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Figure 3


Fig. 3. The thin-airfoil model (A), the normal-forces model (B) and parameters used in calculation of Pind (C). In all panels, FR is the resultant aerodynamic force. (A) The thin-airfoil model for a wing in steady flow (e.g. Norberg, 1990), modified for non-horizontal flight. FL is lift, and FD is drag. β is the angle between the resultant aerodynamic force and the direction of wing movement. (B) The normal-forces model on a static wing in steady flow [after Usherwood and Ellington (Usherwood and Ellington, 2002a)]. The direction of the aerodynamic force is assumed to be normal to the surface of the wing. Fh and Fv are the horizontal and vertical forces acting on the wing, respectively. {alpha}global is the angle of the wing relative to the horizontal. (C) Schematic of parameters used in calculation of Pind. The area of the stroke plane is projected, using the angle {delta}, onto the actuator disc, which is defined as normal to FR. {alpha}disc is the angle of the actuator disc in the global reference frame. {alpha}' is the angle between the flight velocity V and the actuator disc. As they are shown here, both {alpha}disc and {alpha}' have negative values [following Stepniewski and Keys (Stepniewski and Keys, 1984)]. Vx is the horizontal component of the flight velocity. Use of the term Vxsin{alpha}disc eliminates PPE from the Pind calculation.





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