The purpose of this paper is to present a general analysis of the plan
ar circular restricted problem of three bodies in the case of exterior
mean-motion resonances. Particularly, our aim is to map the phase spa
ce of various commensurabilities and determine the singular solutions
of the averaged system, comparing them to the well-known case of inter
ior resonances. In some commensurabilities (e.g. 1/2, 1/3) we show the
existence of asymmetric librations; that is, librations in which the
stationary value of the critical angle theta = (p + q)lambda1 - plambd
a - qomegaBAR is not equal to either zero or pi. The origin, stability
and morphogenesis of these solutions are discussed and compared to sy
mmetric librations. However, in some other resonances (e.g. 2/3, 3/4),
these fixed points of the mean system seem to be absent. Librations i
n such cases are restricted to theta = 0 mod(pi). Asymmetric singular
solutions of the planar circular problem are unknown in the case of in
terior resonances and cannot be reproduced by the reduced Andoyer Hami
ltonian known as the Second Fundamental Model for Resonance. However,
we show that the extended version of this Hamiltonian function, in whi
ch harmonics up to order two are considered, can reproduce fairly well
the principal topological characteristics of the phase space and ther
eby constitutes a simple and useful analytical approximation for these
resonances.