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

AI Thread Summary
The discussion focuses on solving a dynamics problem involving a spool subjected to a horizontal force while rolling without slipping. The key equations involve the relationship between the applied force, the spool's angular velocity, and the moment of inertia. A critical point raised is the necessity to calculate moments about the center of rotation (point A) rather than the center of mass (point O) due to acceleration. This approach eliminates the need to account for friction torque, simplifying the calculations. The final solution for the spool's angular velocity is determined to be approximately 1.94 rad/s.
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?
 
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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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