MadSci Network: Physics |
In a sense all forces are reaction forces because all forces are partners in action reaction pairs. But I think that you mean something different. Friction is a response to motion or to incipient motion, as it were. I would not use the term "reaction force" because that has a specific and technical meaning in Newtonian physics. Consider first static friction and imagine a wooden block on a rough wooden surface. If you push on the block parallel to the surface, no motion occurs until a certain threshold applied force is reached. Until that force is applied, the static frictional force adjusts itself to be equal and opposite the applied force, like the force which a spring exerts on your hand when you pull on it. Note however, that the static friction force and the applied force are ON THE SAME BODY , unlike the action reaction pair of Newton's Third Law. The static frictional force thus matches the applied force until the applied force is made large enough finally to overcome the attractive forces between the surfaces. The bonds are finally broken. These forces are intermolecular in nature, and are applied only where the surfaces are in very close contact, which is only over an area much smaller than the actual physical area of the block. The close- contact area , where the surface separation is of molecular dimensions, is proportional to the normal force - that is, the weight of the block, or more generally, the downward force which the block applies to the surface. It is this force which effectively presses the surfaces together and creates close contact. Now suppose that you are pushing the block along the surface. Static frictional forces have been overcome, but the surfaces still are constantly binding to each other and unbinding as relative motion breaks the bonds. The result is a force which is opposite to the direction of velocity of the block. This is the force of kinetic friction. However kinetic friction does not depend on the magnitude of velocity . Both kinetic and static friction depend on the nature of the surfaces and on the normal force , and , for most materials, on nothing else. For a certain choice of surfaces friction is characterized by two coefficients of friction, mu static and mu kinetic. The static mu is alsways greater than the kinetic and the force of friction in either case is mu times the normal force. Sometimes ( steel on steel ) the coefficients differ little ( 0.7, 0.6 ). But for glass on glass, we have 0.9 compared to 0.4 .
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