The generalised forces corresponding to Q, f, y are therefore components of the torque, not along the line of nodes, the space z-axis, and the body z-axis respectively. Hence, of these three only the generalised force corresponding to y directly furnishes a component of the total torque along one of the principal axes, in this case along with z-axis. The Lagrange equation for y can be therefore be written as follows. | ![]() |