The Lift on a Thin Aerofoil with a Jet-Augmented Flap

The method which was developed in an earlier paper for calculating the lift on a thin jet-flapped aerofoil has been applied to the case in which the jet enters the main stream tangentially from a deflected flap. The lift derivative with respect to the (small) angle of deflection β is of the form where , E being the ratio of flap length to aerofoil chord, and D 0 a function both of E and of the jet momentum coefficient C J . In the special case C J = 0, D o vanishes and the classical results for attached flow on flapped aerofoils without super-circulation are obtained. More generally, D o has been evaluated over the range 0 J E between 0·02 and 0·50, using an electronic computer. The lift derivatives so found lie between those in the limiting cases of “deflection” (E = 0) and “incidence” (E=1) which were calculated in Reference 1. They show that the effectiveness of the jet-flap scheme might be greatly increased by blowing over flaps of the order of 20 or 30 per cent of the chord, rather than over the small “shrouds” which have hitherto been proposed.

[1]  D. A. Spence,et al.  The lift coefficient of a thin, jet-flapped wing , 1956, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.