Freye
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1. A 4.5m diameter merry-go-round is rotating freely with an angular velocity of 0.70 rad/s; its total moment of inertia is 1750 kg X m/s^2. Four people standing on the ground each of 65 kg mass suddenly step onto the edge of the merry-go-round.
a) What will be the angular velocity of the merry-go-round now? b)What if the people were on it initially, and then jumped off?
r= d/2 = 4.5/2 = 2.25m
w_{}1= 0.70 rad/s
I_{}1= 1750kg X m^2
I_{}people = 65 X 4 X 2.25^2 = 1316.25kg X m^2
I_{}2= I_{}1 + I_{}people = 3066.25 Kg X m^2
2. I_{}1w_{}1 = I_{}2w_{}2
T=rFsin\theta
T=I\alpha
3. The correct answers as they are given in the back of the book are a) w_{}2=0.40rad/s and b)no change (if jump off radially)
a)
w_{2} = I_{}1w_{}1/I_{}2
= (1750)(.07)/(3066.25)
= 0.40 rad/s [the correct answer]
b)
w_{}1= 0.40 rad/s [from part a)]
I_{}1 and I_{}2 from part a) switch places
w_{}2=I_{}1w_{}1/I_{}2
w_{}2 = (3066.25)(0.40)/(1750)
w_{}2= 0.70 rad/s [which is to be expected, however apparently incorrect]
At this point, I realized that for some reason the conservation of angular momentum must not apply in this scenario, and so I did
\theta = 0degrees (the angle between the radius and the applied force, assuming they jump of radially)
T=rfsin\theta=0
\alpha=T/I
\alpha=0
Therefore \Deltaw=0 [the correct answer]
Essentially, my question is why the law of conservation of angular momentum applies when people step onto the merry-go-round, but not when they step off? I know I am making some sort of obvious logical blunder, but I cannot see it :(.
a) What will be the angular velocity of the merry-go-round now? b)What if the people were on it initially, and then jumped off?
r= d/2 = 4.5/2 = 2.25m
w_{}1= 0.70 rad/s
I_{}1= 1750kg X m^2
I_{}people = 65 X 4 X 2.25^2 = 1316.25kg X m^2
I_{}2= I_{}1 + I_{}people = 3066.25 Kg X m^2
2. I_{}1w_{}1 = I_{}2w_{}2
T=rFsin\theta
T=I\alpha
3. The correct answers as they are given in the back of the book are a) w_{}2=0.40rad/s and b)no change (if jump off radially)
a)
w_{2} = I_{}1w_{}1/I_{}2
= (1750)(.07)/(3066.25)
= 0.40 rad/s [the correct answer]
b)
w_{}1= 0.40 rad/s [from part a)]
I_{}1 and I_{}2 from part a) switch places
w_{}2=I_{}1w_{}1/I_{}2
w_{}2 = (3066.25)(0.40)/(1750)
w_{}2= 0.70 rad/s [which is to be expected, however apparently incorrect]
At this point, I realized that for some reason the conservation of angular momentum must not apply in this scenario, and so I did
\theta = 0degrees (the angle between the radius and the applied force, assuming they jump of radially)
T=rfsin\theta=0
\alpha=T/I
\alpha=0
Therefore \Deltaw=0 [the correct answer]
Essentially, my question is why the law of conservation of angular momentum applies when people step onto the merry-go-round, but not when they step off? I know I am making some sort of obvious logical blunder, but I cannot see it :(.