“…The following expressions 1 define the trajectory of a fluid particle in a rotating coordinate system with origin at the centre of a radial impeller where θ is the polar angle of the position of a particle at a radial distance, r , from the centre, β the angle which an element of the trajectory makes with the radial direction and r· and θ· the rates of change with respect to time of the parameters. The above equations then yield the following expression for the polar angle, θ , as function of the radial distance, r , of the particle 5 where β 1 is the inlet relative flow angle at the radial distance r 1 .…”