haruspex said:
The question is only concerned with the instantaneous circumstance, so there is as yet no velocity at B.
The will be accelerations. If the angular acceleration is α, what will be the linear acceleration of the mass centre?
What equations can you write relating forces to accelerations and torques to angular accelerations?
-Since there is no angular velocity the normal acceleration will be equal to 0.
-Likewise, the tangential acceleration will be equal to the product of r and α. However, I am unsure of the direction it will move in.
-Also since that is the total net force, ma = mrα = summation of all forces.
-Also, the torque will equal Iα + mad (the perpendicular d).
So I'm assuming I solve for I, which I think would be equal to (1/12)mL^2 = (1/12)(5.4 kg)(1.180 m)^2 = 0.531 kg*m^2. And that would act at the bar's center.
For the net force, I'm assuming I use this to solve for alpha (in terms of r). Also, I assume the tangental acceleration will be completely to the left, in which case:
mrα = P --> α = P/m/r = (75)/(5.4)/r = 13.889/r.
However, I'm not sure what else I can do from here. Was my assumption about the direction of the acceleration wrong? Was my inertia calculation wrong?