Torque: Understanding the Complexity Behind the Physics

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SUMMARY

This discussion centers on the concept of torque, particularly in static equilibrium scenarios involving rigid bars. Participants clarify the relationship between force, distance from the axis of rotation, and torque, emphasizing that a weight of 100 kg at a distance 'r' generates a torque of 980r (using 9.8 m/s² for gravitational acceleration). To maintain equilibrium, an opposing torque must be applied, which is calculated using the formula τ_net = τ_cw + τ_ccw. The conversation highlights the importance of understanding the distribution of forces and the role of the center of gravity in static systems.

PREREQUISITES
  • Understanding of basic physics concepts, including force and torque.
  • Familiarity with static equilibrium and the conditions for equilibrium in rigid bodies.
  • Knowledge of gravitational acceleration (9.8 m/s²) and its application in torque calculations.
  • Ability to differentiate between mass, weight, and force in physical contexts.
NEXT STEPS
  • Study the principles of static equilibrium in rigid body mechanics.
  • Learn about torque calculations and their applications in real-world scenarios.
  • Explore the concept of center of gravity and its impact on force distribution.
  • Investigate the differences between linear and rotational dynamics in physics.
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Physics students, educators, and engineers interested in understanding the complexities of torque and static equilibrium in mechanical systems.

Felix83
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I have a few years of physics experience, and as I was thinking about a few things the other day, something about the concept of torque seemed a little weird to me.

Simple Forces are easy to understand - gravity pulls down on an object, the ground pushes back up with an equal and opposite force, etc, etc. Now torque - If you think about it from the perspective of work it makes sense - If you apply a force at the end of a long arm to rotate it, the force is greater closer to the axis of rotation because it moves a shorter distance, but performs the same amount of work.

However, consider a rigid bar in static equilibrium, with a fixed axis of rotation at one end. There is a weight in the middle, say 100 kg. You push up farther away from the axis so you only have to push with a 50kg force to keep it from falling. At that instant, there is no motion, so you cannot say your hand travels a greater distance than the weight so the force needed is less.

With no motion, how does the system "know" (for lack of a better word) to take your 50kg force at the end, and apply 100kg of upward force where the weight is?
 
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Felix83 said:
Simple Forces are easy to understand - gravity pulls down on an object, the ground pushes back up with an equal and opposite force, etc, etc. Now torque - If you think about it from the perspective of work it makes sense - If you apply a force at the end of a long arm to rotate it, the force is greater closer to the axis of rotation because it moves a shorter distance, but performs the same amount of work.

This sounds fallacious but I think I know what you mean. To apply a torque of equal magnitude at a closer distance requires a larger force.

Felix83 said:
However, consider a rigid bar in static equilibrium, with a fixed axis of rotation at one end. There is a weight in the middle, say 100 kg. You push up farther away from the axis so you only have to push with a 50kg force to keep it from falling. At that instant, there is no motion, so you cannot say your hand travels a greater distance than the weight so the force needed is less.
I'm assuming the bar is horizontal. Firstly, you are mistaking weights, masses and forces. A weight is a force due to gravity, and a mass is just a mass for the purposes of this argument. Having a 100kg weight at a distance 'r' from the AoR will yield a torque of 100kg*9.8m/s^2*r. To counter this torque, you would need to apply a torque of equal magnitude in the opposite direction. Let's say your arm can apply a force of 100N

\tau_{net} = 0 = \tau_{cw} + \tau_{ccw} \ and \ so \ \tau_{cw} = -\tau_{ccw}

Say the weight provides the clockwise torque, then

\tau_{cw} = mgr = 980r_1

\tau_{ccw} \mbox{ will need to be of the same magnitude,} 100r_2

980r_1 = 100r_2 \ and so \ r_2 = 9.8r_1. Only with radiuses described by this relationship will the system be in equilibrium.
felix83 said:
With no motion, how does the system "know" (for lack of a better word) to take your 50kg force at the end, and apply 100kg of upward force where the weight is?

The system doesn't 'know' per sai, it will simply follow through any actions that forces acting on it dictate. If your arm wasnt pushing, the entire system would begin rotating. You deliberately position your arm at a certain radius so that the system is not rotating.

I hope this is along the liens of what you were looking for.
 
Think about it a different way, using center of gravity. Take a rigid beam and support it on each end. Put a weight at the center - it is distributed evenly between the two supports. Put it 2/3 of the way to one side and one support takes double the force of the other. How does the support "know" how much force with which to push up?

For some reason, people have no problem with that scenario, but they do with a lever. But from a standpoint of statics (the way you analyze the system), this situation and the lever situation you describe are exactly the same (just flipped over).
 

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