2013
DOI: 10.1016/j.ijnonlinmec.2013.02.007
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Crawlers in viscous environments: Linear vs non-linear rheology

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Cited by 29 publications
(26 citation statements)
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“…As an example of our results, we call the reader's attention on equations �3.15) and �3. 17), showing that the achievable displacement typically equals a fraction of the change of body length in one cycle, and that this fraction tends to one only in the limit case of infinite contrast between the resistance forces in the easy and hard direction. In this ideal limit case, there is no backsliding, and all the available extension/contraction of the crawler's body is converted into 'useful' displacement, as it is commonly assumed in the classical biological literature [1,31].…”
Section: Discussionmentioning
confidence: 99%
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“…As an example of our results, we call the reader's attention on equations �3.15) and �3. 17), showing that the achievable displacement typically equals a fraction of the change of body length in one cycle, and that this fraction tends to one only in the limit case of infinite contrast between the resistance forces in the easy and hard direction. In this ideal limit case, there is no backsliding, and all the available extension/contraction of the crawler's body is converted into 'useful' displacement, as it is commonly assumed in the classical biological literature [1,31].…”
Section: Discussionmentioning
confidence: 99%
“…In the case of crawlers exploiting dry friction, or lubricating fluid layers with complex rheology �such as the mucus secreted by snails [11,13]), resistance forces are nonlinear functions of the sliding velocity and locomotion is typically accomplished through stick-and-slip. Even when resistance forces are linear in the sliding velocity, if they also depend on the size of the contact region, then locomotion is still possible, provided that more elaborate strategies are employed [16,17,28]. These are very similar to those that are effective in low Reynolds number swimming, and show that the transition between crawling and swimming motility is much more blurred than what was previously thought.…”
Section: � Introductionmentioning
confidence: 91%
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“…We extend now our approach to quasi-static crawling [21][22][23]26] by considering T-periodic, reciprocal shape changes of the system shown in figure 9, such that its length first monotonically decreases from the initial value of L to L −s, and then monotonically increases from L −s to L. At any instant t, the configuration of the system is known upon determination of the two coordinates x i (t) and of the two lengths δ i (t), with i = {1, 2}. The compatibility of the displacements requires that…”
Section: A One-dimensional Model For the Bristle-crawlermentioning
confidence: 99%
“…There are many recent publications where mechanical and/ or mathematical models of locomotion of crawling systems are analysed [8][9][10][11]. Tanaka et al [12] studied the mechanics of peristaltic locomotion and the role of anchoring in locomotory waves by simple mechanical modelling of a peristaltic crawler.…”
Section: Introductionmentioning
confidence: 99%