9.7. Rolling Energy Problems http://www.ck12.org
Ei=Ef
PE=KE+KErot start with conservation of energymgh=1
2
mv^2 +1
2
Iω^2 substitute the proper value for each energy termmgh=1
2
mv^2 +1
2
mr^2 ω^2 substitute in the moment of inertia of the hoopmgh=1
2
m(ωr)^2 +1
2
mr^2 ω^2 we can putvin terms of omega because the hoop is rolling without sliding2 gh= (ωr)^2 +r^2 ω^2 now we will multiply by 2 and divide by m to simplify the equation
2 gh= 2 ω^2 r^2ω=√
gh
r
solving forωω=√
9 .8 m/s^2 ∗3 m
.75 m
plug in the known values
ω= 7 .2 rad/sWatch this Explanation
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- Your bike brakes went out! You put your feet on the wheel to slow it down. The rotational kinetic energy of
the wheel begins to decrease. Where is this energy going?