What is the acceleration of the center of mass of the rolling hollow sphere?

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The discussion focuses on calculating the acceleration of the center of mass of a hollow spherical shell rolling down a slope at a 40-degree angle. The mass of the shell is given as 1.50 kg, and the problem involves applying Newton's second law and resolving forces. The key equations derived include the normal force and the gravitational force components acting on the shell. It is clarified that the radius of the shell is not necessary for determining linear acceleration, which can be expressed as a_cm = (3gsin(theta))/5. The final result provides a clear method for solving the problem without needing additional parameters.
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A hollow spherical shell with mass 1.50kg rolls without slipping down a slope that makes an angle of 40.0degree angle with the horizontal.
-Find the magnitude of the acceleration of the center of mass of the spherical shell

I am really confused on how to go about this problem. I know it has to do with inertia, but wow, i just don't know where to start.
 
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U used the term 'rolls without slipping'. I thought of using rotational mechanics to solve it but u are not given the radius of the spherical shell. Thus, i shall treat it like a case of linear motion down the slope. Resolving forces and applying Newton's 2nd law on the shell, we have Normal reaction force = mg cos 40 and mg sin 40 = ma. Thus a = g sin 40 = 9.8 sin 40. If u want to find angular acceleration of the shell, u need to have the shell's radius and use the relation, linear acceleration = spherical radius x angular acceleration.
 
No, you don't need the radius for this one. This is a hollow shell and it's moment of inertia is 2/3mr^2 = I
Fy = 0
Fx = mgsin(theta) - f = ma_cm

I get from Fx=mgsin(theta)-f=ma_cm (1)
and fR = 2/3mra_cm (2)

Solve f from (1).
Substitute that into (2) and then solve for a_cm

I get a_cm = (3gsin(theta))/5
 
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