Acceleration of a Block Sliding Down a Wedge

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SUMMARY

The discussion focuses on the dynamics of a block sliding down a wedge, specifically analyzing the forces acting on both the block and the wedge. The equations of motion are established, including the force balance for the wedge (FBD of '1') and the block (FBD of '2'). Key concepts include the tension in the string and the effects of kinetic friction, represented by the equation f = μMgcos(θ). The participants emphasize the importance of understanding the relative motion between the block and the wedge to simplify the problem.

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Bling Fizikst
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Consider the wedge as '1' and block as '2' : i need to find ##a_{2/F}=a_{2/1}+a_{1/F}## .
The FBD of '1' : $$Mg\sin\theta - f=Ma_{1/F}$$ $$Mg\cos\theta=N$$
The FBD of '2' : $$mg - T =ma_{2/1}$$
Assuming kinetic friction : ##f=\mu Mg\cos\theta##. But how do i find ##T##?
 
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You are overlooking some forces. The string exerts a force on the pulley, while the wedge and block exert contact forces on each other.
You also have the constraint that the block does not penetrate the wedge.

But, unless I am missing something, the question is much simpler than it looks. Think about how the block moves relative to the wedge.
 
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Is this correct? Seems fairly complicated . How do i handle all these tension forces , moreover since it's an ideal pully , the net force acting on it would be zero .
 
Bling Fizikst said:
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Is this correct? Seems fairly complicated . How do i handle all these tension forces , moreover since it's an ideal pully , the net force acting on it would be zero .
The net force on the pulley is zero, but the string exerts a force on it, so that force is transferred to the wedge.
As I wrote, think first about the relative motions of the two bodies.
 

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