Moments of Inertia, Kinetic Energy and rotations

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Homework Help Overview

The problem involves a bicycle racer whose wheel detaches while descending a hill. The scenario requires calculating the final speed of the wheel and its total kinetic energy upon reaching the bottom, considering the wheel's properties as a thin-walled cylinder and the principles of energy conservation.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the conservation of energy and the relationship between translational and rotational kinetic energy. There is uncertainty about how to apply the equations correctly, particularly regarding the initial and final energy states. Some participants question the assumptions about the wheel's motion and the relevance of the height from which it descends.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the energy conservation principle. Some guidance has been offered regarding the initial energy components, but there is no explicit consensus on the correct approach to the problem.

Contextual Notes

Participants note confusion regarding the relationship between linear and angular velocities, as well as the role of potential energy in the calculations. There is also mention of the initial speed of the bike and its impact on the total energy considerations.

lsatwd
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Homework Statement


A bicycle racer is going downhill at 11.0 m/s when, to his horror, one of his 2.25 kg wheels comes off when he is 75.0 m above the foot of the hill. We can model the wheel as a thin-walled cylinder 85.0 cm in diameter and neglect the small mass of the spokes.

How fast is the wheel moving when it reaches the foot of the hill if it rolled without slipping all the way down? How much total kinetic energy does the wheel have when it reaches the bottom of the hill?

Homework Equations


I think...
mgy = 1/2*m*v^2 + 1/2*I*w^2
I=mr^2
v=rw ("w" is supposed to be angular velocity)

The Attempt at a Solution



I'm totally stumped by part A. I just don't see how i can solve for its final speed without knowing the time or the degree. I'm also assuming the question is asking for its linear speed since it wants the answer in m/s.

I thought about using mgy = 1/2*m*v^2 + 1/2*I*w^2
= squareroot{4gy} = v

but this didn't work and I was thinking that this didn't work because the wheel isn't falling straight down from a height of 75 m, but rather rolling down from what would be the hypotenuse of a triangle with that height...but i understand a triangle isn't needed in this problem. (but I'm not sure)

I then tried finding the angular velocity by using the given speed of the wheel, 11 m/s (which i assumed to be equal to the linear velocity of the wheel) by using the equation v=rw ([11m/2]/.425 = w) which gave me a value of 25.88 rad/s to plug into the equation: 1/2*2.25kg*11^2 + 1/2(2.25*.425^2)25.88^2 = 136.30 J for total kinetic energy... but this was incorrect. I'm also not sure why the total kinetic energy isn't just mgy which would equal 1653.75 J; this number is a lot bigger than 136.30 and I'm just really confused :mad:
 
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mgy = 1/2*m*v^2 + 1/2*I*w^2
I=mr^2
This doesn't look right. Conservation of energy means that

Initial energy = final energy

So for starters, what is the initial energy? Remember that the bike was going 11.0 m/s initially.

I then tried finding the angular velocity ... by using the equation v=rw
Yes, that is helpful to relate v and w.
 
I was thinking that its total initial energy would be the sum of its translational and rotational kinetic energy so that is why i thought i could use that equation.

I don't know what to use if that's not it.
 
lsatwd said:
I was thinking that its total initial energy would be the sum of its translational and rotational kinetic energy ...

In addition to that, potential energy should be part of the sum also.
 

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