Angular speed of merry-go-round

AI Thread Summary
A playground merry-go-round with a radius of 2.40 m and a moment of inertia of 2100 kgm^2 is initially at rest. A child applies an 18.0 N force tangentially for 15.0 seconds, resulting in an angular speed of 0.309 rad/s. The torque generated by the force is calculated as 43.2 N·m, leading to an angular acceleration of 0.021 rad/s². Using the relationship between angular acceleration and time, the final angular speed is determined. The calculations illustrate the application of rotational dynamics principles in solving the problem.
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Homework Statement


A playground merry-go-round has a radius 2.40 m and a moment of inertia 2100 kgm^2 about a vertical axle through its center, and it turns with negligible friction.

A child applies an 18.0 N force tangential to the edge of the merry-go-round for 15.0 s. If the merry-go-round is initially at rest, what is its angular speed after this 15.0 s interval?


Homework Equations


\vec \tau = \vec r \times \vec F

The Attempt at a Solution



I have absolutely no idea what to do. I know the answer is .309 rad/s. From playing around with the numbers I know that (2.40 m * 18.0 N * 15.0 s)/2100 kg*m^2 = 0.309 rad/s, but I don't know why. I can't find any sort of relationship between what I have and what I need.
 
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Immediately after clicking post, it clicked in my mind. Wow. For anyone else who is having trouble with this problem:

<br /> \begin{array}{l}<br /> \vec \tau = \vec r \times \vec F\\<br /> \sum \vec \tau = I \vec \alpha\\<br /> \omega_f = \omega_i + \alpha t\\\\<br /> \vec \tau = (2.40 m)(18.0 N)(sin 90) = 43.2 N \cdot m\\<br /> \sum \vec \tau = 43.2 N \cdot m = (2100 kg \cdot m^2)(\alpha)\\<br /> \Rightarrow \alpha = 0.021 rad/s^2\\<br /> \omega_f = 0 + (0.021 rad/s^2)(15.0 s)\\<br /> \Rightarrow \omega_f = 0.309 rad/s<br /> \end{array}<br />
 
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