The shape of long, trailing cavities behind three-dimensional headform
s is discussed. The case of a flat elliptic wing is specifically treat
ed. Three distinct shape regimes are found: quasi-planar, long-flat, s
pheroidal. These appear in successively higher speed ranges (lower cav
itation numbers, sigma). It is argued that the cavities may be replace
d by surrogates in the form of slender ellipsoids. The pressures on th
ese are almost constant and correspond to a cavitation number equal to
twice their longitudinal added mass coefficient, k(1). A heuristic th
eory based on kinetic energy fields is given, relating k(1) to the pro
duct of head form drag and cavity length. This theory correlates with
an exact theory in the same form given by Garabedian for axi-symmetric
cones and also with its extension to planar flows. Results are given
here for the shape of the cavity behind an elliptic wing of any aspect
ratio, given drag, and cavitation number. Specific formulae are given
in the form, sigma = f(C-D/AR), for the transition between the quasi-
planar and long-flat regime, and the long-flat and spheroidal regime.