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Published byLynne Hensley Modified over 9 years ago
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INVERTEBRATES AND FLUID DYNAMICS: OFF THE GROUND & MOVIN’ AROUND
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FLIGHT
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Chord Thickness Angle of attack Airfoil
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FLIGHT Standard airfoil Area of relatively low pressure Area of relatively high pressure LIFT
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FLIGHT Lift Drag Resultant force
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In flapping flight, need to compromise 1) lift 2) propulsion 3) Lowering of drag As you increase angle of attack generated
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H.G. Magnus (1802 – 1870)
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+ LIFT = translationcirculation MAGNUS EFFECT
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Same principle is used in various sports
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Curve ball
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Overall flow - Translational flow circulation =
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Circulation around wing
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At the beginning of flight Establish a counter vortex
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Some coefficients of lift BirdRe – 70002.0 LocustRe – 20001.3 Drosophila Re – 2000.9
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Hovering Flight
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Encarsia formosa Wing – 0.6 mm Mass -.000025 gm Re - 15 Coefficient of lift (predicted) = 0.02 Coefficient of lift (actual) = 5.0
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Clap-and Fling Mechanism Hovering flight
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Flip Mechanism - Dragonfly
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Hovering flight Translational Phase A) upstroke B) downstroke High angle of attack Rotational Phase A) pronation B) supination When wing reverses direction
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Hovering Flight
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Hovering flight Red arrows – total force and direction 1. Delayed Stall2. Rotational lift3 Forward motion Blue arrows – wing position
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Hovering flight
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Vortices around a flying animal Bound vortexTip vortices
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Propulsion at very low Re’s Rowing a boat – propulsive stroke is in lower Re (water) than recovery stroke (air)
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Propulsion at very low Re’s What about smaller animals that have to do both in low Re? Cladoceran Dytiscid beetle Thrips Nepticulid moth Mymarid wasp Ptiliid beetle Aquatic Aerial
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Propulsion at very low Re’s What about smaller animals that have to do both in low Re? Relative sizes Size difference and different viscosity of medium similar low Re’s
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Fringed propelling mechanism Power stroke (fringe expands) Recovery stroke (fringe collapses)
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