How do space and time relate m rhythmical tasks that reqmre the hmbs to move singly or together m various modes of coordination ? And what kind of minimal theoretical model could account for the observed data9 Ead~er findings for human cychcal movements were consistent w~th a nonhnear, limit cycle oscdlator model (Kelso, Holt, Rubm, & Kugler, 198 l) although no detailed modehng was performed at that Ume In the present study, lonemauc data were sampled at 200 samples/second, and a detmled analysis of movement amphtude, frequency, peak velooty, and relative phase (for the blmanual modes, m phase and anuphase) was performed As frequency was scaled from l to 6 Hz (m steps of l Hz) using a pacing metronome, amphtude dropped reversely and peak veiooty m-creased WRhm a frequency condmon, the movement's amphtude scaled &rectly with lls peak veloc-Ry These &verse lonematlc behaviors were modeled exphotly m terms oflow-&menslonal (nonhn-ear) dlsslpaUve dynamics, wRh hnear stiffness as the only control parameter Data and model are shown to compare favorably The abstract, dynamical model offers a umfied treatment of a number of fundamental aspects of movement coordination and control How do space and time relate m rhythmical tasks that require the hands to move singly or together in various modes of coordi-nation9 And what kind of minimal theoretical model could account for the observed data? The present article addresses these fundamental questions that are of longstanding interest to experimental psychology and movement science (e g, von Hoist, 1937/1973; Scripture, 1899; Stetson & Bouman, 1935) It is well known, for example, that discrete and repetitive movements of different amplitude vary systematically in movement duration (provided accuracy requirements are held constant, e g, Cralk, 1947a, 1947b) This and related facts were later for-mahzed into F~tts's Law (1954), a relation among movement time, movement amplitude, and target accuracy, whose under-pmnmgs have been extensively studied (and debated upon) quite recently (e g.