What is the Maximum Mass M That Can Be Balanced on Two Wedges Without Slipping?

AI Thread Summary
The discussion focuses on determining the maximum mass M that can be balanced on two wedges without slipping, given that there is no friction between the block and the wedges. The participants analyze the forces acting on the system, particularly the normal force and frictional force, using equations related to inclined planes. They clarify that the normal force should be perpendicular to the block's surface, leading to the conclusion that the normal force equals Mg/(2cos(theta)). Ultimately, they derive an equation relating the static friction coefficient, mass, and angles involved, aiming to solve for the largest mass M that can be supported. The conversation emphasizes the importance of resolving forces correctly in this physics problem.
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Homework Statement



There are two wedges, each with mass m, placed on a flat floor. A cube of mass M is balanced on the wedges. Assume there is no friction between wedge and block, and the coefficient of static friction is less than 1 between the floor and wedges. What is the largest M that can be balanced without moving?

diagram here:
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Homework Equations


The Attempt at a Solution



If we split the block in half due to symmetry, the question will get easier.

force of friction is given by:
F=\mu (\frac{M}{2}+m)g
the M/2 comes from taking only half of the block

i want to equate the force that the block has on one of the wedge.

Still considering half of the diagram, i want the normal force of (M/2)g to the wedge's surface. The normal force is give by the usual inclined plane equation, mgcos(theta)

So normal force of (M/2) is:

N=\frac{Mg}{2}cos(\theta)

this normal force pushes in the opposite direction of the force of friction... but we have to consider the horizontal component, which tags on a sin(theta) term

I finally get:

\mu (\frac{M}{2}+m)g=\frac{Mg}{2}cos(\theta)sin(\theta)

And then i solve for mu. How close am I to being correct?
 
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learning_phys said:
Assume there is no friction between wedge and block,

Still considering half of the diagram, i want the normal force of (M/2)g to the wedge's surface. The normal force is give by the usual inclined plane equation, mgcos(theta)

So normal force of (M/2) is:

N=\frac{Mg}{2}cos(\theta)

Hi learning_phys! :smile:

No … consider the forces on the block

there is no friction, so the only forces are Mg/2 and N …

the horizontal components balance anyway …

so resolve vertically, and that gives you … ? :smile:
 
are you sayin N=Mg/2? but the normal force should be perpendicular to the blocks surface right? (that's why I have the cosine term)
 
learning_phys said:
but the normal force should be perpendicular to the blocks surface right?

Yes (because there is no friction). :smile:
are you sayin N=Mg/2?

No … resolve vertically.
 
learning_phys said:
ok, i get N=Mg/(2cos(theta))
??

That's it! :smile:
 
awesome

so I would get:
\mu (\frac{M}{2}+m)g=\frac{Mg}{2cos(\theta)}sin(\theta )
 
learning_phys said:
awesome

so I would get:
\mu (\frac{M}{2}+m)g=\frac{Mg}{2cos(\theta)}sin(\theta )

:biggrin: Woohoo! :biggrin:
(you're easily awed! … :wink:)

And so the largest M is … ? :smile:
 
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