Maximum Horizontal Force for Two Blocks to Accelerate Without Slipping?

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SUMMARY

The maximum horizontal force that can be applied to the lower block (M_2) without causing the upper block (M_1) to slip is determined by the equation F_{max} = \mu g (M_1 + M_2). This relationship arises from the requirement that the frictional force, which is f = \mu M_1 g, must be sufficient to accelerate M_1 at the same rate as M_2. The acceleration of both blocks is given by a = F/(M_1 + M_2), and for M_1 to remain stationary relative to M_2, the frictional force must equal the product of M_1 and the acceleration.

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Homework Statement



A block of mass [tex]M_1[/tex] rests on a block of mass [tex]M_2[/tex] which lies on a frictionless table. The coefficient of friction between the blocks is [tex]\mu[/tex]. What is the maximum horizontal force which can be applied to the lower ([tex]M_2[/tex]) block for the blocks to accelerate without slipping on one another?

Homework Equations




The Attempt at a Solution


The acceleration of the two blocks (assuming they're not slipping) is [tex]a = \frac{F}{M_1 + M_2}[/tex], and you want the upper block ([tex]M_1[/tex]) to not slip, that is, the acceleration times [tex]M_1[/tex] must be less than or equal to the frictional force. When the blocks start slipping, [tex]M_1 a = \mu M_1 g[/tex] where the frictional force holding the upper block is [tex]f = \mu M_1 g[/tex]. This means that [tex]a = \frac{F_{max}}{M_1 + M_2} = \mu g[/tex], or [tex]F_{max} = \mu g (M_1 + M_2)[/tex].

I'm not sure if this answer is right, but it makes intuitive sense when looking at the final equation. Thanks for any help!

[edit] Sorry, posted in wrong section. I can't find a delete button, but any help would still be appreciated
 
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Looks correct.
 

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