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By George V. Lauder (auth.), Graham K. Taylor, Michael S. Triantafyllou, Cameron Tropea (eds.)

ISBN-10: 3642116329

ISBN-13: 9783642116322

The actual ideas of swimming and flying in animals are intriguingly various from these of ships and airplanes. The research of animal locomotion for this reason holds a different position not just on the frontiers of natural fluid dynamics study, but in addition within the utilized box of biomimetics, which goals to emulate salient features of the functionality and serve as of dwelling organisms. for instance, fluid dynamic lots are so major for swimming fish that they're anticipated to have built effective circulate keep watch over tactics during the evolutionary means of model by way of usual choice, which would in flip be utilized to the layout of robot swimmers. And but, sharply contrasting perspectives as to the lively potency of oscillatory propulsion – particularly for marine animals – call for a cautious evaluation of the forces and effort expended at life like Reynolds numbers. For this and lots of different study questions, an experimental strategy is usually the main applicable technique. This holds as a lot for flying animals because it does for swimming ones, and comparable experimental demanding situations practice – learning tethered in place of loose locomotion, or learning the circulate round robot types in preference to actual animals. This ebook presents a wide-ranging photo of the cutting-edge in experimental learn at the physics of swimming and flying animals. The ensuing photo displays not just upon the questions which are of curiosity in present natural and utilized study, but additionally upon the experimental concepts which are on hand to respond to them.

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3 Working principle of our flapping mechanism. The spinning disk (constant RPM) is connected to the rod (by a pin fixed with bearings), and the rod is connected to the sled that slides over two (horizontal) rails. The rod moves up and down with a sine, while the sled moves left and right with a cosine. The cosine of the sled is used to drive the heave of the foil while the sine of the rod drives the pitch of the foil. We use one such mechanism to generate the heave kinematics (using the sleds cosine) and another one to generate the pitch kinematics (using the rods sine).

The variable range considered (Table 1) comprises the most extreme cases that we can obtain with our setup. Hence our error analysis can be considered a worst case analysis. We found that the mechanism accurately produces harmonic (sinusoidal) pitch and heave kinematics (Fig. 5). The maximum (local) deviation from ideal sinusoidal kinematics occurs at maximum excursion and is less than 5%, but this is an extreme value, it is typically less than 2%. Hence our new mechanism does not produce perfectly sinusoidal kinematics (as any other mechanism would) but it does generate significantly more sinusoidal kinematics than our earlier design (Lentink et al.

7e) from where the film flows into the main reservoir, which completes the cycle. The soap film speed and thickness can be controlled by two parameters once the Nylon wires are fixed to the frame: first, the valve (control of mass flow) and second, the tilt angle of the film with respect to the horizon (preset of gravitational component in flow direction). Reducing the flow at the valve results in slower and thinner films, while reducing the tilt angle results in slower and thicker films. T. Muijres and D.

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Animal Locomotion by George V. Lauder (auth.), Graham K. Taylor, Michael S. Triantafyllou, Cameron Tropea (eds.)


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