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

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Homework Help Overview

The problem involves a rigid rod of mass M and length L rotating in a vertical plane about a pivot at its center of mass, with masses m1 and m2 attached at its ends. The goal is to determine the angular acceleration of the system when the rod is at an angle θ with the horizontal.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the calculation of torque and the forces acting on the system, questioning how to account for the gravitational forces on both masses. There is exploration of the relationship between torque, inertia, and angular acceleration.

Discussion Status

Participants have engaged in a detailed examination of the forces and torques involved, with some guidance provided on defining torque and considering the direction of forces. There is an ongoing exploration of how to combine the effects of the two masses on the system's angular acceleration.

Contextual Notes

There is a focus on ensuring all forces are accounted for in the torque calculation, and participants are clarifying the definitions and relationships between torque, inertia, and angular acceleration. The discussion reflects uncertainty about the correct approach to combining the effects of the two attached masses.

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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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