After summarlzlng the basic equations, the type of the equations for the upper-convected Maxwell model and for the Jeffreys-type models is derived. It is shown that the corotational Maxwell model changes type which is unacceptable from a physical point of view. The Jeffreys-type models (including the Leonov model) have a drastic different type compared to the Maxwell models and are physically more appealing. Correct boundary conditions are briefly discussed for a linearized upper-convected Maxwell model. The boundary conditions for the Jeffreys models are shown to be equal to the boundary conditions for the Navier-Stokes equations, supplemented by boundary conditions for all the extra stresses at the inflow boundary. Jump conditions are derived for Jeffreys-type models. It is shown that in complex flows with sharp corners discontinuities may arise. Numerical methods are discussed that take into account the special type of the equations.P. Wesseling (ed.), Research in Numerical Fluid mechanics