Torque to rotate pulley with equal mass on each side.

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Discussion Overview

The discussion centers on the mechanics of a pulley system with equal weights on either side, specifically examining the torque required to rotate the pulley and the effects of friction. Participants explore the theoretical and practical implications of friction, inertia, and the conditions under which the rope may slip from the pulley.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant suggests that in a frictionless scenario, no torque would be needed to rotate the pulley, but acknowledges that real-world friction complicates this situation.
  • Another participant emphasizes that the outcome regarding whether the rope slips depends on the friction values, indicating that without specific numbers, no definitive answer can be given.
  • A third participant adds that speed and acceleration are also relevant factors in the system's dynamics.
  • Further elaboration indicates that torque is required to overcome various resistances, including shaft and bearing friction, rope and pulley friction, and the inertia of the weights, pulley, and rope.
  • It is noted that increasing weight raises friction, which could reduce the likelihood of slipping, but also increases the torque required to initiate motion.
  • Participants discuss that inertia affects the system only during acceleration, and if the torque is sufficient, it can overcome shaft friction to initiate rotation.
  • There is a mention of static and kinetic friction forces, highlighting that if the torque exceeds the maximum static friction, slipping will occur, necessitating the use of kinetic friction in calculations.

Areas of Agreement / Disagreement

Participants express differing views on the role of friction and the conditions under which the rope may slip. There is no consensus on a definitive answer regarding the torque required or the behavior of the system under varying conditions.

Contextual Notes

The discussion relies heavily on assumptions regarding friction values and does not provide specific numerical examples, leaving the analysis somewhat open-ended. The interplay between static and kinetic friction is also noted but not resolved.

mrkevelev
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Lets say there is a pulley attached to the ceiling. Hanging on the pulley is a rope and on each end is a 1000 lb. weight. I believe that theoretically it wouldn't take any torque at all to rotate the pulley if it were frictionless (maybe inertia would play a role, but let's ignore that). However, in reality there will be a downward force on the pulley's shaft, causing friction. Let's say that a motor is connected to the pulley. I want to know if I turn the pulley, will the rope slip? My thoughts are that increasing weight will give better friction between the pulley and rope, and therefore, as long as the weights are equal, the torque required to rotate the pulley will be quite low, even though shaft friction increases as well with weight.
 
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Everything in your question is related to friction. One kind of friction compared to another kind of friction.

There can be no answer without putting numbers on the friction values. You can make the answer come out either way, it slips or doen't slip, depending on the friction values.
 
In your system, there is a torque required for each of these resistances:
  • The friction between the shaft and bearing;
  • The friction between the rope and pulley;
  • The inertia of the weights, pulley and rope.
The first one will be there all the time, as soon as the pulley rotates. If you increase the weight, the friction increases and with it, the torque required.

The second one is present only if there is slipping between the rope and the pulley. If you increase the weight, the friction increases and this reduces the chance of slipping.

The third one is present only if there is an acceleration. This means inertia has no effect at constant speed. Of course, if you increase the weight, you increase inertia. In this case if you don't increase the extra torque (i.e. above the friction torque already discussed), it will only reduce the acceleration. So it is not a requirement for the system to work, unless you have a minimum acceleration to achieve.

That being said, if the torque input is high enough, it will break the shaft friction and the pulley will begin to rotate. If the pulley is accelerating, then some part of the torque is lost there too. If the resultant output torque creates a friction force that exceeds the maximum static friction force between the pulley and the rope, then slipping begins and you have to use the kinetic friction force instead, no matter how high the input torque is. This friction force (whether it is static or kinetic friction) will be the force that accelerates the rope and the weights.
 

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