Properties of Friction — Question 6

Section 6-2 · Physics pages 802–803

Question 6 A hanging mass has an entire equilibrium interval Take g = 10 m/s2. Use ideal dry friction, |fs| ≤µsN and |fk| = µkN. A 4 kg block on a 30◦ incline is connected by a light taut cord over an ideal fixed pulley to hanging mass M. The incline has µs = 0.25. All bodies start at rest. T 40 N N incline block T Mg hanging mass Separate force sketches; unknown friction along the slope is to be determined. (a) Find normal force and maximum static friction on the incline block. (b) Find all M for which equilibrium is possible. (c) For M = 2 kg, determine tension and friction; identify the slip tendency beyond each interval endpoint.
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Question 6 - Solution A hanging mass has an entire equilibrium interval T 40 N N incline block T Mg hanging mass (a) Separate normal and tangential forces. Only the weight has a normal component: N = mg cos 30◦= 20 √ 3 N , fs,max = .25N = 5 √ 3 N . (b) Bound the force needed for equilibrium. Hanging equilibrium gives T = Mg = 10M in SI units. With uphill positive on the incline, T + f −mg sin 30◦= 0 =⇒f = 20 −10M. |20 −10M| ≤5 √ 3 =⇒2 − √ 3 2 ≤M ≤2 + √ 3 2 kg. The numerical interval is [1.134, 2.866] kg. (c) Interpret the interval. For the specified hanging mass, T = 2(10) = 20 N , f = 20 −20 = 0 . Below the allowed interval, insufficient tension leaves a downhill tendency for the incline block. Above it, the hanging mass tends downward and pulls the incline block uphill.

Question 6

A hanging mass has an entire equilibrium interval

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 4 kg block on a 30∘30^\circ incline is connected by a light taut cord over an ideal fixed pulley to hanging mass M. The incline has μs=0.25\mu_s=0.25. All bodies start at rest.

Diagram shown in the original SVG worksheet.

  1. Find normal force and maximum static friction on the incline block.

  2. Find all M for which equilibrium is possible.

  3. For M=2M=2 kg, determine tension and friction; identify the slip tendency beyond each interval endpoint.

Question 6 - Solution

A hanging mass has an entire equilibrium interval

Diagram shown in the original SVG worksheet.

(a) Separate normal and tangential forces.

Only the weight has a normal component: N=mgcos⁡30∘=203N,fs,max=.25N=53N.\boxed{N=mg\cos30^\circ=20\sqrt3\ \mathrm N},\qquad\boxed{f_{s,\max}=.25N=5\sqrt3\ \mathrm N}.

(b) Bound the force needed for equilibrium.

Hanging equilibrium gives T=Mg=10MT=Mg=10M in SI units. With uphill positive on the incline, T+f−mgsin⁡30∘=0⇒f=20−10M.T+f-mg\sin30^\circ=0\Longrightarrow f=20-10M. |20−10M|≤53⇒2−32≤M≤2+32kg.|20-10M|\leq5\sqrt3\Longrightarrow \boxed{2-\frac{\sqrt3}{2}\leq M\leq2+\frac{\sqrt3}{2}}\ \mathrm{kg}. The numerical interval is [1.134,2.866][1.134,2.866] kg.

(c) Interpret the interval.

For the specified hanging mass, T=2(10)=20N,f=20−20=0.\boxed{T=2(10)=20\ \mathrm N},\qquad\boxed{f=20-20=0}. Below the allowed interval, insufficient tension leaves a downhill tendency for the incline block. Above it, the hanging mass tends downward and pulls the incline block uphill.