2007: Problems 31-33

Topic: Rigid Bodies
Concepts: Moments of inertia


Solution:

Recall the moment of inertia of a rod about its center is

I=112mL2I=\frac{1}{12}mL^2

We are given I=md2I=md^2 which means

112L2=d2\frac{1}{12}L^2=d^2
Ld=12=23\frac{L}{d}=\sqrt{12}=2\sqrt{3}

so the answer is D.

Topic: Oscillatory Motion
Concepts: Parallel-axis theorem, Physical pendulum


Solution:

Recall the angular frequency of a physical pendulum is given by

ω=mgsI\omega=\sqrt{\frac{mgs}{I}}

where ss is the distance between the CM and the pivot point and II is the moment of inertia around the pivot point. In our case, we have

s=kds=kd
I=md2+m(kd)2=(1+k2)md2I=md^2+m(kd)^2=(1+k^2)md^2

using Irod=md2I_{\text{rod}}=md^2 (by definition of dd in the problem) and the parallel-axis theorem. Then

ω=mgkd(1+k2)md2=k1+k2gd\omega=\sqrt{\frac{mgkd}{(1+k^2)md^2}}=\sqrt{\frac{k}{1+k^2}}\sqrt{\frac{g}{d}}

Since we are given

ω=βgd\omega=\beta\sqrt{\frac{g}{d}}

we can identify

β=k1+k2\beta=\sqrt{\frac{k}{1+k^2}}

so the answer is E.

Topic: Oscillatory Motion
Concepts: Physical pendulum


Solution:

From the previous problem, we have

β=k1+k2\beta=\sqrt{\frac{k}{1+k^2}}

To maximize β\beta, we can equivalently minimize 1/β21/\beta^2:

1β2=1+k2k=k+1k\frac{1}{\beta^2}=\frac{1+k^2}{k}=k+\frac{1}{k}

which occurs at k=1k=1. Thus,

βmax=11+12=12\beta_{\text{max}}=\sqrt{\frac{1}{1+1^2}}=\frac{1}{\sqrt{2}}

so the answer is C.

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