peak deceleration (about 300 ms), during the<br />

low velocity phase. Shown in Figure 5.20, grip formation for the<br />

S->L perturbation showed a first peak (corresponding in time and<br />

amplitude to the peak aperture for the small dowel in control<br />

conditions), some discontinuity, then reincreased to accommodate the<br />

size of the new dowel. This reincreasing occurred 330 ms after<br />

movement onset (as determined from the grip velocity profile), after<br />

peak deceleration. The time between the two peaks in grip aperture for<br />

S->L was about 180 ms. The aperture evolution for the L->S<br />

perturbation was much attenuated, showing no discontinuities and<br />

only one peak, and identical to control large conditions, except for a<br />

longer enclose phase, until the fingers reached their contacting<br />

locations on the smaller dowel. Remarkable in these data was the low<br />

variability in the spatial paths of the hand, as enclosing occurred. This

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