Work and Rotational Kinetic Energy — Question 9

Section 10-9 · Physics pages 1548–1549

Question 9 Torsional spring work reveals a reduced opposite turning angle A rotor of inertia 0.50 kg m2 is attached to a torsional spring exerting τs = −kθ, with k = 4 N m/rad. It is released from rest at θ = 1 rad. A constant resisting torque of magnitude 0.50 N m opposes motion; static capacity is no larger than this value. θ τs −kθ Linear restoring torque; bearing resistance is a separate contribution. (a) Derive the spring energy and find angular speed at θ = 0. (b) Find the first negative turning angle, accounting for total angular travel.
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Question 9 - Solution Torsional spring work reveals a reduced opposite turning angle θ τs −kθ (a) Derivation and calculation Define spring energy by the negative work of its restoring torque: U(θ) −U(0) = − ∫θ 0 (−kq) dq = 1 2kθ2 . The spring torque initially exceeds static resistance, so motion begins toward decreasing angle. At zero angle, K(0) = 1 2(4)(1)2 −(0.50)(1) = 1.50 J. |ω(0)| = √ 2K/I = √ 6 = 2.449 rad/s , ω(0) < 0. (b) Result and interpretation Write the first negative turning angle as −a with a > 0. The travel from +1 to −a is 1 + a, so 2 = 1 2(4)a2 + 0.50(1 + a) ⇒2a2 + 0.50a −1.50 = 0. (a + 1)(2a −1.50) = 0 ⇒a = 0.75 , θt = −0.75 rad . The root a = −1 is not a negative-side amplitude. Physical check At the turn, spring energy is 1.125 J and dissipation is 0.875 J, totaling the initial 2 J.

Question 9

Torsional spring work reveals a reduced opposite turning angle

A rotor of inertia 0.50kgm20.50\,\mathrm{kg\,m^2} is attached to a torsional spring exerting τs=−kθ\tau_s=-k\theta, with k=4Nm/radk=4\,\mathrm{N\,m/rad}. It is released from rest at θ=1rad\theta=1\,\mathrm{rad}. A constant resisting torque of magnitude 0.50Nm0.50\,\mathrm{N\,m} opposes motion; static capacity is no larger than this value.

Diagram shown in the original SVG worksheet.

  1. Derive the spring energy and find angular speed at θ=0\theta=0.

  2. Find the first negative turning angle, accounting for total angular travel.

Question 9 - Solution

Torsional spring work reveals a reduced opposite turning angle

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Define spring energy by the negative work of its restoring torque: U(θ)−U(0)=−∫0θ(−kq)dq=12kθ2.U(\theta)-U(0)=-\int_0^\theta(-kq)\,dq=\boxed{\frac12k\theta^2}. The spring torque initially exceeds static resistance, so motion begins toward decreasing angle. At zero angle, K(0)=12(4)(1)2−(0.50)(1)=1.50J.K(0)=\tfrac12(4)(1)^2-(0.50)(1)=1.50\ \mathrm J. |ω(0)|=2K/I=6=2.449rad/s,ω(0)<0.\boxed{|\omega(0)|=\sqrt{2K/I}=\sqrt6=2.449\ \mathrm{rad/s}},\qquad\omega(0)<0.

(b) Result and interpretation

Write the first negative turning angle as −a-a with a>0a>0. The travel from +1+1 to −a-a is 1+a1+a, so 2=12(4)a2+0.50(1+a)⇒2a2+0.50a−1.50=0.2=\frac12(4)a^2+0.50(1+a)\Rightarrow 2a^2+0.50a-1.50=0. (a+1)(2a−1.50)=0⇒a=0.75,θt=−0.75rad.(a+1)(2a-1.50)=0\Rightarrow\boxed{a=0.75},\qquad \boxed{\theta_t=-0.75\ \mathrm{rad}}. The root a=−1a=-1 is not a negative-side amplitude.

Physical check

At the turn, spring energy is 1.125 J and dissipation is 0.875 J, totaling the initial 2 J.