Pulley problem with moment of inetia

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SUMMARY

The discussion centers on calculating the acceleration of Block A with mass 'M' on a surface with kinetic friction 'Uk', connected via a cord over a pulley to Block B with mass '2M'. The pulley is modeled as a thin disk with a moment of inertia given by I=0.5*M*r² and mass 'M/4'. The moment of inertia plays a critical role in the system's dynamics, as it introduces resistance to angular acceleration, affecting the overall acceleration of Block A when Block B is released.

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  • Understanding of Newton's laws of motion
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  • Knowledge of free body diagrams
  • Basic principles of rotational dynamics
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Iansno1
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Problem

As shown below, Block A has mass 'M' and rests on a surface with a coefficient of kinetic friction 'Uk' .The cord attached to A passes over a pulley at C and is attached to a block B of mass '2M'. If B is released calculate the acceleration of A.

Assume the cord does not slip over the pulley. The Pulley can be approximated as a thin disk of radius 'r' and mass 'M/4' . Neglect the mass of the cord
Relevant equations

moment of inertia of the disk: I=0.5*M*r2
Not sure where to start
 

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with free body diagrams?

ehild
 
How does the Moment of inertia come into the equation? I can do these problems when the pulley is assumed to have no mass and no friction.
 
Iansno1 said:
How does the Moment of inertia come into the equation? I can do these problems when the pulley is assumed to have no mass and no friction.

Moment of inertia is the analog of mass for rotational motion. The moment of inertia resists angular acceleration in the same fashion as mass resists linear acceleration.

In this problem the pulley adds resistance to the acceleration of the overall system because the cord does not slip, and so must cause angular acceleration of the pulley. The angular acceleration is related to the linear acceleration (how?).
 

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