Relating the Linear and Angular Variables — Question 7

Section 10-4 · Physics pages 1444–1445

Question 7 A sliding bead is not a fixed-radius point of the rotor A bead is constrained to a straight radial slot rotating at constant ω = 3 rad/s. Its radius is r(t) = 0.20 + 0.10t m. Use the polar acceleration relations ar = ¨r −rω2 and aθ = rα + 2 ˙rω. x y + A bead slides outward in a rotating radial slot; its radius is not fixed. (a) Find velocity components and acceleration components at t = 1 s. (b) Explain the error in using only aθ = rα.
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Question 7 - Solution A sliding bead is not a fixed-radius point of the rotor x y + (a) Derivation and calculation At t = 1 s, the given radial law yields r = 0.30 m, ˙r = 0.10 m/s, ¨r = 0, ω = 3, α = 0. (vr, vθ) = ( ˙r, rω) = (0.10, 0.90) m/s . ar = 0 −0.30(3)2 = −2.70, aθ = 0 + 2(0.10)(3) = 0.60, (ar, aθ) = (−2.70, 0.60) m/s2 . (b) Result and interpretation The full polar formula separates two tangential contributions: aθ = rα |{z} 0 + 2 ˙rω |{z} 0.60 m/s2 . The bead slides relative to the rotor, so ˙r̸ = 0 and the fixed-radius formula aθ = rα omits a required term. Physical check Setting the radial sliding rate to zero recovers the usual rigid-body formula.

Question 7

A sliding bead is not a fixed-radius point of the rotor

A bead is constrained to a straight radial slot rotating at constant ω=3rad/s\omega=3\,\mathrm{rad/s}. Its radius is r(t)=0.20+0.10tmr(t)=0.20+0.10t\,\mathrm m. Use the polar acceleration relations ar=r̈−rω2a_r=\ddot r-r\omega^2 and aθ=rα+2ṙωa_\theta=r\alpha+2\dot r\omega.

Diagram shown in the original SVG worksheet.

  1. Find velocity components and acceleration components at t=1st=1\,\mathrm s.

  2. Explain the error in using only aθ=rαa_\theta=r\alpha.

Question 7 - Solution

A sliding bead is not a fixed-radius point of the rotor

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

At t=1t=1 s, the given radial law yields r=0.30m,ṙ=0.10m/s,r̈=0,ω=3,α=0.r=0.30\ \mathrm m,\quad\dot r=0.10\ \mathrm{m/s},\quad\ddot r=0,\quad\omega=3,\quad\alpha=0. (vr,vθ)=(ṙ,rω)=(0.10,0.90)m/s.\boxed{(v_r,v_\theta)=(\dot r,r\omega)=(0.10,0.90)\ \mathrm{m/s}}. ar=0−0.30(3)2=−2.70,aθ=0+2(0.10)(3)=0.60,(ar,aθ)=(−2.70,0.60)m/s2.a_r=0-0.30(3)^2=-2.70,\quad a_\theta=0+2(0.10)(3)=0.60, \quad\boxed{(a_r,a_\theta)=(-2.70,0.60)\ \mathrm{m/s^2}}.

(b) Result and interpretation

The full polar formula separates two tangential contributions: aθ=rα⏟0+2ṙω⏟0.60m/s2.a_\theta=\underbrace{r\alpha}_{0}+\underbrace{2\dot r\omega}_{0.60\ \mathrm{m/s^2}}. The bead slides relative to the rotor, so ṙ≠0\dot r\ne0 and the fixed-radius formula aθ=rαa_\theta=r\alpha omits a required term.

Physical check

Setting the radial sliding rate to zero recovers the usual rigid-body formula.