2014: Problem 21

Topic: System of Masses
Concepts: Atwood machine, Moments of inertia, Pulleys with rotational inertia


Solution:

We first find the acceleration in an Atwood machine where the pulley has moment of inertia II. Applying Newton’s 2nd law to each mass and the pulley,

T1mg=maT_1-mg=ma
MgT2=MaMg-T_2=Ma
τ=T2RT1R=Iα\tau=T_2R-T_1R=I\alpha

Assuming there is no slipping α=a/R\alpha=a/R, we have

T2T1=IaR2T_2-T_1=\frac{Ia}{R^2}

Adding this equation and the first two equations yields

Mgmg=ma+Ma+IaR2Mg-mg=ma+Ma+\frac{Ia}{R^2}

so the acceleration is

a=Mmm+M+I/R2ga=\frac{M-m}{m+M+I/R^2}g

The ratio between the accelerations in systems AA and BB is

aAaB=(Mm)gm+M+IA/R2m+M+IB/R2(Mm)g=(m+M)R2+IB(m+M)R2+IA\frac{a_A}{a_B}=\frac{(M-m)g}{m+M+I_A/R^2}\frac{m+M+I_B/R^2}{(M-m)g}=\frac{(m+M)R^2+I_B}{(m+M)R^2+I_A}

Since pulley AA has mass m+Mm+M and is a uniform disk,

IA=12(m+M)R2I_A=\frac{1}{2}(m+M)R^2

The mass of a disk is proportional to its area mr2m \propto r^2 so a disk with radius r/2r/2 has mass m/4m/4. Thus, the moment of inertia of the removed hole is

Ihole=12(m+M)4(R2)2=IA16I_{\text{hole}}=\frac{1}{2}\frac{(m+M)}{4}\left(\frac{R}{2}\right)^2=\frac{I_A}{16}

so for pulley BB,

IB=IAIhole=1516IA=1532(m+M)R2I_B=I_A-I_{\text{hole}}=\frac{15}{16}I_A=\frac{15}{32}(m+M)R^2

Substituting this into the ratio of accelerations,

aAaB=(m+M)R2+(15/32)(m+M)R2(m+M)R2+(1/2)(m+M)R2=1+(15/32)1+(1/2)=47/323/2=4748\frac{a_A}{a_B}=\frac{(m+M)R^2+(15/32)(m+M)R^2}{(m+M)R^2+(1/2)(m+M)R^2}=\frac{1+(15/32)}{1+(1/2)}=\frac{47/32}{3/2}=\frac{47}{48}

so the answer is A.

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