Calculating Resultant Force at a Pivoted Rod | Uniform Rod in Vertical Plane

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SUMMARY

The discussion focuses on calculating the resultant force at the pivot of a uniform rod, 1.6 m in length and 20 kg in mass, released from a horizontal position. The moment of inertia is determined using the formula 1/3*m*L^2, resulting in an angular acceleration of 9.1875 rad/s². The participant initially calculates the tangential force as 147 N but realizes the correct resultant force at the pivot is 49 N, leading to a total force of 196 N when combined with the tangential force. The confusion arises regarding the normal force, which is assumed to be zero during the calculation.

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Homework Statement



A uniform rod of length 1.6 m and mass 20 kg is free to rotate about a frictionless pivot at one end in a vertical plane. The rod is released from rest in the horizontal position. The acceleration of gravity is 9.80 m/s2.


Homework Equations



What is the resultant force in the pivot immediately after the release?

The Attempt at a Solution



I know that the Moment of Inertia around such a rod is 1/3*m*L^2 and that the tourqe around that rod is L/2*mg, this gives me the angular acceleration 9.1875. I assume that the normal force in this situation is zero?

That would only give me the tangental force F_t = m*r_cm*a left (since F_n = m*r*w^2, but w = 0), which gives me the answer 147 N, but the answer should be 49 N
 
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hi fkf! :smile:
fkf said:
That would only give me the tangental force F_t = m*r_cm*a left (since F_n = m*r*w^2, but w = 0), which gives me the answer 147 N, but the answer should be 49 N

hint: 49 + 147 = 196 :wink:
 
fkf said:
I assume that the normal force in this situation is zero?
What are you calling the normal force here? What is the linear acceleration of the rod's centre?
 

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