A spinning top - moment of inertia/ Torque/ Angular momentum

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SUMMARY

The discussion focuses on the physics principles of torque, moment of inertia, and angular momentum as they relate to a spinning top. The torque is defined as \(\vec{T} = \vec{r} \times m\vec{g}\), where \(\vec{r}\) is expressed as \(d\hat{r}\). Participants clarify that the moment of inertia should be plugged into the equations provided in the assignment, and the relationship between angular speed \(\Omega\) and the vectors involved is emphasized. The conversation highlights the complexity of integrating these concepts in solving the assignment questions.

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  • Understanding of torque as a vector quantity
  • Familiarity with moment of inertia in rotational dynamics
  • Knowledge of angular momentum and its conservation
  • Basic vector calculus, particularly cross products
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  • Study the relationship between torque and angular momentum using \(\vec{T} = \frac{d\vec{L}}{dt}\)
  • Learn how to calculate moment of inertia for various shapes and systems
  • Explore the dynamics of rotating bodies, focusing on gyroscopic effects
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Theknight330
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Hey guys,

I have this really annoying last question on my assignment which is a pain. It combines 3 physics principles together.


I am having problems specifically with 2) 3) and 4)

2)I know that T = | r x F |, but what kind of general vector do I use to represent F?
4) I have no clue how to do this one unfortunately.

The question should be in the attached thumbnail
 

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The only force acting on the top is gravity.
 
For part b, note that torque is a vector: \vec{T}=\vec{r}\times m\vec{g} as the torque is calculated about the origin. You can express \vec{r}=d\hat{r}.

For part c, the problem has already given you the answer. Just plug moment of inertial in.

For part d, again, the problem has already shown you the way. Substitute L and T found earlier in the equation: \vec{T}=d\vec{L}/dt. You have known that the top will rotate around the Y axis beside spinning very fast about its own axis of symmetry (because of this "very fast" spin, we can achieve L as in part c). That means the \hat{r} vector will rotate around the Y axis just like the shaft. If so, then how would you relate d\hat{r}/dt , the angular speed of the rotation about the Y axis \Omega and the vector \hat{r} \times \hat{g}. Note that \hat{g} is only a unit vector whose direction is downward, nothing special. Find \Omega and then the time needed.
 
Nice one Jong trying to get the internet to solve the final question.
 
hahahahhaa oh that's classic mate!
 
hey clive this doesn't help at all so stop trying to get the answer from it.
 

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