Question

A wheel of radius R, mass M, and moment of inertia I is mounted on a frictionless, horizontal axles. A light cord wrapped around the wheel supports an object of mass m. When the wheel is released, the object accelerates downwards, the cord unwraps off the wheel, and the wheel rotates with an angular acceleration. The cord is not slipping.

Answer 1

`\alpha =(m*g*R)/(I-m*R^2)`

`a = (m*g*R^2)/(I-m*R^2)`

`T=(I*m*g)/(I-m*R^2)`

Step-by-step explanation:

By analyzing the torque on the wheel we get:

`T*R=I*\alpha` Solving for T:
`T=I/R*\alpha`

On the object:

`T-m*g = -m*a` Replacing our previous value for T:

`I/R*\alpha-m*g = -m*a`

The relation between angular and linear acceleration is:

`a=\alpha*R`

So,

`I/R*\alpha-m*g = -m*\alpha*R`

Solving for α:

`\alpha =(R*m*g)/(I+m*R^2)`

The linear acceleration will be:

`a =(R^2*m*g)/(I+m*R^2)`

And finally, the tension will be:

`T =(I*m*g)/(I+m*R^2)`

These are the values of all the variables: α, a, T