| Literature DB >> 28820898 |
Abstract
How effort is internally quantified and how it influences both movement generation and decisions between potential movements are 2 difficult questions to answer. Physical costs are known to influence motor control and decision-making, yet we lack a general, principled characterization of how the perception of effort operates across tasks and conditions. Morel and colleagues introduce an insightful approach to that end, assessing effort indifference points and presenting a quadratic law between perceived effort and force production.Entities:
Mesh:
Year: 2017 PMID: 28820898 PMCID: PMC5576751 DOI: 10.1371/journal.pbio.2002885
Source DB: PubMed Journal: PLoS Biol ISSN: 1544-9173 Impact factor: 8.029
Fig 1(A) Utility function traces (solid traces) resulting from trading off benefits (black solid trace) minus their associated costs (dashed-dot traces) as a function of movement time (T) for reaching movements of path distance (D) between 5 and 25 cm. The dots on the utility traces indicate the optimal time (T*) resulting from maximizing utility for that specific reaching, which increases with distance. (B) Effect of temporal discount (γ) on utility. Optimal movement times derived by maximizing utility are plotted as a function of distance for 3 specific temporal discount values. Movement times decrease as discount rates increase.
Fig 2Effect of biomechanical costs in motor control and decision-making.
(A) Decision-making task in which movements were aimed at the black rectangles. In each arrangement, the difference in biomechanical costs between T1 (right) and T2 (left) is maximal, although the relative path distance may vary. (B) Predicted versus measured average movement times for each of the 12 possible movements shown in (A). The equation below is the utility function used to obtain the optimal trajectory (and movement time). (C) Predicted versus measured group patterns of choices for T1 as a function of relative target path distance (D1 and D2: path distances from the origin to T1 and T2, respectively) (see [11,15,19] for further detail). The predicted pattern is obtained by fitting the softmax temperature to the utilities (J) obtained for either movement and for each relative distance.