A separatrix trajectory of a general solution to an ordinary differential equation is one which differs topologically from near by trajectories. Maximal regions of parallel flow are separated by a union of separatrices. The structure of these solutions has been a useful tool in the qualitative theory, especially in the plane (see, for example, [‘2, 6, 71). We will consider the separatrix structure of a flow near a solitary periodic solution in 3-space (cf. [Sj). A periodic orbit y is solitary if it has a compact neighborhood (neighborhood of solitude) G such that any negative (respectively, positive) semitrajectory contained in i? has its 4imit (resp., w-limit) at y. Within a neighborhood of solitude, trajectories are distinguished by their eventual behavior in time. For those sets of trajectories which are elhptic, that is, are contained in L’ and hence have CLand w-limit at y, an analysis of separatrix structure in a slightly different situation has already been set forth [a]. Our interest here will be primarily in the set &I+ of positively attracted trajectories, i.e.,. those which have w-limit at y, but leave U in the negative time direction. In contrast with the situation in two-dimensional settings, where each separatrix trajectory is thought of as separating two canonical regions, our analysis of separatrix structure must be concerned with connected components of the union of all separatrices. Thus, whereas a study of a planar flow is concerned with the geometry of individual trajectories, we must concern ourselves with the geometry of “surfaces” of separatrices. In general, these surfaces may be quite different from manifolds, even for C” flows. Our approach here is to restrict attention to those flows whose separatrix sets satisfy some kind of “manifold hypothesis.” We will also demand that no positive semitrajectory with initial state in the boundary of A !be internally tangent to the boundary of the neighborhood of solitude. Under a strict version of these hypotheses, a classification of regions of 9, is given by boundary type.