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

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Homework Help Overview

The discussion revolves around a physics problem involving two wedges and a cube balanced on them. The scenario assumes no friction between the cube and the wedges, while the wedges themselves have a static friction coefficient with the floor that is less than 1. Participants are exploring how to determine the maximum mass M that can be balanced on the wedges without slipping.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the forces acting on the cube and the wedges, including the normal force and friction. There is an exploration of resolving forces vertically and horizontally, with some questioning the application of trigonometric functions in their calculations.

Discussion Status

The discussion is active, with participants sharing their reasoning and calculations. Some guidance has been offered regarding the resolution of forces, and there is a collaborative effort to clarify the relationships between the forces involved.

Contextual Notes

Participants are working under the assumption of no friction between the cube and the wedges, which influences their calculations and reasoning about the normal force and equilibrium conditions.

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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?

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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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