Friction — Question 9

Section 6-1 · Physics pages 788–789

Question 9 A friction force can be inferred from motion without knowing a coefficient A 2 kg puck slides right on a stationary horizontal surface. A force of 3 N acts left. At one instant the measured acceleration is 4 m/s2 left. No other horizontal interaction acts. block v 3 N Schematic horizontal contact; arrows show specified motion or applied forces. (a) Infer friction at that instant. (b) Find the reaction force exerted by the puck on the surface. (c) A second report gives acceleration 1 m/s2 right with the same rightward slip and applied force. Can ordinary friction explain it?
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Question 9 - Solution A friction force can be inferred from motion without knowing a coefficient block v 3 N (a) Use a signed force balance. Take right positive and use the measured acceleration: −3 + f = 2(−4) =⇒f = −5 N . The inferred 5 N leftward force agrees with kinetic friction opposing rightward slip. (b) Reverse agent and recipient. The tangential third-law pair is⃗ ffloor→puck = −5ˆi N,⃗ fpuck→floor = +5ˆi N . The applied 3 N force is a separate interaction, not this force’s reaction partner. (c) Audit signs before fitting parameters. The alternative acceleration would require −3 + f = 2(+1) =⇒f = +5 N. But rightward sliding on a stationary floor requires fk ≤0. The positive inferred force contradicts ordinary kinetic friction; an observation or the force inventory must change.

Question 9

A friction force can be inferred from motion without knowing a coefficient

A 2 kg puck slides right on a stationary horizontal surface. A force of 3 N acts left. At one instant the measured acceleration is 4 m/s2^2 left. No other horizontal interaction acts.

Diagram shown in the original SVG worksheet.

  1. Infer friction at that instant.

  2. Find the reaction force exerted by the puck on the surface.

  3. A second report gives acceleration 1 m/s2^2 right with the same rightward slip and applied force. Can ordinary friction explain it?

Question 9 - Solution

A friction force can be inferred from motion without knowing a coefficient

Diagram shown in the original SVG worksheet.

(a) Use a signed force balance.

Take right positive and use the measured acceleration: −3+f=2(−4)⇒f=−5N.-3+f=2(-4)\Longrightarrow\boxed{f=-5\ \mathrm N}. The inferred 5 N leftward force agrees with kinetic friction opposing rightward slip.

(b) Reverse agent and recipient.

The tangential third-law pair is f→floor→puck=−5𝒊̂N,f→puck→floor=+5𝒊̂N.\vec f_{\mathrm{floor\to puck}}=-5\hat{\mathbf i}\ \mathrm N,\qquad\boxed{\vec f_{\mathrm{puck\to floor}}=+5\hat{\mathbf i}\ \mathrm N}. The applied 3 N force is a separate interaction, not this force’s reaction partner.

(c) Audit signs before fitting parameters.

The alternative acceleration would require −3+f=2(+1)⇒f=+5N.-3+f=2(+1)\Longrightarrow f=+5\ \mathrm N. But rightward sliding on a stationary floor requires fk≤0f_k\leq0. The positive inferred force contradicts ordinary kinetic friction; an observation or the force inventory must change.