Angular speed of merry-go-round

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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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The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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