2007: Problem 10

Topic: Rigid Bodies
Concepts: Rotational Newton’s 2nd law


Solution:

Recall for rotational motion,

τ=Iα\tau=I\alpha

We are given the moment of inertia of the wheel:

I=mR2I=mR^2

The force is applied perpendicular to the moment arm:

τ=FR\tau=FR

Thus,

FR=mR2αFR=mR^2\alpha
F=mRαF=mR\alpha

Both wheels have the same mass, so for both to have the same angular acceleration,

FRF \propto R

Hence,

R2=2R1R_2=2R_1
F2=2F1=2NF_2=2F_1=2 \,\mathrm{N}

so the answer is D.

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