“…The flow related side force component will be a function of the local flow angle and when the car and truck velocities are equal is approximately: (4) where C Yβ is the gradient of side force with yaw and A is the frontal area of the car. When the car is travelling at velocity, V C , the side force becomes; (5) Assuming that ΔV X is very much smaller than V C or V T , then equation (3) in coefficient form, based on the truck velocity, V T , and car frontal area, A, becomes: (6) As the function f(ΔV Y ) will be directly related to V T along a given path, equation (6) can be written simply as: (7) Similar expressions can be developed for the rolling and yawing moment: (8) The side force and yawing moment data presented by Schrefl et al, [13], has been replotted in Figure 8 using values estimated from his published results and converted for the relevant reference speed. The vertical axis represents the increase in the side force or yawing moment above the extrapolated notional value for a velocity ratio V C /V T = 1.0, and normalised by the yaw derivatives for the same vehicle given by Mayer et al, [15].…”