Pendulums — Question 4

Section 15-5 · Physics pages 2318–2319

Question 4 Two different pivots can give the same physical-pendulum period A body has radius of gyration kg = .20 m. It can hang from pivots on the same line through its center of mass, each above the center in its own hanging configuration. One pivot distance is d1 = .10 m. Use the effective length ℓeff= d + k2 g/d. pivot CM d Physical pendulum: the pivot-to-center-of-mass distance controls both inertia and restoring torque. (a) Find a distinct pivot distance d2 giving the same small-angle period. (b) Find the common effective length and period for g = 10 m/s2. Derive the product relation between distinct equal-period pivot distances.
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Question 4 - Solution Two different pivots can give the same physical-pendulum period pivot CM d (a) Derivation and calculation Equal periods require equal effective lengths: Leff= d + k2 g d . kg = .200, d1 = .100 : Leff= .100 + .0400 .100 = .500 m. d2 −.500d + .0400 = 0 ⇒d = .100 or .400 m. (b) Result and interpretation d2 = .400 m , T = 2π √ .500/10 = 1.40496 s . d1 + k2 g d1 = d2 + k2 g d2 ⇒(d1 −d2) ( 1 −k2 g d1d2 ) = 0. d1̸ = d2 ⇒d1d2 = k2 g . Physical check The two distances lie on opposite sides of the minimum-period distance d = kg.

Question 4

Two different pivots can give the same physical-pendulum period

A body has radius of gyration kg=.20mk_g=.20\,\mathrm{m}. It can hang from pivots on the same line through its center of mass, each above the center in its own hanging configuration. One pivot distance is d1=.10md_1=.10\,\mathrm{m}. Use the effective length ℓeff=d+kg2/d\ell_{\mathrm{eff}}=d+k_g^2/d.

Diagram shown in the original SVG worksheet.

  1. Find a distinct pivot distance d2d_2 giving the same small-angle period.

  2. Find the common effective length and period for g=10m/s2g=10\,\mathrm{m/s^2}. Derive the product relation between distinct equal-period pivot distances.

Question 4 - Solution

Two different pivots can give the same physical-pendulum period

Diagram shown in the original SVG worksheet.

(a) Derivation and calculation

Equal periods require equal effective lengths:Leff=d+kg2d.L_{\mathrm{eff}}=d+\frac{k_g^2}{d}.kg=.200,d1=.100:Leff=.100+.0400.100=.500m.k_g=.200,\ d_1=.100:\quad L_{\mathrm{eff}}=.100+\frac{.0400}{.100}=.500\,\mathrm m.d2−.500d+.0400=0⇒d=.100or.400m.d^2-.500d+.0400=0\Rightarrow d=.100\ \text{or}\ .400\,\mathrm m.

(b) Result and interpretation

d2=.400m,T=2π.500/10=1.40496s.\boxed{d_2=.400\,\mathrm m},\qquad\boxed{T=2\pi\sqrt{.500/10}=1.40496\,\mathrm s}.d1+kg2d1=d2+kg2d2⇒(d1−d2)(1−kg2d1d2)=0.d_1+\frac{k_g^2}{d_1}=d_2+\frac{k_g^2}{d_2}\Rightarrow(d_1-d_2)\left(1-\frac{k_g^2}{d_1d_2}\right)=0.d1≠d2⇒d1d2=kg2.d_1\ne d_2\Rightarrow\boxed{d_1d_2=k_g^2}.

Physical check

The two distances lie on opposite sides of the minimum-period distance d=kgd=k_g.