An Angular Simple Harmonic Oscillator — Question 4

Section 15-4 · Physics pages 2298–2299

Question 4 A tangential impulse launches angular oscillation A disk on a torsional suspension is initially at its untwisted equilibrium and at rest. Its inertia is I = .020 kg m2 and stiffness κ = .50 N m/rad. A brief tangential impulse J = .10 N s acts at radius R = .20 m. I κ Torsional oscillator schematic; the suspension defines a fixed vertical axis. (a) Find the initial angular speed and ensuing twist amplitude. (b) Find the maximum restoring torque and verify the oscillator energy using both the initial angular motion and the turning point.
Show solutionHide solution
Question 4 - Solution A tangential impulse launches angular oscillation I κ (a) Derivation and calculation For a tangential impulse, ∆L = RJ = (.20)(.10) = .0200 kg m2/s. I ˙θ+ = RJ ⇒˙θ+ = 1.00 rad/s . Ω= √ κ/I = √ .50/.020 = 5.00 rad/s, θA = ˙θ+/Ω= .200 rad . (b) Result and interpretation |τ|max = κθA = .100 N m , E = 1 2I ˙θ2 + = 1 2κθ2 A = .0100 J . ∆L = r × J, J ∥r ⇒∆L = 0. A radial impulse therefore does not launch torsional oscillation about the axis. Physical check The impulse changes angular velocity while angular position remains continuous.

Question 4

A tangential impulse launches angular oscillation

A disk on a torsional suspension is initially at its untwisted equilibrium and at rest. Its inertia is I=.020kgm2I=.020\,\mathrm{kg\,m^2} and stiffness κ=.50Nm/rad\kappa=.50\,\mathrm{N\,m/rad}. A brief tangential impulse J=.10NsJ=.10\,\mathrm{N\,s} acts at radius R=.20mR=.20\,\mathrm{m}.

Diagram shown in the original SVG worksheet.

  1. Find the initial angular speed and ensuing twist amplitude.

  2. Find the maximum restoring torque and verify the oscillator energy using both the initial angular motion and the turning point.

Question 4 - Solution

A tangential impulse launches angular oscillation

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

For a tangential impulse,ΔL=RJ=(.20)(.10)=.0200kgm2/s.\Delta L=RJ=(.20)(.10)=.0200\,\mathrm{kg\,m^2/s}.Iθ̇+=RJ⇒θ̇+=1.00rad/s.I\dot\theta_+=RJ\Rightarrow\boxed{\dot\theta_+=1.00\,\mathrm{rad/s}}.Ω=κ/I=.50/.020=5.00rad/s,θA=θ̇+/Ω=.200rad.\Omega=\sqrt{\kappa/I}=\sqrt{.50/.020}=5.00\,\mathrm{rad/s},\quad\boxed{\theta_A=\dot\theta_+/\Omega=.200\,\mathrm{rad}}.

(b) Result and interpretation

|τ|max=κθA=.100Nm,E=12Iθ̇+2=12κθA2=.0100J.\boxed{|\tau|_{\max}=\kappa\theta_A=.100\,\mathrm{N\,m}},\qquad\boxed{E=\tfrac12I\dot\theta_+^2=\tfrac12\kappa\theta_A^2=.0100\,\mathrm J}.Δ𝑳=𝒓×𝑱,J∥𝒓⇒ΔL=0.\Delta\mathbf L=\mathbf r\times\mathbf J,\qquad J\parallel\mathbf r\Rightarrow\Delta L=0.A radial impulse therefore does not launch torsional oscillation about the axis.

Physical check

The impulse changes angular velocity while angular position remains continuous.