Friction — Question 5

Section 6-1 · Physics pages 780–781

Question 5 A block can stop and remain stopped under a continuing pull A 2 kg block initially slides left at 3 m/s on a fixed floor. A constant 4 N force pulls right. Kinetic friction has magnitude 6 N; static friction can be at most 8 N. Take right as positive. block v0 4 N Schematic horizontal contact; arrows show specified motion or applied forces. (a) Find acceleration until the block first stops. (b) Find stopping time and displacement. (c) Determine what happens immediately afterward; explain why extending the first acceleration is invalid.
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Question 5 - Solution A block can stop and remain stopped under a continuing pull block v0 4 N (a) Use the current slip direction. Initially vx < 0, so kinetic friction acts right. Thus Fnet = 4 + 6 = 10 N, ax = 10/2 = +5 m/s2 . (b) End this phase at zero velocity. Use the sliding acceleration only until the first zero of velocity: 0 = −3 + 5ts =⇒ts = .60 s , ∆x = −3(.60) + 1 2(5)(.60)2 = −.90 m . (c) Test the rest constraint. At rest the necessary static force is 4 + fs = 0 =⇒fs = −4 N, |fs| = 4 < 8 N. The block remains at rest: a = 0 . Extending a = 5 beyond the stop incorrectly retains a kinetic-friction law after sliding has ceased.

Question 5

A block can stop and remain stopped under a continuing pull

A 2 kg block initially slides left at 3 m/s on a fixed floor. A constant 4 N force pulls right. Kinetic friction has magnitude 6 N; static friction can be at most 8 N. Take right as positive.

Diagram shown in the original SVG worksheet.

  1. Find acceleration until the block first stops.

  2. Find stopping time and displacement.

  3. Determine what happens immediately afterward; explain why extending the first acceleration is invalid.

Question 5 - Solution

A block can stop and remain stopped under a continuing pull

Diagram shown in the original SVG worksheet.

(a) Use the current slip direction.

Initially vx<0v_x<0, so kinetic friction acts right. Thus Fnet=4+6=10N,ax=10/2=+5m/s2.F_{\mathrm{net}}=4+6=10\ \mathrm N,\qquad\boxed{a_x=10/2=+5\ \mathrm{m/s^2}}.

(b) End this phase at zero velocity.

Use the sliding acceleration only until the first zero of velocity: 0=−3+5ts⇒ts=.60s,0=-3+5t_s\Longrightarrow\boxed{t_s=.60\ \mathrm s}, Δx=−3(.60)+12(5)(.60)2=−.90m.\boxed{\Delta x=-3(.60)+\tfrac12(5)(.60)^2=-.90\ \mathrm m}.

(c) Test the rest constraint.

At rest the necessary static force is 4+fs=0⇒fs=−4N,|fs|=4<8N.4+f_s=0\Longrightarrow f_s=-4\ \mathrm N,\qquad |f_s|=4<8\ \mathrm N. The block remains at rest: a=0\boxed{a=0}. Extending a=5a=5 beyond the stop incorrectly retains a kinetic-friction law after sliding has ceased.