An Angular Simple Harmonic Oscillator — Question 2

Section 15-4 · Physics pages 2294–2295

Question 2 Moving identical masses outward isolates a torsion balance inertia A torsion balance has unknown bare inertia I0 and stiffness κ. Two point masses, each m = .050 kg, are placed symmetrically at radius r. Squared periods are T 2 1 = 1.00 s2 at r1 = .10 m and T 2 2 = 1.60 s2 at r2 = .20 m. r m m Two equal added masses lie symmetrically about the rotation axis. (a) Infer κ and I0. (b) Predict the period without the point masses. Explain why period squared is linear in r2, not in r.
Show solutionHide solution
Question 2 - Solution Moving identical masses outward isolates a torsion balance inertia r m m (a) Derivation and calculation I(r) = I0 + 2mr2, T 2 = 4π2 κ (I0 + 2mr2). ∆I = 2(.050)(.202 −.102) = .00300 kg m2. κ = 4π2∆I 1.60 −1.00 = .197392 N m/rad . (b) Result and interpretation I0 = κT 2 1 4π2 −2mr2 1 = .00500 −.00100 = .00400 kg m2 . T 2 0 = 4π2I0 κ = .800 s2, T0 = .89443 s . Physical check The bare inertia is positive and the bare period is shorter than either loaded period.

Question 2

Moving identical masses outward isolates a torsion balance inertia

A torsion balance has unknown bare inertia I0I_0 and stiffness κ\kappa. Two point masses, each m=.050kgm=.050\,\mathrm{kg}, are placed symmetrically at radius rr. Squared periods are T12=1.00s2T_1^2=1.00\,\mathrm{s^2} at r1=.10mr_1=.10\,\mathrm{m} and T22=1.60s2T_2^2=1.60\,\mathrm{s^2} at r2=.20mr_2=.20\,\mathrm{m}.

Diagram shown in the original SVG worksheet.

  1. Infer κ\kappa and I0I_0.

  2. Predict the period without the point masses. Explain why period squared is linear in r2r^2, not in rr.

Question 2 - Solution

Moving identical masses outward isolates a torsion balance inertia

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

I(r)=I0+2mr2,T2=4π2κ(I0+2mr2).I(r)=I_0+2mr^2,\qquad T^2=\frac{4\pi^2}{\kappa}(I_0+2mr^2).ΔI=2(.050)(.202−.102)=.00300kgm2.\Delta I=2(.050)(.20^2-.10^2)=.00300\,\mathrm{kg\,m^2}.κ=4π2ΔI1.60−1.00=.197392Nm/rad.\boxed{\kappa=\frac{4\pi^2\Delta I}{1.60-1.00}=.197392\,\mathrm{N\,m/rad}}.

(b) Result and interpretation

I0=κT124π2−2mr12=.00500−.00100=.00400kgm2.I_0=\frac{\kappa T_1^2}{4\pi^2}-2mr_1^2=.00500-.00100=\boxed{.00400\,\mathrm{kg\,m^2}}.T02=4π2I0κ=.800s2,T0=.89443s.T_0^2=\frac{4\pi^2 I_0}{\kappa}=.800\,\mathrm{s^2},\qquad\boxed{T_0=.89443\,\mathrm s}.

Physical check

The bare inertia is positive and the bare period is shorter than either loaded period.