How would the frictional force vary for an object being slid
across the floor, for example? Starting with an applied force of
zero and then increasing it (1), we see that the static frictional force
increases as well, always just enough to counteract the applied force.
Once the applied force, and therefor the static force, reaches the value
mSN (2), the object will start to
slide, and the frictional force will become kinetic in nature (heavy dotted
line)(3). If the applied force were to continue to remain constant
or even increase, the kinetic frictional force would remain at mKN
and the object would accelerate (4). However, the tendency of a mover
is usually to let up once the object starts to slide, and so we might expect
to move to the left along the lightly dotted line (5). Now, so long
as the applied force value is greater or equal to the kinetic frictional
force, the object will continue to slide, but if the applied force is allowed
to become smaller than mKN (6), the
object will decelerate and eventually come to rest, at which point the
frictional force immediately resumes its static nature, thus dropping to
whatever value FAPPLIED has (7).