Three Masses - pulley, rotational and translational forces

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SUMMARY

The discussion centers on a physics problem involving a green hoop (mass mh = 2.4 kg, radius Rh = 0.18 m), a blue solid disk pulley (mass md = 2.4 kg, radius Rd = 0.09 m), and an orange sphere (mass ms = 3.3 kg, radius Rs = 0.25 m) in a system released from rest. The linear acceleration of the hoop is determined by analyzing the forces and torques acting on the pulley and sphere. Key insights include the relationship between tension forces in the system and the necessity of using free body diagrams to visualize the forces acting on each component.

PREREQUISITES
  • Understanding of Newton's laws of motion
  • Knowledge of rotational dynamics and torque
  • Familiarity with free body diagrams
  • Concept of rolling without slipping
NEXT STEPS
  • Study the equations of motion for rotational systems
  • Learn about torque and its application in pulley systems
  • Explore the concept of rolling motion and friction in detail
  • Investigate the use of free body diagrams in complex mechanical systems
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Students of physics, mechanical engineers, and anyone interested in understanding the dynamics of pulley systems and rotational motion.

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An green hoop with mass mh = 2.4 kg and radius Rh = 0.18 m hangs from a string that goes over a blue solid disk pulley with mass md = 2.4 kg and radius Rd = 0.09 m. The other end of the string is attached to a massless axel through the center of an orange sphere on a flat horizontal surface that rolls without slipping and has mass ms = 3.3 kg and radius Rs = 0.25 m. The system is released from rest.

1)What is magnitude of the linear acceleration of the hoop?

I'm wondering how to solve this question, especially wondering how the tension forces would be related to each other throughout the system?
 

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From what is written, the hoop is not rotating - so it is just a mass falling: you can do the free body diagram for that one.

The pulley rotates, the net torque on the pulley will have it accelerate consistently with the acceleration of the falling mass. Label the tensions on each side of the pulley differently.

The sphere is rotating, the tension acts through the center, but there is a force from friction (rolling without slipping) where there is contact with the table. Just think of it as a wheel being pulled by the axle - you will have course notes for that situation.
 

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