1985
DOI: 10.1016/0375-9601(85)90065-9
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The chaotic behavior of the leaky faucet

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Cited by 107 publications
(51 citation statements)
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“…Let DT (n) be the time interval that separates the (n + 1)th droplet from the nth droplet. The time series of interdrop intervals DT (n) connects the study of the formation and dynamics of droplets in ants to that of a dripping faucet, which was introduced as an early and simple example of a chaotic system (Shaw, 1984;Martien et al, 1985;Austin, 1991;Sartorelli et al, 1994;Penna et al, 1995;Sanchez-Ortiz and Salas-Brito, 1995). The physics of the dripping faucet involves surface tension, which decreases the dripping rate, and gravity, which acts as a nonlinearly coupled competitive force.…”
Section: Resultsmentioning
confidence: 99%
“…Let DT (n) be the time interval that separates the (n + 1)th droplet from the nth droplet. The time series of interdrop intervals DT (n) connects the study of the formation and dynamics of droplets in ants to that of a dripping faucet, which was introduced as an early and simple example of a chaotic system (Shaw, 1984;Martien et al, 1985;Austin, 1991;Sartorelli et al, 1994;Penna et al, 1995;Sanchez-Ortiz and Salas-Brito, 1995). The physics of the dripping faucet involves surface tension, which decreases the dripping rate, and gravity, which acts as a nonlinearly coupled competitive force.…”
Section: Resultsmentioning
confidence: 99%
“…If the seemingly random florescence gives rise to a distinct structure in phase space, with noninteger fractal dimension, onto which the phase space points are concentrated, it would be a clear indication that it is actually the consequence of dynamical deterministic chaos (i.e., hidden variables), in direct analogy to how [11,12] revealed deterministic chaos in the dynamics of the dripping water faucet ( Figure 6). For examples of qualitatively typical chaotic attractors/structures see, for example, the figures in [11,12] or the famous examples presented in the figures in this article : "The Lorenz map"-when successive, erratically fluctuating, amplitude maxima were plotted for the Lorenz attractor (previous figure) using a technique analogous to the one described in this article, the surprising result was this nearly one-dimensional attractor; hidden order in chaos [20], and a concrete simple example of the relation between continuous dynamics and discrete mappings.…”
mentioning
confidence: 95%
“…For examples of qualitatively typical chaotic attractors/structures see, for example, the figures in [11,12] or the famous examples presented in the figures in this article : "The Lorenz map"-when successive, erratically fluctuating, amplitude maxima were plotted for the Lorenz attractor (previous figure) using a technique analogous to the one described in this article, the surprising result was this nearly one-dimensional attractor; hidden order in chaos [20], and a concrete simple example of the relation between continuous dynamics and discrete mappings.…”
mentioning
confidence: 99%
“…First, one asks the question of whether this system, which seems inherently to be a predictable, periodic flow, can yield complex dynamics? Evidence exists that this is indeed the case, and that the capillary jet can serve as a model dynamical system for chaos studies (Martien et al 1985).…”
Section: Introductionmentioning
confidence: 99%