A theoretical framework is developed to predict the rate of geometric colli
sion and the collision velocity of small size inertialess particles in gene
ral turbulent flows. The present approach evaluates the collision rate for
small size, inertialess particles in a given instantaneous flow field based
on the local eigenvalues of the rate-of-strain tensor. An ensemble average
is then applied to the instantaneous collision rate to obtain the average
collision rate. The collision rates predicted by Smoluchowski (1917) for la
minar shear flow and by Saffman & Turner (1956) for isotropic turbulence ar
e recovered. The collision velocities presently predicted in both laminar s
hear flow and isotropic turbulence agree well with the results from numeric
al simulations for particle collision in both flows. The present theory for
evaluating the collision rate anti the collision velocity is also applied
to a rapidly sheared homogeneous turbulence to assess the effect of strong
anisotropy on the collision rate. Using (epsilon/nu)(1/2), in which epsilon
is the average turbulence energy dissipation rate and nu is the fluid kine
matic viscosity, as the characteristic turbulence shear rate to normalize t
he collision rate, the effect of the turbulence structure on the collision
rate and collision velocity can be reliably described. The combined effects
of the mean flow shear and the turbulence shear on the collision rate and
collision velocity are elucidated.