Finding largest angle - mechanics

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The discussion focuses on determining the largest angle θ for which two connected bars AB and BC remain at rest between rough vertical walls, given a static friction coefficient of 0.4. The initial calculations incorrectly assumed equal friction forces on both bars, leading to an angle of 64 degrees, while the correct approach indicates that the friction forces can vary and must not exceed the maximum static friction. The equilibrium conditions require separate torque equations for each bar, considering their ability to rotate around the pin at B. By correctly applying these principles, the equations reveal that the angle θ can be determined by balancing the forces and torques, ultimately leading to the correct solution. The final angle, as per the book, is 10 degrees, highlighting the importance of accurately accounting for friction in static equilibrium problems.
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Homework Statement


The two homogeneous bars AB and BC are connected with a pin at B and placed between rough vertical walls. If the coefficient of static friction between each bar and the wall is 0.4, determine the largest angle θ for which the assembly will remain at rest.

http://screensnapr.com/e/vU9M3X.jpg


Homework Equations



summation of forces among horizontal
summation of forces among vertical
summation of forces - point

The Attempt at a Solution



so i use the fbd of the whole body, and take summation of forces on x axis, and i got Na = Nc (normal at point a is equal to point c). then, i take summation of forces on y axis, so thats

Fa - 6N -8N +Fb = 0 (where fa and fb are friction forces on a and b), and since fa = fb (their normals are equal), i use f = uN and yielded Na = 17.5 N.

I then take summation of moments at point B( bar of A to B) and here's eqn

(6)(300)(cos(x)) - 17.5 (600)(cos(x)) + 7(600)(sin(x)) = 0 and

the value of angle is 64 degress. the book says 10 degress. Where did I go wrong?
 
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The bars are not fixed together, but connected with a pin, they can turn around. Write out the conditions for equilibrium for both.
The force of friction is static, so you can not say that fa=fb. It is only true that neither of them can exceed 0.4 times the normal force. ehild
 
I would not like to waste this problem...

blackandyello said:
Fa - 6N -8N +Fb = 0 (where fa and fb are friction forces on a and b), and since fa = fb (their normals are equal), i use f = uN and yielded Na = 17.5 N.

The equation is correct for the resultant of all vertical components, but the forces of static friction are not the same: Fa is not equal to Fb. The force of static friction can not exceed the maximum value, so Fa, Fb ≤μN and the greater one is equal to it.

The bars can turn around B with respect to each other, so the torques must be balanced separately for both. If L is the length of the rods, the sum of torques on the left rod is

NLsinθ+6L/2 cosθ-Fa Lcosθ=0 => Ntan(θ)=Fa-3, Fa=Ntan(θ)+3

The equation for the right rod is

NLsinθ+8L/2 cosθ-Fb Lcosθ=0 => Ntan(θ)=Fb-4, Fb=Ntan(θ)+4

That means Fa<Fb≤0.4N. Taking Fb equal to 0.4N, Ntan(θ)+4=0.4N,

N(0.4-tan(θ))=4

The equation for vertical force components yields Fa+Fb=14. Plugging in Fa and Fb:

Ntan(θ)+3+Ntan(θ)+4=14 =>2N tan(θ)=7

Solve the equations in bold for θ.

ehild
 

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