We analyse pair trajectories of equal-sized spherical particles in simple shear flow for small but finite Stokes numbers. The Stokes number, St =γ τ p , is a dimensionless measure of particle inertia; here, τ p is the inertial relaxation time of an individual particle andγ is the shear rate. In the limit of weak particle inertia, a regular small-St expansion of the particle velocity is used in the equations of motion to obtain trajectory equations to the desired order in St. and St 1/3 φ 1, respectively. Further, the region of zero-Stokes closed trajectories is destroyed, and there exists a new attracting limit cycle whose location in the shearing plane is, at leading order, independent of St. The extension of the present analysis to include a generic linear flow, and the implications of the finite-St trajectory modifications for coagulating systems are discussed.