I've found that the floor where I have my computer desk is slightly sloped, which sometimes causes my wheeled office chair to drift away from the table. What's interesting is that it only happens under certain circumstances. In order to roll back, the wheels must be pointed close enough to the direction of the slope that gravity, the force rolling it down the slope, can overcome the rolling friction created by imperfections in the wheels and the floor.

We can define an effective slope for the floor based on the direction relative to the full slope that the wheels point. If we call the full slope

*θ*and the deviation from the straight backward direction

*φ*, then the effective slope is

Using this, the force exerted by gravity is

where

*m*is the mass of the chair (plus anyone in it). Frictional forces generally depend on the normal force between two surfaces. In this case, that's

Plotting these together as functions of

*φ*gives something like

where the green line is

*F*and the red line is*N*. Anywhere the green is over the red, the chair will roll. Varying*θ*changes the crossing point; for sufficiently small angles, the chair will not move at all. Also note that frictional forces are usually some fraction of*N*, so the red line will likely be lower than shown.With luck, my power will be back on sooner than scheduled, but I'll try to keep posting regardless...