Angular acceleration of a rigid rod with a mass at both ends

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A rigid rod with masses m1 and m2 at its ends rotates about a pivot, and the discussion focuses on calculating its angular acceleration when the rod is at an angle θ. The inertia of the system is determined to be (M/12 + (m1 + m2)/4)L². The torque is calculated using the forces acting on both masses, with the gravitational force on m1 needing to be considered alongside m2. The total torque is derived from the opposing forces, leading to the formula α = [((m2g - m1g)Lsin(90 - θ))/2] / [(M/12 + (m1 + m2)/4)L²]. The inertia calculation is confirmed to be correct, with a note on the trigonometric identity sin(90° - x) = cos(x).
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1. A rigid rod of mass M and length L rotates in a vertical plane about a frictionless pivot through its center of mass. Particles of masses m1 and m2 are attached at the ends of the rod. Determine the angular acceleration of the system when the rod makes an angle θ with the horizontal.
In the accompanying picture, m2 is obviously larger and the rod is rotating clockwise.


2. τ=Iα=Frsinθ

3. The inertia I calculated for the system is (M/12 + (m1 + m2)/4)L2. I think that the angle between position vector r and the force F would be 90 - θ. So then the angular acceleration α would be m2g(L/2)sin(90 - θ) / I? I'm confused about whether or not the force of gravity on m1 also needs to be taken into account and if so, how.
 
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Yes, you need to take into account all of the forces acting on the system when you compute the torque. First order of business: How do you define the torque?
 
It's the product of the rotational inertia and the angular acceleration. I know the angular acceleration is at/r, so would I need to subtract (m1g)/(L/2) from (m2g)/(L/2) to get this?
 
Not in terms of the inertia and the acceleration, in terms of the forces acting on the object.
 
Like τ = (r)(Fsinθ)?
 
Yes. So the forces on each of the masses are going to provide a torque around the pivot. What is then the total torque?
 
τ = (L/2)(m2gsin(90-θ) + (L/2)(m1gsin(90-θ) ?
 
I guess I'm not sure if they need to be added or subtracted.
 
Do the forces tend to accelerate the rod in the same or in opposite directions?
 
  • #10
Opposite, so they'd be subtracted?
 
  • #11
Correct. You have to define a direction for the torque, if the force acts to accelerate the object in that direction, the torque is positive. If it tries to spin it in the other, the torque is negative.
 
  • #12
So, α = [((m2g-m1g)Lsin(90 - θ))/2] / [(M/12 + (m1 + m2)/4)L2]? Was my calculation of the inertia correct?
 
  • #13
Yes, the inertia seems correct. Just also note that sin(90o - x) = cos(x).
 
  • #14
Right - thank you!
 
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