Rolling as Translation and Rotation Combined — Question 2

Section 11-1 · Physics pages 1554–1555

Question 2 A stationary contact point can have nonzero acceleration A wheel rolls right without slip at constant center speed 4 m/s and radius 0.50 m. Track the particular material point currently touching the ground. C vC⃗ aP Side view; arrows and labels specify the directions. (a) Find its instantaneous velocity and acceleration. (b) Explain why zero velocity does not imply zero acceleration or a permanently fixed pivot.
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Question 2 - Solution A stationary contact point can have nonzero acceleration C vC⃗ aP (a) Derivation and calculation No slip gives ω = −V/R = −8 rad/s. At the bottom,⃗r = −Rˆy:⃗ vb = V ˆx + ωˆz × (−Rˆy) =⃗0 . Because⃗aC = 0 and α = 0,⃗ ab = −ω2⃗r = V 2 R ˆy = 32ˆy m/s2 . (b) Result and interpretation Zero instantaneous velocity does not imply zero velocity derivative:⃗ vb(t0) = 0, d⃗vb dt t0 = 32ˆy̸ = 0. For a short interval ∆t, ∆y ≃1 2(32)(∆t)2 > 0. The material point rises away from the surface as another point becomes the contact; it is not a permanently fixed pivot. Physical check The acceleration is upward because the centripetal component points from the bottom toward the center.

Question 2

A stationary contact point can have nonzero acceleration

A wheel rolls right without slip at constant center speed 4m/s4\,\mathrm{m/s} and radius 0.50m0.50\,\mathrm m. Track the particular material point currently touching the ground.

Diagram shown in the original SVG worksheet.

  1. Find its instantaneous velocity and acceleration.

  2. Explain why zero velocity does not imply zero acceleration or a permanently fixed pivot.

Question 2 - Solution

A stationary contact point can have nonzero acceleration

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

No slip gives ω=−V/R=−8\omega=-V/R=-8 rad/s. At the bottom, r→=−Rŷ\vec r=-R\hat y: v→b=Vx̂+ωẑ×(−Rŷ)=0→.\vec v_b=V\hat x+\omega\hat z\times(-R\hat y)=\boxed{\vec0}. Because a→C=0\vec a_C=0 and α=0\alpha=0, a→b=−ω2r→=V2Rŷ=32ŷm/s2.\vec a_b=-\omega^2\vec r=\frac{V^2}{R}\hat y =\boxed{32\hat y\ \mathrm{m/s^2}}.

(b) Result and interpretation

Zero instantaneous velocity does not imply zero velocity derivative: v→b(t0)=0,dv→bdt|t0=32ŷ≠0.\vec v_b(t_0)=0,\qquad\left.\frac{d\vec v_b}{dt}\right|_{t_0}=32\hat y\ne0. For a short interval Δt\Delta t, Δy≃12(32)(Δt)2>0.\Delta y\simeq\tfrac12(32)(\Delta t)^2>0. The material point rises away from the surface as another point becomes the contact; it is not a permanently fixed pivot.

Physical check

The acceleration is upward because the centripetal component points from the bottom toward the center.