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

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Homework Help Overview

The problem involves a solid sphere with a mass of 6 kg and a radius of 0.18 m, subjected to an applied force of 33 N while rolling on a horizontal surface under no-slip conditions. The setup includes a frictionless axle and a rope that causes the sphere to rotate without slipping, raising questions about the relationship between linear and rotational motion.

Discussion Character

  • Exploratory, Conceptual clarification, Problem interpretation

Approaches and Questions Raised

  • Participants discuss identifying forces acting on the sphere and applying Newton's second law to both rotational and translational dynamics. There are questions regarding how to find the acceleration of the sphere's center and how translational acceleration relates to rotational acceleration. Some participants express confusion about the formulas needed to connect applied force to both dynamics.

Discussion Status

The discussion is ongoing, with participants seeking clarification on the relationships between forces, acceleration, and the equations governing motion. Some guidance has been provided regarding the application of Newton's laws and the conditions for rolling without slipping, but no consensus has been reached on the specific formulas to use.

Contextual Notes

Participants note the absence of a coefficient of friction and express uncertainty about how to proceed with the calculations given the information provided. There is a focus on understanding the dynamics without explicit solutions being offered.

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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