A fuselage is usually associated with the use of a delta wing on an actual aircraft. It is also in many cases necessary to use a centerbody of some shape in tunnel tests of pure delta wings. The present paper describes the ow physics causing the experimentally observed large effect of a fuselage on delta-wing vortex breakdown.
NomenclatureB = de ection angle of apex ap, Fig. 6 b = wingspan c = wing root chord l = rolling moment, coef cient C l = 2 l/(r U /2)Sbp = static pressure, coef cient C p = ( p 2 2 p )/(r U /2)`R e = Reynolds number based on c and freestream conditions S = reference area, projected wing area U = horizontal velocity W LE = body-induced upwash effect at the leading edge x = chordwise coordinate, distance from apex a = angle of attack D = increment Da LE = angular delay of leading-edge ow separation, Eq. (1) dLE = angle of leeside leading-edge bevel L = leading-edge sweep j = dimensionless x coordinate, x/c r = air density s = inclination of the roll axis f = roll angle Subscripts B = vortex breakdown eff = effective LE = leading edgè = freestream conditions