The problem is illustrated in As indicated in Fig. the block slides a distance x in coming to a halt on the rough surface. First, find the forces which act on the block... draw the damn picture, as we do in Fig. The forces are gravity (mg, downward) the normal force from the surface (FN , upward) and the force of kinetic friction (fk, backward i.e. opposite the direction of motion). Now, the motion only takes place along a horizontal line, so the vertical acceleration is zero. So the net vertical force on the mass is zero, giving:
Now that we have the normal force of the surface,
(b) The net force on the block is the friction force so that the magnitude of the block’s acceleration is
We should note that the direction of the acceleration opposes the diretion of motion, so if the velocity is along the +x direction, the acceleration of the block is
ax = −2.94 m/s2
Actually, by plugging the numbers into the formulae we’ve missed an important point. Going back to part (a), we had FN = mg, so that
fk = µkFN = µkmg
and the magnitude of the acceleration is
that is, the acceleration of the mass does not depend on the value of m, just on µk and g.
(c) The distance travelled by the mass before it comes to a halt: We have the initial velocity v0 of the mass, the final velocity (v = 0) and the acceleration.