Properties of Friction — Question 2

Section 6-2 · Physics pages 794–795

Question 2 A wall clamp has a lower and an upper useful load Take g = 10 m/s2. Use ideal dry friction, |fs| ≤µsN and |fk| = µkN. A 2 kg block is pressed against a vertical wall by a force P directed 30◦above horizontal toward the wall. The static coefficient is 0.5. Treat the block as a particle. 2 kg P wall The angled force points into the wall and upward; wall friction may point either way. (a) Find N and the signed upward friction required for rest. (b) Find the full interval of nonnegative P allowing rest. (c) Explain the two endpoint slip tendencies and locate the zero-friction load.
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Question 2 - Solution A wall clamp has a lower and an upper useful load 2 kg P wall (a) Resolve relative to the wall. Horizontal equilibrium fixes the wall normal; vertical equilibrium fixes friction: N = P cos 30◦= √ 3 2 P , f = mg −P sin 30◦= 20 −P 2 . Here f > 0 means upward friction, with all force values in newtons. (b) Use both sides of the inequality. Rest requires both signs of the static bound: 20 −P 2 ≤µsN = √ 3 4 P. 20 ≤  1 2 + √ 3 4  P, 20 ≥  1 2 − √ 3 4  P. 80 2 + √ 3 ≤P ≤ 80 2 − √ 3 N =⇒ 21.436 ≤P ≤298.564 N. (c) Interpret the signed demand. At the lower endpoint, f = +µsN prevents downward slip. At the upper endpoint, f = −µsN prevents upward slip. Between them, f = 0 =⇒20 −P/2 = 0 =⇒P = 40 N . Large P can therefore destroy equilibrium by demanding too much downward friction.

Question 2

A wall clamp has a lower and an upper useful load

Take g=10g=10 m/s2^2. Use ideal dry friction, |fs|≤μsN|f_s|\le\mu_sN and |fk|=μkN|f_k|=\mu_kN. A 2 kg block is pressed against a vertical wall by a force P directed 30∘30^\circ above horizontal toward the wall. The static coefficient is 0.5. Treat the block as a particle.

Diagram shown in the original SVG worksheet.

  1. Find N and the signed upward friction required for rest.

  2. Find the full interval of nonnegative P allowing rest.

  3. Explain the two endpoint slip tendencies and locate the zero-friction load.

Question 2 - Solution

A wall clamp has a lower and an upper useful load

Diagram shown in the original SVG worksheet.

(a) Resolve relative to the wall.

Horizontal equilibrium fixes the wall normal; vertical equilibrium fixes friction: N=Pcos⁡30∘=32P,f=mg−Psin⁡30∘=20−P2.\boxed{N=P\cos30^\circ=\frac{\sqrt3}{2}P},\qquad\boxed{f=mg-P\sin30^\circ=20-\frac P2}. Here f>0f>0 means upward friction, with all force values in newtons.

(b) Use both sides of the inequality.

Rest requires both signs of the static bound: |20−P2|≤μsN=34P.\left|20-\frac P2\right|\leq\mu_sN=\frac{\sqrt3}{4}P. 20≤(12+34)P,20≥(12−34)P.20\leq\left(\tfrac12+\tfrac{\sqrt3}{4}\right)P,\qquad20\geq\left(\tfrac12-\tfrac{\sqrt3}{4}\right)P. 802+3≤P≤802−3N⇒21.436≤P≤298.564N.\boxed{\frac{80}{2+\sqrt3}\leq P\leq\frac{80}{2-\sqrt3}}\ \mathrm N \quad\Longrightarrow\quad\boxed{21.436\leq P\leq298.564}\ \mathrm N.

(c) Interpret the signed demand.

At the lower endpoint, f=+μsNf=+\mu_sN prevents downward slip. At the upper endpoint, f=−μsNf=-\mu_sN prevents upward slip. Between them, f=0⇒20−P/2=0⇒P=40N.f=0\Longrightarrow20-P/2=0\Longrightarrow\boxed{P=40\ \mathrm N}. Large PP can therefore destroy equilibrium by demanding too much downward friction.