Circular Constant Acceleration Formula

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Homework Help Overview

The problem involves a uniform circular flywheel subjected to a constant tangential force, with the goal of determining its rotational speed after a specified number of revolutions. The subject area includes dynamics and rotational motion, specifically focusing on concepts such as torque, angular acceleration, and moment of inertia.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the application of work-energy principles and kinematic equations to solve for the final speed of the flywheel. There is an exploration of the relationship between tangential and angular acceleration, as well as the calculation of torque and moment of inertia.

Discussion Status

Some participants have provided guidance on calculating torque and moment of inertia, suggesting that the original poster's approach may have overlooked these critical components. There is an acknowledgment of the need to use the correct formula for the moment of inertia based on the flywheel's geometry.

Contextual Notes

Participants note the importance of considering the mass distribution of the flywheel, as it affects the moment of inertia and, consequently, the angular acceleration. There is also a mention of homework constraints that may limit the methods available for solving the problem.

CyclicCircle
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A constant tangential force of magnitude 12N is applied to the rim of a stationary, uniform circular flywheel of mass 100kg and radius 0.5m. Find the speed at which the flywheel is rotating after it has completed 25 revolutions?

I know that this can be done using work-energy. But since a constant tangential force is applied, I tried using kinematic equations.

Initial angular velocity \omega = 0, angular displacement \theta = 25 \times 2\pi = 50\pi.

If \alpha is the angular acceleration, mr\alpha = 12, (100)(0.5)\alpha = 12, \alpha = 0.24.

Final velocity \Omega^2 = \omega^2 + 2\alpha \theta, which gives \Omega = 8.68. But the correct answer is apparently 12.3.
 
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It is not clear what you are doing in the second last line.

First calculate the Torque ##\tau## applied by the force to the flywheel.
Then find the Moment of Inertia ##I## of the flywheel.
Then the angular acceleration is ##\alpha=\tau/I##. It is not 0.24.

If you do this and then substitute into the last line of your post, you should get 12.3.
 
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Thank you so much.

I used the fact that tangential acceleration = radius*(angular acceleration) and F = ma to obtain force = mass*radius*(tangential acceleration). What is the error in this?
 
CyclicCircle said:
Thank you so much.

I used the fact that tangential acceleration = radius*(angular acceleration) and F = ma to obtain force = mass*radius*(tangential acceleration). What is the error in this?
It is a disc, not a ring. You need to use the right formula for its moment of inertia.
 
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Thanks. I completely forgot about mass distribution!
 

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