Rotation with Constant Angular Acceleration — Question 1

Section 10-3 · Physics pages 1412–1413

Question 1 A stopping-angle specification determines the brake rate A rotor initially turns at 12 rad/s. It must stop after exactly 18 rad under constant angular acceleration. t ω 12 3 area 18 Constant signed acceleration produces a straight velocity trace; continuing it past rest reverses the motion. (a) Find the acceleration and stopping time. (b) If the same signed acceleration continues for two more seconds, find the additional signed displacement.
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Question 1 - Solution A stopping-angle specification determines the brake rate t ω 12 3 area 18 (a) Derivation and calculation Eliminate time during the stopping phase: ω2 f = ω2 0 + 2α∆θ, 0 = 144 + 36α ⇒α = −4 rad/s2 . ts = 0 −12 −4 = 3 s . (b) Result and interpretation Start a new time interval at the stopping instant. If the same signed acceleration persists, ∆θextra = 0(2) + 1 2(−4)(2)2 = −8 rad , ωf = (−4)(2) = −8 rad/s. This model reverses the motion; a brake that holds the rotor at rest would instead change its torque after stopping. Physical check The stopping area is 1 2(3)(12) = 18 rad, as required.

Question 1

A stopping-angle specification determines the brake rate

A rotor initially turns at 12rad/s12\,\mathrm{rad/s}. It must stop after exactly 18rad18\,\mathrm{rad} under constant angular acceleration.

Diagram shown in the original SVG worksheet.

  1. Find the acceleration and stopping time.

  2. If the same signed acceleration continues for two more seconds, find the additional signed displacement.

Question 1 - Solution

A stopping-angle specification determines the brake rate

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Eliminate time during the stopping phase: ωf2=ω02+2αΔθ,0=144+36α⇒α=−4rad/s2.\omega_f^2=\omega_0^2+2\alpha\Delta\theta, \qquad 0=144+36\alpha\Rightarrow\boxed{\alpha=-4\ \mathrm{rad/s^2}}. ts=0−12−4=3s.t_s=\frac{0-12}{-4}=\boxed{3\ \mathrm s}.

(b) Result and interpretation

Start a new time interval at the stopping instant. If the same signed acceleration persists, Δθextra=0(2)+12(−4)(2)2=−8rad,ωf=(−4)(2)=−8rad/s.\Delta\theta_{\mathrm{extra}}=0(2)+\tfrac12(-4)(2)^2=\boxed{-8\ \mathrm{rad}},\qquad \omega_f=(-4)(2)=-8\ \mathrm{rad/s}. This model reverses the motion; a brake that holds the rotor at rest would instead change its torque after stopping.

Physical check

The stopping area is 12(3)(12)=18\tfrac12(3)(12)=18 rad, as required.