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Chapter Summary
Dry Friction
  Frictional forces exist at the rough surfaces of
  contact
  They act on a body so as to oppose the motion
  or tendency of the motion of the body
  A static friction force approaches a maximum
  value of Fs = µsN
  µs is the coefficient of kinetic friction
  Solution of the problem requires first drawing of
  the FBD
Chapter Summary
Dry Friction
  If the unknowns cannot be determined strictly
  from the equations of equilibrium, and the
  possibility of slipping can occur, then the friction
  equation should be applied at the appropriate
  points of contact in order to complete the
  solution
  It may be possible for slender objects to tip over
  and this situation should also be investigated
Chapter Summary
Wedges, Screws, Belts and Bearings
 A frictional analysis of these objects can be
 performed by applying the frictional equation at
 the points of contact and then using the
 equations of equilibrium to relate the frictional
 force to other external force acting on the object
 By combining the resulting equations, the forces
 of friction can be eliminated so that the force
 needed to overcome the effects of friction can be
 found
Chapter Summary
Rolling Resistance
  The resistance of a wheel to roll over a surface is
  caused by deformation between two materials of
  contact
  This effect causes the resultant normal force
  acting on the rolling body to be inclined so that it
  provides a component that acts in the opposite
  direction of the force causing the motion
  The effect is characterized using coefficient of
  rolling resistance
Chapter Review
Chapter Review
Chapter Review
Chapter Review
Chapter Review
Chapter Review
Chapter Review
Chapter Review

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6161103 8.9 chapter summary and review

  • 1. Chapter Summary Dry Friction Frictional forces exist at the rough surfaces of contact They act on a body so as to oppose the motion or tendency of the motion of the body A static friction force approaches a maximum value of Fs = µsN µs is the coefficient of kinetic friction Solution of the problem requires first drawing of the FBD
  • 2. Chapter Summary Dry Friction If the unknowns cannot be determined strictly from the equations of equilibrium, and the possibility of slipping can occur, then the friction equation should be applied at the appropriate points of contact in order to complete the solution It may be possible for slender objects to tip over and this situation should also be investigated
  • 3. Chapter Summary Wedges, Screws, Belts and Bearings A frictional analysis of these objects can be performed by applying the frictional equation at the points of contact and then using the equations of equilibrium to relate the frictional force to other external force acting on the object By combining the resulting equations, the forces of friction can be eliminated so that the force needed to overcome the effects of friction can be found
  • 4. Chapter Summary Rolling Resistance The resistance of a wheel to roll over a surface is caused by deformation between two materials of contact This effect causes the resultant normal force acting on the rolling body to be inclined so that it provides a component that acts in the opposite direction of the force causing the motion The effect is characterized using coefficient of rolling resistance