Particle Equilibrium: Solving for the Minimum Angle in a Roller System

AI Thread Summary
The discussion revolves around solving a particle equilibrium problem involving three identical smooth rollers in a groove. Participants analyze the forces acting on the system to determine the minimum angle α required to prevent collapse, with one contributor suggesting a method that balances half of the system. They derive equations based on the forces and moments acting on the rollers, ultimately arriving at a solution for α. A critical insight is the condition that the normal force N2 must equal zero, which simplifies the calculations. The final consensus indicates that the minimum angle α is approximately 10.89 degrees, demonstrating a solid understanding of the problem's geometric properties.
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Hi

(see attached picture for problem)

"Three identical smooth rollers are positioned in a groove as shown. Knowing that each roller (with radius 2.5 ft) weighs 500 lb, determine the minimum angle \alpha required to make the pile not collapse (all surfaces are assumed frictionless)."

I know this is a particle equilibrium problem. My idea is that since the system is symmetric, we should be able to balance half of the system inorder to get a solution (in fact, I believe we have too, otherwise the balances will yield 0=0). For example, taking the right half of the system, I believe the that the only forces we have to worry about are the N2 pointing left, the N1 pointing up, the two weights, and the N1 normal between the two balls should be ignored. These are the equations I've come up with (though I think the geometic relations are wrong and variable with the value of \alpha), with O being the low point where the two slopes intersect:

\sum {F_Y} & = & \frac{1}{2}w + w + N_1 \cdot sin(\alpha)=0
\sum {M_O} & = & 2.5 \cdot w \cdot cos(\alpha) + 2.5 \cdot N_1 + N_2 \cdot 2.5 (1 + sin(\alpha))=0
\sum {F_X} & = & N_2 - N_1 \cdot cos(\alpha)=0

(sorry, my latex is bad)

and of course, w=-500

Solving those equations, I fiind alpha = -112.8 (deg) (along with several imaginary answers)
Any help would be greatly appreciated!

Thanks
 

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I don't know if you agree with me, but I work this ploblem like this:
First, I work on the roller on top, so--> (N4+N5)sin(60)=mg and N4cos(60)=N5cos(60)---> N4=N5--->2(N5)sin(60)=mg--->N5=mg/(2sin(60))...(1).
Then, I start working with the roller on the right.
N5cos(60)+N2-N1sin(alpha)=0...(2) and N1cos(alpha)-mg-N5sin(60)=0...(3).
Substituting (1) on (3)----> N1cos(alpha)=mg+(1/2)mg=(3/2)mg...(1)*
In equation (2) in order to get a minimum (alpha), N2 must be zero----->
--->N1sin(alpha)=N5cos(60) and from (1)--->N1sin(alpha)=mg/(2tan(60)...(2)*
Finally, dividing (2)* by (1)*---> tan(alpha)=(1/3tan(60))-----> alpha~10.8933...
Due to certain geometrical properties, I used 60 degrees.

I hope this help and forgive me because I don't know how to use Latex wisky40
 
That makes perfect sense. The critical condition that I couldn't come up with was that N2=0. And your solution, being independent of mass or dimension, also makes sense. The work looks solid. Thanks a lot!
 
Kindly see the attached pdf. My attempt to solve it, is in it. I'm wondering if my solution is right. My idea is this: At any point of time, the ball may be assumed to be at an incline which is at an angle of θ(kindly see both the pics in the pdf file). The value of θ will continuously change and so will the value of friction. I'm not able to figure out, why my solution is wrong, if it is wrong .
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