Overhead crane and pulleys problem

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    Crane Pulleys
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Discussion Overview

The discussion revolves around a problem involving an overhead crane system with multiple pulleys and winches, focusing on the discrepancies in load measurements during lifting and lowering operations. Participants explore the dynamics of forces in the system, particularly the effects of cable deformation and friction in the pulleys.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant notes a discrepancy in load measurements, observing that the load cell reads 30 tons during lifting, 36.2 tons during lowering, and 32.5 tons when the load is stationary.
  • Another participant suggests that the deformation of the steel cable at pulleys 3 and 4 may affect the force balance between the cable segments.
  • Some participants agree that the force at the pulley is 2 times F1, rather than 4 times, as initially indicated.
  • There is a proposal that the outgoing rope experiences higher force due to friction in the pulleys, which requires additional torque to overcome.
  • One participant expresses a desire for a mathematical description of the observed phenomena, indicating that they understand the concept intuitively but seek formal evidence.
  • A suggestion is made to simplify the problem to analyze the forces in the rope under constant speed and when stopping the lift.
  • Another participant elaborates that at constant speed, the forces at each pulley must balance, and introduces the idea of friction torque affecting the force distribution.

Areas of Agreement / Disagreement

Participants generally agree on the presence of friction affecting the forces in the system, but there are competing views regarding the exact dynamics and mathematical modeling of the situation. The discussion remains unresolved as participants seek further clarification and mathematical backing.

Contextual Notes

Limitations include the potential impact of cable deformation and friction not being fully quantified, as well as the need for clearer definitions of forces and torques involved in the system.

Marinel
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The problem bellow is a real problem and I would like to get some ideas in order to overcome it.

As you can see in the attached doc, we have two winches ( drum 1 and 2 ) on the same shaft of motor M1, two moving pulleys ( 3 and 4 ) and a fixed pulley (5).
The load is 130 Tons, and we can measure that with a load cell at pulley 5 ( 32,5 Tons) after the lifting of the load.
But during the time as the load is rising we measure only 30 tons! Note that we have a cable of steel with 30mm diam. and the rising speed is about 1m/min.

When we lower the load, the load cell measures 36,2 Tons. and as soon it stops we get again 32m5 Tons.

When the load gets the floor than we read 0 Tons (of course!)

Can someone explain this? This is a real case and my problem is to adjust the safety relay to 110% of nominal load, which is impossible with this beahviour of the system!
 

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Marinel said:
The load is 130 Tons, and we can measure that with a load cell at pulley 5 ( 32,5 Tons) after the lifting of the load.
Intuitively I would think that Ft = 2 x F1 here (not 4 x F1 as denoted in your PDF)

Marinel said:
But during the time as the load is rising we measure only 30 tons! Note that we have a cable of steel with 30mm diam. and the rising speed is about 1m/min.

When we lower the load, the load cell measures 36,2 Tons. and as soon it stops we get again 32m5 Tons.
Could it be that the deformation of the steel cable at pulley 3 & 4 changes the force balance between the two cable segments going from/to the pulley? It seems that the side to which the cable goes is taking more load.
 
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You are right! The force at pulley is 2XF1 and not 4X.

In fact I have a display showing the real load and that's whya mmy mistake.

I thought that the problem is concerned with the deformation of the rope but I cannot explain how it works. The length of each rope ( distance from 3 to 5 ) is about 10 meters.

Could someone explain it??
 
Marinel said:
Could someone explain it??

Isn't it a general phenomenon of lossy pulley dynamics, that the outgoing rope has a higher force, because it includes the force needed to overcome friction? The bearings at the axis of pulley 3 & 4 have some friction. To overcome that friction you need some torque. So the outgoing rope must have a greater force than the incoming rope, to create that torque.
 
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OK, I can understand what you say, but that is just a feeling. Can you or someone describe it mathematically?
The feeling I have already but that's all!I would like to have the evidence of the phenomenon.
 
May be we can simplify the problem using the arrangement below.
What will be the force in the rope when it goes up with no acceleration? And what happens if we stop the lifting?
 

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Marinel said:
May be we can simplify the problem using the arrangement below.
What will be the force in the rope when it goes up with no acceleration? And what happens if we stop the lifting?
For your simplified arrangement:
https://www.physicsforums.com/attachment.php?attachmentid=37850&d=1312849616

At constant speed the force in the right rope will be always the weight of the green mass (Ft). Due to friction in the upper pulley the force in the left rope will be more than Ft when lifting the weight, and less than Ft when lowering it. So the force at the pulley axis F1, which is the sum of the rope forces will vary accordingly.

Marinel said:
Can you or someone describe it mathematically?
At constant speed all the forces acting at each pulley must balance each other and all the torques acting at each pulley must balance each other. If you introduce a friction torque into the equation, the force vectors must still sum to zero, but to balance the friction torque they have to be redistributed.
 

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