What Is the Maximum Mass M3 Can Have Without the Block Sliding Off the Slab?

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Homework Help Overview

The problem involves a block of mass M1 resting on a slab of mass M2, both initially at rest. A hanging mass M3 is connected to the slab via a string over a pulley. The goal is to determine the maximum mass M3 can have without the block sliding off the slab, considering the coefficients of friction between the block, slab, and table.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss treating the block and slab as separate entities to analyze the forces acting on each. There is a focus on drawing free body diagrams and relating the forces to find the maximum mass of M3 without slipping. Some participants express confusion about how to connect the forces and accelerations of the block and slab.

Discussion Status

Participants are actively exploring the relationships between the forces acting on the block and slab. Guidance has been offered regarding the treatment of the block and slab as separate systems, and some have calculated the maximum static friction force. There is an ongoing discussion about how to relate the forces and find an appropriate acceleration.

Contextual Notes

Participants are working under the constraints of static and kinetic friction coefficients and are considering the implications of these on the maximum mass of M3. There is an emphasis on not exceeding the static friction force to prevent slipping.

Singdasorrow
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Homework Statement


A block of mass M1 = .430 kg is initially at rest on a slab of mass M2 = .845 kg, and the slab is initially at rest on a level table. A string of negligible mass is connected to the slab, runs over a frictionless pulley on the edge of the table, and is attached to a hanging mass M3. The block rests on the slab but is not tied to the string, so friction provides the only horizontal force on the block. The slab has a coefficient of kinetic friction .365 and a coefficient of static friction .566 with both the table and the block. When released, M3 pulls on the string and accelerates the slab, which accelerates the block. Find the max mass of M3 that allows the block to accelerate with the slab, w/o sliding on the top of the slab


Homework Equations


Ʃfx= T-f
Ʃfy = T - W
f=uN

The Attempt at a Solution


I treated the masses on the table as one single mass which was 1.275 kg. i multiplied that by gravity to find N and it was 12.495. I took the kinetic coefficient of friction and found friction to be -4.56

i plugged this into the Ʃfx= T-f equation with my other knowns to find T+4.56= 1.275a
Looking at the second equation i see that i have two variables for the weight will depend on the mass of the hanging mass. so Ʃfy = T - (mass3 x gravity)

i'm stuck at this point relating the two together. Am i correct in how i have things set up so far? or have i not solved for a variable that i should b able to?
 
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You need to treat the block separately from the slab, or you'll never find the max that M3 can be without the block slipping on the slab.

Draw TWO Free Body Diagrams; one for the block, one for the slab.
 
Ok, so since I'm going to treat them individually. I have 3 force diagrams (1 for each object) and have the sum of the forces acting on each one.

I am tho confused how to relate them because i do know i can't exceed fs. so i need to find an acceleration that will allow me to do that, then a mass as a result. am i thinking of this right?
 
Static friction: fs ≤ μ2 FNormal
 
ok so since i know the coefficient of static friction and the normal force of the block. Fs ≤ .566 x .430(-9.8). Fs ≤ -2.385 N
 
Singdasorrow said:
ok so since i know the coefficient of static friction and the normal force of the block. Fs ≤ .566 x .430(-9.8). Fs ≤ -2.385 N
So, that's the maximum force that the slab can exert on the block.

I think you may be able to finish the problem now.
 

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