Static and Kinetic Friction on a Vertical Wall

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Dynamics Intermediate Friction

Source: High school physics (Chinese)

Problem Sets:

Dynamics set 1008

Problem

A block weighing 22 N is held at rest against a vertical wall by a horizontal force $\vec{F}$ of magnitude 60 N. The coefficient of static friction between the wall and the block is 0.55, and the coefficient of kinetic friction between them is 0.38. In six experiments, a second force $\vec{P}$ is applied to the block, directed parallel to the wall.

  1. In each experiment, what is the magnitude of the frictional force on the block? The experiments are: (a) $P = 34$ N, up; (b) $P = 12$ N, up; (c) $P = 48$ N, up; (d) $P = 62$ N, up; (e) $P = 10$ N, down; and (f) $P = 18$ N, down.
  2. In which case(s) does the block move up the wall?
  3. In which case(s) does the block move down the wall?
  4. In which case(s) is the frictional force directed down the wall?
P0438-problem-1

P0438-problem-1

[Q1] (a) $f = 12$ N, (b) $f = 10$ N, (c) $f = 26$ N, (d) $f = 22.8$ N, (e) $f = 32$ N, (f) $f = 22.8$ N. [Q2] (d) [Q3] (f) [Q4] (a), (c), (d)

First, determine the normal force and the maximum static and kinetic friction forces. The block is in horizontal equilibrium, so the normal force $N$ from the wall balances the applied horizontal force $F$.

$$N = F = 60 \text{ N}$$

The maximum possible static friction is:

$$f_{s,max} = \mu_s N = 0.55(60 \text{ N}) = 33 \text{ N}$$

The kinetic friction, which applies when the block is moving, is:

$$f_k = \mu_k N = 0.38(60 \text{ N}) = 22.8 \text{ N}$$

For each case, we analyze the vertical forces: the weight $W=22$ N (down), the applied force $P$, and the friction force $f$. Let's define the net vertical force without friction as $F_{net,v}$ (positive up). If $|F_{net,v}| \le f_{s,max}$, the block remains static, and the static friction $f_s$ is equal in magnitude to $|F_{net,v}|$ and opposes it. If $|F_{net,v}| > f_{s,max}$, the block moves, and the friction is kinetic, $f_k=22.8$ N, opposing the motion.

(a) $P = 34$ N up. $F_{net,v} = P - W = 34 - 22 = 12$ N (up). Since $12 \text{ N} < f_{s,max}$, the block is static. $f_s = 12$ N (down). (b) $P = 12$ N up. $F_{net,v} = P - W = 12 - 22 = -10$ N (down). Since $|-10 \text{ N}| < f_{s,max}$, the block is static. $f_s = 10$ N (up). (c) $P = 48$ N up. $F_{net,v} = P - W = 48 - 22 = 26$ N (up). Since $26 \text{ N} < f_{s,max}$, the block is static. $f_s = 26$ N (down). (d) $P = 62$ N up. $F_{net,v} = P - W = 62 - 22 = 40$ N (up). Since $40 \text{ N} > f_{s,max}$, the block moves up. The friction is kinetic, $f_k = 22.8$ N (down). (e) $P = 10$ N down. $F_{net,v} = -P - W = -10 - 22 = -32$ N (down). Since $|-32 \text{ N}| < f_{s,max}$, the block is static. $f_s = 32$ N (up). (f) $P = 18$ N down. $F_{net,v} = -P - W = -18 - 22 = -40$ N (down). Since $|-40 \text{ N}| > f_{s,max}$, the block moves down. The friction is kinetic, $f_k = 22.8$ N (up).

[Q2] The block moves up only in case (d). [Q3] The block moves down only in case (f). [Q4] The frictional force is directed down when the net force tends to push the block up, or when it is moving up. This occurs in cases (a), (c), and (d).