Swimming and Flying in Nature 1975
DOI: 10.1007/978-1-4757-1326-8_33
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Ornithopter Aerodynamic Experiments

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Cited by 8 publications
(4 citation statements)
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“…of 125 are depicted in Figure 10 for two cycles of flapping at V ¼ 3m=s and f ¼ 4:5Hz. As Liu and Kawachi 55 and Bennett et al 56 showed, the maximum normal force happens near the mid-downstroke zone, where the maximum value of separation vortex is achieved. Next, shedding the vortex causes the normal force to be reduced at the beginning of the upstroke.…”
Section: Resultsmentioning
confidence: 90%
“…of 125 are depicted in Figure 10 for two cycles of flapping at V ¼ 3m=s and f ¼ 4:5Hz. As Liu and Kawachi 55 and Bennett et al 56 showed, the maximum normal force happens near the mid-downstroke zone, where the maximum value of separation vortex is achieved. Next, shedding the vortex causes the normal force to be reduced at the beginning of the upstroke.…”
Section: Resultsmentioning
confidence: 90%
“…The instantaneous normal forces for the rigid wing at V ¼ 0 m=s and f ¼ 4:5Hz, the flapping angle of the mechanism and also the bending deflection angle are depicted in Figure 6 for two cycles of flapping. As Liu and Kawachi 42 and Bennett et al 43 manifested, the maximum normal force occurs near the mid-downstroke zone, where the separation vortex achieves its maximum value. Subsequently, shedding the vortex causes the normal force to decrease at the beginning of the upstroke.…”
Section: Methodsmentioning
confidence: 90%
“…In 1943, Holst (3) measured the lift and thrust forces generated by a small elliptical wing (32 mm semi-span) in an attempt to show how small Reynolds numbers (below 1000) affected the forces obtained. In 1974, Bennet, Obye and Jeglum (1) measured the instantaneous lift and thrust forces on a symmetrical aerofoil section undergoing sinusoidal oscillation.…”
Section: Introductionmentioning
confidence: 99%