An Angular Simple Harmonic Oscillator — Question 7

Section 15-4 · Physics pages 2304–2305

Question 7 An unanchored torsional pair has a free overall rotation Two coaxial rotors of inertias I1 and I2 are joined by a torsional spring of constant κ. Neither rotor is attached to a fixed angular reference. Let q = θ2 −θ1 be the spring twist. External torque is zero. I1 I2 κ Two unanchored rotors exchange equal and opposite torsional moments. (a) Derive the twist oscillation frequency. (b) If total angular momentum is zero and I2 = 3I1, find the ratio of angular amplitudes. How does nonzero total angular momentum alter the motion?
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Question 7 - Solution An unanchored torsional pair has a free overall rotation I1 I2 κ (a) Derivation and calculation I1¨θ1 = κq, I2¨θ2 = −κq, q = θ2 −θ1. ¨q = −κ ( 1 I1 + 1 I2 ) q. Ω= √ κ/Ired , Ired = I1I2 I1 + I2 . (b) Result and interpretation L = I1 ˙θ1 + I2 ˙θ2 = constant, ˙Θ = L I1 + I2 . δθ1 = − I2q I1 + I2 , δθ2 = I1q I1 + I2 . I2 = 3I1 ⇒A1/A2 = 3 . The oscillatory parts are opposite in phase; common rotation may be superposed. Physical check Internal spring torques cannot change the total angular momentum.

Question 7

An unanchored torsional pair has a free overall rotation

Two coaxial rotors of inertias I1I_1 and I2I_2 are joined by a torsional spring of constant κ\kappa. Neither rotor is attached to a fixed angular reference. Let q=θ2−θ1q=\theta_2-\theta_1 be the spring twist. External torque is zero.

Diagram shown in the original SVG worksheet.

  1. Derive the twist oscillation frequency.

  2. If total angular momentum is zero and I2=3I1I_2=3I_1, find the ratio of angular amplitudes. How does nonzero total angular momentum alter the motion?

Question 7 - Solution

An unanchored torsional pair has a free overall rotation

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

I1θ̈1=κq,I2θ̈2=−κq,q=θ2−θ1.I_1\ddot\theta_1=\kappa q,\qquad I_2\ddot\theta_2=-\kappa q,\qquad q=\theta_2-\theta_1.q̈=−κ(1I1+1I2)q.\ddot q=-\kappa\left(\frac1{I_1}+\frac1{I_2}\right)q.Ω=κ/Ired,Ired=I1I2I1+I2.\boxed{\Omega=\sqrt{\kappa/I_{\mathrm{red}}}},\qquad I_{\mathrm{red}}=\frac{I_1I_2}{I_1+I_2}.

(b) Result and interpretation

L=I1θ̇1+I2θ̇2=constant,Θ̇=LI1+I2.L=I_1\dot\theta_1+I_2\dot\theta_2=\text{constant},\qquad\dot\Theta=\frac L{I_1+I_2}.δθ1=−I2qI1+I2,δθ2=I1qI1+I2.\delta\theta_1=-\frac{I_2q}{I_1+I_2},\quad\delta\theta_2=\frac{I_1q}{I_1+I_2}.I2=3I1⇒A1/A2=3.I_2=3I_1\Rightarrow\boxed{A_1/A_2=3}.The oscillatory parts are opposite in phase; common rotation may be superposed.

Physical check

Internal spring torques cannot change the total angular momentum.