Thread: Friction Puzzle
View Single Post
  #4   Spotlight this post!  
Unread 05-01-2009, 14:29
writchie writchie is offline
Engineering Mentor
AKA: Wally Ritchie
FRC #2152 (Team Daytona)
Team Role: Coach
 
Join Date: Dec 2007
Rookie Year: 2007
Location: Daytona Beach, Florida
Posts: 148
writchie has a reputation beyond reputewritchie has a reputation beyond reputewritchie has a reputation beyond reputewritchie has a reputation beyond reputewritchie has a reputation beyond reputewritchie has a reputation beyond reputewritchie has a reputation beyond reputewritchie has a reputation beyond reputewritchie has a reputation beyond reputewritchie has a reputation beyond reputewritchie has a reputation beyond repute
Re: Friction Puzzle

It depends on the center of gravity and the configuration of the wheels, i.e. are the wheels co-planer or are one or more wheels raised (or lowered).

When wheels are co-planer and the CG is in the geometric center then each wheel supports an equal weight and the normal forces are equal. If the transverse friction is higher than the inline (or longitudinal) friction then the physics say the robot will not move. Spinning the wheels might not help this situation. It will lower the inline friction, but the static transverse friction still applies - not the dynamic. For the dynamic transverse friction to apply, you generally need movement in the transverse direction. (To understand why this could be so think about a grooved wheel on a deformable surface - spinning in the grove won't help you get over the humps between the grooves ) This is true for the standard friction model but may be different with heat effects, lubrication effects, etc. are present.

If you drop (or raise) an opposing set of wheels, then the physics is quite different. The robot will be supported by at most 3 wheels. If the CG is in the geometric center, almost all of the normal force will be on the set of opposing wheels that is dropped. With a center CG the robot will teeter around the axis of the supporting wheels but both of the raised wheels will never be on the floor at the same time. To calculate the actual normal forces, you have to calculate the forces in three dimensions, accounting for the height of the CG. You also have to account for the force on the trailer hitch which can create an additional moment. Bottom line is that the robot will easily move, even with a transverse/inline ratio of 2.3. The friction force from the lower wheel will be very low because of the low normal force.

With a CG near the center, nearly all of the normal force will be on the two dropped wheels and if these are powered they can deliver the maximum force possible. If you drive those wheels in opposing directions, you will also have pretty close to the maximum possible turning moment, especially if these wheels are along the longest dimension. (Turning the orientation of the robot, however, does not necessarily turn the velocity vector).

We think it's worth evaluating your configuration. In fact, we are currently evaluating a similar configuration with two opposing driven wheels and two opposing steerable wheels, as well as a couple of other unconventional configurations involving raisable wheels and pairs of driven wheels. Note what happens if your dropped set of opposing wheels becomes your raised set and visa versa, especially if the documented transverse/inline ratio proves to be correct.