Properties of Friction — Question 9

Section 6-2 · Physics pages 808–809

Question 9 An area test can falsify an overextended friction model Take g = 10 m/s2. Use ideal dry friction, |fs| ≤µsN and |fk| = µkN. A 3 kg rectangular block slides on the same level material in two orientations. Contact areas are 20 and 40 cm2. With no pull, measured decelerations are respectively 2 and 3 m/s2. Assume measurement error is negligible and no other horizontal forces act. 20 cm2 40 cm2 v v |a| = 2 m/s2 |a| = 3 m/s2 The same 3 kg block slides in two orientations. Labeled contact areas, rather than drawing dimensions, specify the measurements. (a) Infer the kinetic coefficient in each trial. (b) Can one constant area-independent coefficient fit both trials? (c) For a new 6 kg block, what predictions follow from the two fitted coefficients, and why is neither guaranteed by these data?
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Question 9 - Solution An area test can falsify an overextended friction model 20 cm2 40 cm2 v v |a| = 2 m/s2 |a| = 3 m/s2 (a) Infer from force and normal load. For unforced sliding, the deceleration magnitude is m|a| = µkmg =⇒µk = |a| g . µk,20 = 2 10 = .20 , µk,40 = 3 10 = .30 . (b) Compare with the model’s restriction. One common coefficient would require |a20| = µkg = |a40|. The measured 2̸ = 3 m/s2 contradicts that restricted model. The comparison does not isolate contact area as the cause: changing orientation may also change other surface properties. (c) State conditional extrapolations. Conditional on transferring either fitted coefficient to the new block, |a| = µk(6)g 6 = µkg = { 2 m/s2, µk = .20, 3 m/s2, µk = .30. Mass cancels within each ideal model. The two measurements establish neither coefficient’s applicability to the new contact.

Question 9

An area test can falsify an overextended friction model

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 3 kg rectangular block slides on the same level material in two orientations. Contact areas are 20 and 40 cm2^2. With no pull, measured decelerations are respectively 2 and 3 m/s2^2. Assume measurement error is negligible and no other horizontal forces act.

Diagram shown in the original SVG worksheet.

  1. Infer the kinetic coefficient in each trial.

  2. Can one constant area-independent coefficient fit both trials?

  3. For a new 6 kg block, what predictions follow from the two fitted coefficients, and why is neither guaranteed by these data?

Question 9 - Solution

An area test can falsify an overextended friction model

Diagram shown in the original SVG worksheet.

(a) Infer from force and normal load.

For unforced sliding, the deceleration magnitude is m|a|=μkmg⇒μk=|a|g.m|a|=\mu_kmg\Longrightarrow\mu_k=\frac{|a|}{g}. μk,20=210=.20,μk,40=310=.30.\boxed{\mu_{k,20}=\frac2{10}=.20},\qquad\boxed{\mu_{k,40}=\frac3{10}=.30}.

(b) Compare with the model’s restriction.

One common coefficient would require |a20|=μkg=|a40|.|a_{20}|=\mu_kg=|a_{40}|. The measured 2≠32\ne3 m/s2^2 contradicts that restricted model. The comparison does not isolate contact area as the cause: changing orientation may also change other surface properties.

(c) State conditional extrapolations.

Conditional on transferring either fitted coefficient to the new block, |a|=μk(6)g6=μkg={2m/s2,μk=.20,3m/s2,μk=.30.|a|=\frac{\mu_k(6)g}{6}=\mu_kg =\begin{cases}2\ \mathrm{m/s^2},&\mu_k=.20,\\3\ \mathrm{m/s^2},&\mu_k=.30.\end{cases} Mass cancels within each ideal model. The two measurements establish neither coefficient’s applicability to the new contact.