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Two Different Masses on an Uncentered Fulcrum (Torque) 
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#1
Oct3110, 07:15 PM

P: 3

1. The problem statement, all variables and given/known data
Two blocks each of mass 1.9 kg are suspended from the ends of a rigid weightless rod of length l1 = 1.43 m and l2 = .085 m. The rod is held in the horizontal position shown and then released. Calculate the initial acceleration of the mass attached to l1. Assume up is positive and down is negative. Also to clarify, the problem is asking for tangential acceleration 2. Relevant equations T = r x F T = Ia A = ar I = mr^{2} 3. The attempt at a solution First I summed the torque of the two sides T = L_{1}mg + L_{2}mg = Ia where mg is the force acting on the mass on each side and L_{1} and L_{2} are the radii. For the moment of Inertia I, I used the point mass formula (I = mr^{2}) But that would apply for the system, so I added the two moment of Inertia for the two sides I = mr_{1}^{2} + mr_{2}^{2} Doing some algebra to move the variables around I came up with g(L_{1}+L_{2})  = a (L_{1}^{2} + L_{2}^{2}) Putting in my numbers yielded me 9.8*(1.43+.085)/(1.43^{2}+.085^{2}) = a = 7.23 rad/s^{2} Then after that I would need to divide 7.23 by the radius, r, to get the tangential acceleration. But I'm not sure which r I would use. r = L1? or r = (L1+L2)/2? Anyway, that's what I came up with. I'm guessing there are a lot of mistakes in here, but I'm not sure what I did right and what I did wrong. Any help pointing me in the correct direction would be great! :) 


#2
Oct3110, 09:26 PM

P: 3

If there's any other information you need from me, let me know so we can work to help me figure this out.



#3
Oct3110, 10:40 PM

P: 3

Nevermind, I found out the answer. It seems I was pretty close. I needed to make my equation
g(L1+L2) *L1  = A (or alpha *r) (L1^2 + L2^2) The thing that was throwing me off was multiplying it by L1 instead of dividing it by L1. But I understand now. My original equation solved alpha. Then by multiplying both sides by L1 you get what I have above on the left is equal to alpha * r (which = tangential acceleration) 


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