Insects are too small and too slow, by conventional aerodynamics, to fly at all. A fixed wing at insect-scale Reynolds numbers should stall — flow separates and lift collapses — long before it produces enough force to support the animal's weight. Real insects get around this with unsteady, flapping-specific tricks: a leading-edge vortex (LEV) that stays attached to the top of the wing throughout each stroke (delayed stall), and rapid wing rotation at each stroke reversal that adds extra "rotational" circulation.
Re = U·c / ν — Reynolds number from mean wingtip speed U = 2ΦfR,
chord c, and air's kinematic viscosity ν ≈ 1.5×10⁻⁵ m²/s.
Lift coefficient C_L(α) = 0.225 + 1.58·sin(2.13α − 7.2°), and
instantaneous lift L = q·S·C_L with dynamic pressure q = ½ρU².
Flies, bees, wasps and beetles use asynchronous (fibrillar) flight muscle that oscillates at its own mechanical resonance — the wingbeat frequency can be several times higher than the rate at which the insect's nerves actually fire. Dragonflies and butterflies instead use synchronous muscle, contracting once per nerve impulse, which caps their wingbeat frequency far lower.