Friction — Question 1

Section 6-1 · Physics pages 772–773

Question 1 Friction can accelerate a moving object forward Take g = 10 m/s2. A 2 kg parcel slides right at 1 m/s on a conveyor moving right at a constant 4 m/s. Kinetic friction has magnitude 6 N. Once velocities match, the parcel can stick. No other horizontal force acts. block vp = 1 m/s vb = 4 m/s Schematic horizontal contact; arrows show specified motion or applied forces. (a) Find the direction of friction and the parcel acceleration while it slips. (b) Find the time to match the belt speed and the parcel displacement in that time. (c) Find the sliding distance relative to the belt and the friction force after matching.
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Question 1 - Solution Friction can accelerate a moving object forward block vp = 1 m/s vb = 4 m/s (a) Compare the two velocities. Take right as positive. The contact slip is vp/b = vp −vb = 1 −4 = −3 m/s. Friction opposes this relative motion, so fk = +6 N. Newton’s second law gives ap = fk m = 6 2 = +3 m/s2 . (b) Follow the ground-frame motion. While slipping, vp(t) = 1 + 3t in SI units. End this phase when vp = vb: 1 + 3tc = 4 =⇒tc = 1 s . ∆xp = vp0tc + 1 2apt2 c = 1(1) + 1 2(3)(1)2 = 2.5 m . (c) Compare travel and then test sticking. The belt travels ∆xb = 4(1) = 4 m. Hence ∆xp/b = 2.5 −4 = −1.5 m, sslip = 1.5 m . After matching, the common velocity is constant: ap = 0. Therefore fs = map = 0 . Friction opposes contact slip, not necessarily ground-frame velocity.

Question 1

Friction can accelerate a moving object forward

Take g=10g=10 m/s2^2. A 2 kg parcel slides right at 1 m/s on a conveyor moving right at a constant 4 m/s. Kinetic friction has magnitude 6 N. Once velocities match, the parcel can stick. No other horizontal force acts.

Diagram shown in the original SVG worksheet.

  1. Find the direction of friction and the parcel acceleration while it slips.

  2. Find the time to match the belt speed and the parcel displacement in that time.

  3. Find the sliding distance relative to the belt and the friction force after matching.

Question 1 - Solution

Friction can accelerate a moving object forward

Diagram shown in the original SVG worksheet.

(a) Compare the two velocities.

Take right as positive. The contact slip is vp/b=vp−vb=1−4=−3m/s.v_{p/b}=v_p-v_b=1-4=-3\ \mathrm{m/s}. Friction opposes this relative motion, so fk=+6f_k=+6 N. Newton’s second law gives ap=fkm=62=+3m/s2.\boxed{a_p=\frac{f_k}{m}=\frac62=+3\ \mathrm{m/s^2}}.

(b) Follow the ground-frame motion.

While slipping, vp(t)=1+3tv_p(t)=1+3t in SI units. End this phase when vp=vbv_p=v_b: 1+3tc=4⇒tc=1s.1+3t_c=4\Longrightarrow\boxed{t_c=1\ \mathrm s}. Δxp=vp0tc+12aptc2=1(1)+12(3)(1)2=2.5m.\boxed{\Delta x_p=v_{p0}t_c+\tfrac12a_pt_c^2=1(1)+\tfrac12(3)(1)^2=2.5\ \mathrm m}.

(c) Compare travel and then test sticking.

The belt travels Δxb=4(1)=4\Delta x_b=4(1)=4 m. Hence Δxp/b=2.5−4=−1.5m,sslip=1.5m.\Delta x_{p/b}=2.5-4=-1.5\ \mathrm m,\qquad\boxed{s_{\mathrm{slip}}=1.5\ \mathrm m}. After matching, the common velocity is constant: ap=0a_p=0. Therefore fs=map=0\boxed{f_s=ma_p=0}. Friction opposes contact slip, not necessarily ground-frame velocity.