Balancing Forces | Min Force to Hold Rod at Point A

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SUMMARY

The minimum force required to hold the rod at point A is determined to be 0.5 mg cosθ, where m is the mass of the rod, g is the acceleration due to gravity, and θ is the angle of inclination. The solution involves analyzing the torque about point B, where the torque τ is expressed as (L/2)(mg cos θ). By balancing the forces and torques, it is established that the force Fa at point A must counteract the torque generated by the normal force from the hinge, resulting in the derived expression for Fa.

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Homework Statement


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What is the minimum force required to hold the rod at point A?

Homework Equations




The Attempt at a Solution


If no one is holding the rod, point B would get the force mg from the rod. So the normal force from the hinge to the rod is mg, pointing up. This normal force would create a torque τ, which will cause the rod to rotate.

τ = (L/2)(mg cos θ)

The force that holds the rod in place counters this torque by having the component

Fτ = mg cos θ

that is perpendicular to the rod, in the clockwise direction. However, now the three forces acting on the rod--gravity, the normal force from the hinge, and the force from the hand--no longer sum up to zero. What is wrong?

- Thanks
 
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Forget about B. Just use torques, and take for granted that B is the pivot point. Note: there is a range of forces in different direction that will hold the rod at A. You need to find the minimum.
 
Ok, suppose there is a force Fa at A, and we some the torque about B:

(L/2)(mg cosθ) - LFa = 0

So the tangential component of Fa must be 0.5 mg cosθ. Suppose I let Fa to have no radial component and let the hinge do the rest, then:

Fbx = - Fasinθ

Fby = mg - Facosθ

Since the torque was summed at B, the force at B won't change the net torque. This shows that the x and y direction forces are also balanced. So Fa must be 0.5 mg cosθ, and it is tangent to the rod in clockwise direction.
 
Last edited:

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