Rotational Motion Final Angular Speed Calculation

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The discussion revolves around calculating the final angular speed of an object with rotational inertia I, initially at rest, after a torque is applied for one-quarter of a revolution. The torque is defined as τ = A cos(Θ), where A is a constant and Θ is the angle of rotation. The work-energy principle is applied, leading to the equation W = ΔK, which is integrated to find the relationship between torque and angular speed. The correct evaluation of the integral reveals that the final angular speed is ω = √(2A/I), correcting an earlier miscalculation. The importance of accurate integral evaluation in deriving the final formula is emphasized.
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Homework Statement



An object of rotational inertia I is initially at rest. A torque is then applied to the object, causing it to begin rotating. The torque is applied for only one-quarter of a revolution, during which time its magnitude is given by \tau =Acos\Theta , where A is a constant and /Theta is the angle through which the object has rotated. What is the final angular speed of the object?

Homework Equations

The Attempt at a Solution



##W=\Delta K\\ \int _{ 0 }^{ \frac { \pi }{ 2 } }{ \tau d\theta } =\frac { 1 }{ 2 } I\omega ^2\\ \\ \int _{ 0 }^{ \frac { \pi }{ 2 } }{ Acos\theta d\theta } =\frac { 1 }{ 2 } I\omega ^2\\ \\ \frac{A\pi}{2}=\frac { 1 }{ 2 } I\omega ^2\\\\\omega=\sqrt { \frac{A\pi }{I} }##Answer in the back of the book:##omega=\sqrt { \frac{2A }{I} }##

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Check your evaluation of the integral.
 
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yup, I see it now. I appreciate it. I am not sure how I missed that.

Thanks again
 
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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