Angular acceleration of solid sphere on frictionless yoke unde no slip roll condition

AI Thread Summary
The discussion centers on calculating the angular acceleration of a solid sphere rolling without slipping under the influence of a 33N force. The sphere has a mass of 6kg and a radius of 0.18m, with a frictionless axle allowing for rotation. Participants emphasize the need to apply Newton's second law for both translational and rotational motion to find the correct acceleration of the center of mass. The relationship between linear and angular acceleration is crucial, and the condition for rolling without slipping must be applied. Clarification is sought on how to correctly correlate the applied force to both translational and rotational dynamics.
jvani
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Homework Statement



m=6kg
r=0.18m
Fapp=33N


I'm struggling to understand how to answer this question and correlate the linear force applied to rotation without being given the coefficient of friction causing the rotational motion.

The question states that a solid sphere of 6kg is free to roll on a horizontal surface under no slip conditions. A frictionless axle is run through the middle of the sphere, with a rope thread through it, the rope applies 33N on the sphere, and the sphere starts to rotate without slipping

Any help would be appreciated
 
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Start by identifying the forces acting on the sphere. Then apply Newton's 2nd law to both rotation and translation.
 


The only forces I can see in the horizontal direction is the force applied of 33N and the force of friction. I'm struggling see how to find the acceleration of the center of the sphere from what was given, and then how the translational acceleration of the sphere correlates to the rotational acceleration explicitly.
 


jvani said:
The only forces I can see in the horizontal direction is the force applied of 33N and the force of friction.
Right.
I'm struggling see how to find the acceleration of the center of the sphere from what was given,
Apply Newton's 2nd law, as I suggested.
and then how the translational acceleration of the sphere correlates to the rotational acceleration explicitly.
To relate translational and rotational motion, apply the condition for rolling without slipping.
 


I have the same question, with different numbers. I do not understand which formula I am to use that relates the force applied to both the translational and rotational dynamics. I realize that the tangential acceleration and centre of mass acceleration are the same.

If I say that Fext=ma and then divide by the mass to get the acceleration, and then use the relationship between linear and angular acceleration it does not work.

How do I find the correct acceleration of the centre of mass?
 


canadiankid said:
If I say that Fext=ma and then divide by the mass to get the acceleration, and then use the relationship between linear and angular acceleration it does not work.
Make sure you use ƩF = ma. To solve for the acceleration, you'll need to combine two equations: one for translation and one for rotation.
 
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