1988
DOI: 10.1016/0167-9457(88)90016-4
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The dimensionality of movement trajectories and the degrees of freedom problem: A tutorial

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Cited by 114 publications
(98 citation statements)
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“…Equation (1) is not proposed as a model of a rhythmic limb, it simply identifies the class of dynamics involved and provides a framework for discussion. Research by Kay and colleagues (Kay 1988;Kay et al 1991) has confirmed that a rhythmically moving limb segment abides the limit cycle attractor dynamics of (1). Application of the spatial correlation procedure (Grassberger and Procaccio 1984) for computing the dimensionality of an attractor revealed a dimension closely approximating 1, the dimension of a limit cycle attractor.…”
Section: ;: + O~2x = F(x De) -2gy¢ = H(x De)mentioning
confidence: 75%
“…Equation (1) is not proposed as a model of a rhythmic limb, it simply identifies the class of dynamics involved and provides a framework for discussion. Research by Kay and colleagues (Kay 1988;Kay et al 1991) has confirmed that a rhythmically moving limb segment abides the limit cycle attractor dynamics of (1). Application of the spatial correlation procedure (Grassberger and Procaccio 1984) for computing the dimensionality of an attractor revealed a dimension closely approximating 1, the dimension of a limit cycle attractor.…”
Section: ;: + O~2x = F(x De) -2gy¢ = H(x De)mentioning
confidence: 75%
“…Other rhythmic limb movements have similarly been modeled as limit-cycle attractors (Kelso et al 1981;Kay et al 1987;Kay et al 1991). Once again, however, this is only an approximation, for the trajectory of a limb movement in the phase plane is not a single closed orbit, but rather a band of attraction due to slight modulations from cycle to cycle (Kay 1988). Such a limit-cycle oscillator, when forced, takes on the frequency of the driver under restricted conditions, but also exhibits N:M mode locking, quasiperiodicity, intermittency, and chaotic behavior.…”
Section: A Preliminary Modelmentioning
confidence: 99%
“…In that regard, deterministic, autonomous, and timecontinuous systems are unambiguously described by their flow in phase (or state) space (or vector field), i.e., the space spanned by the system's state variables [19]. For movements along a single physical direction, as in a (sliding) Fitts' task, it is commonplace to use the movement's position and its time-derivative velocity as the state variables [11,20,21] (but see [22,23] for a critical discussion). The attractors that may live in such two-dimensional spaces are limited to (different kinds of ) fixed points (i.e., points where velocity and acceleration are zero) and limit cycles (nonlinear closed orbits), which are associated with discrete and rhythmic movements, respectively [24,25].…”
Section: Introductionmentioning
confidence: 99%