Dynamics: planar kinetics of a rigid body (impulse and momentum)

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SUMMARY

The discussion focuses on calculating the angular velocity of a spool subjected to a horizontal force while rolling without slipping. Given parameters include an inner radius of 0.3 m, an outer radius of 0.9 m, a weight of 300 N, and a radius of gyration of 0.45 m. The correct angular velocity after 4 seconds, starting from rest, is determined to be 1.94 rad/s. The key takeaway is that moments should be taken about the center of rotation (point A) rather than the center of mass (point O) to simplify the analysis and avoid accounting for friction torque.

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silentwf
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Homework Statement


http://img340.imageshack.us/img340/7379/87835960.png
r_{i}=.3 m \text{ and } r_{o}=.9 m
The spool has a weight of 300N and a radius of gyration k_{O} = .45 m. A cord is wrapped around its inner hub and the end subjected to a horizontal force P = 50N. Determine the spool's angular velocity in 4seconds starting from rest. Assume the spool rolls without slipping.


Homework Equations


\int_{0}^{t}{P\cdot r_{i}}{dt} = mv_{O}r_{i} + I_{O}\omega


The Attempt at a Solution


\left \{ \begin{matrix}\int_{0}^{4}{50 \cdot 0.3}{dt} = \frac{300}{9.81}\cdot v_{O}\cdot0.9 + \frac{300}{9.81}\cdot 0.45^{2} \cdot \omega\\v_{O}=0.9\omega\end{matrix}
Solving the two equations i get \omega = 1.94 \text{rad/s}

The book provides the solution as follows
\left \{ \begin{matrix}<br /> 50(0.9 - 0.3)4 = \frac{300}{9.81}v_{O}\cdot 0.9+\frac{300}{9.81}\cdot.45^{2}\omega \\<br /> v_{O}=\omega\cdot0.9 \end{matrix}
I don't get why the book does .9 - .3 for its radius, i thought it was around point O?
 
Last edited by a moderator:
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Hi silentwf! :smile:

(have an omega: ω and an integral: ∫ :wink:)
silentwf said:
Assume the spool rolls without slipping.

\int_{0}^{t}{P\cdot r_{i}}{dt} = mv_{O}r_{i} + I_{O}\omega

I don't get why the book does .9 - .3 for its radius, i thought it was around point O?

[STRIKE]You can't take moments about the centre of mass (O) when it is accelerating.

But you can always take moments about the centre of rotation (A).[/STRIKE]

If you take moments about the centre of mass (O), you need to take the torque of the friction force at A into account.

To avoid that, use A instead of O, so that the friction torque is zero.

So all you need is the torque of P about A, for which the distance is 0.6 :wink:
 
Last edited:
oops!

I've changed my mind …

the conclusion of my last post is still correct (that you must take moments about A, not about O), but the reasoning wasn't, so I've edited it. :redface:
 

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