Properties of Friction — Question 7

Section 6-2 · Physics pages 804–805

Question 7 A rough patch can reveal where a sliding body stops Take g = 10 m/s2. Use ideal dry friction, |fs| ≤µsN and |fk| = µkN. A small block enters a 2 m long horizontal patch at 4 m/s. That patch has µk = 0.20; beyond it a second patch has µk = 0.40. No horizontal applied force acts. Ignore block length. µk = 0.20 µk = 0.40 2 m 4 m/s The coefficient changes at a fixed spatial boundary. (a) Determine whether it reaches the second patch and find its entry speed. (b) Find the stopping distance measured from the start of the first patch. (c) Find total stopping time and explain why using an average coefficient over the distance is unnecessary.
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Question 7 - Solution A rough patch can reveal where a sliding body stops µk = 0.20 µk = 0.40 2 m 4 m/s (a) Check speed squared at the boundary. In patch 1, a1 = −µk1g = −2 m/s2. At its far boundary, v2 b = v2 0 + 2a1L1 = 16 + 2(−2)(2) = 8 > 0. The block reaches patch 2 with vb = 2 √ 2 m/s . (b) Stop under the second acceleration. Patch 2 supplies a2 = −4 m/s2. Its stopping segment satisfies 0 = v2 b + 2a2L2 =⇒L2 = 8 8 = 1 m. Lstop = L1 + L2 = 2 + 1 = 3 m . (c) Add the two durations. Use each phase’s acceleration and endpoint speeds: t1 = 2 √ 2 −4 −2 = 2 − √ 2 s, t2 = 0 −2 √ 2 −4 = √ 2 2 s. tstop = 2 − √ 2 2 = 1.2929 s . No averaged coefficient is needed; the boundary speed connects the two exact constant-acceleration solutions.

Question 7

A rough patch can reveal where a sliding body stops

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 small block enters a 2 m long horizontal patch at 4 m/s. That patch has μk=0.20\mu_k=0.20; beyond it a second patch has μk=0.40\mu_k=0.40. No horizontal applied force acts. Ignore block length.

Diagram shown in the original SVG worksheet.

  1. Determine whether it reaches the second patch and find its entry speed.

  2. Find the stopping distance measured from the start of the first patch.

  3. Find total stopping time and explain why using an average coefficient over the distance is unnecessary.

Question 7 - Solution

A rough patch can reveal where a sliding body stops

Diagram shown in the original SVG worksheet.

(a) Check speed squared at the boundary.

In patch 1, a1=−μk1g=−2a_1=-\mu_{k1}g=-2 m/s2^2. At its far boundary, vb2=v02+2a1L1=16+2(−2)(2)=8>0.v_b^2=v_0^2+2a_1L_1=16+2(-2)(2)=8>0. The block reaches patch 2 with vb=22m/s\boxed{v_b=2\sqrt2\ \mathrm{m/s}}.

(b) Stop under the second acceleration.

Patch 2 supplies a2=−4a_2=-4 m/s2^2. Its stopping segment satisfies 0=vb2+2a2L2⇒L2=88=1m.0=v_b^2+2a_2L_2\Longrightarrow L_2=\frac8{8}=1\ \mathrm m. Lstop=L1+L2=2+1=3m.\boxed{L_{\mathrm{stop}}=L_1+L_2=2+1=3\ \mathrm m}.

(c) Add the two durations.

Use each phase’s acceleration and endpoint speeds: t1=22−4−2=2−2s,t2=0−22−4=22s.t_1=\frac{2\sqrt2-4}{-2}=2-\sqrt2\ \mathrm s,\qquad t_2=\frac{0-2\sqrt2}{-4}=\frac{\sqrt2}{2}\ \mathrm s. tstop=2−22=1.2929s.\boxed{t_{\mathrm{stop}}=2-\frac{\sqrt2}{2}=1.2929\ \mathrm s}. No averaged coefficient is needed; the boundary speed connects the two exact constant-acceleration solutions.