Chain with distance-dependent mass problem

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SUMMARY

The discussion revolves around the dynamics of a particle of mass m attached to a long chain with linear density μ, particularly focusing on the maximum height the particle can reach when thrown upwards with an initial velocity V. The application of Newton's Second Law, F = dp/dt, is central to solving the problem, with the mass considered as m + μx during upward motion and m during downward motion due to the normal force N from the ground. The participant seeks clarification on the differences in force dynamics between the upward and downward motions, specifically regarding the role of the normal force.

PREREQUISITES
  • Understanding of Newton's Second Law (F = dp/dt)
  • Familiarity with linear density concepts (μ in kg/m)
  • Basic knowledge of forces acting on objects (normal force, gravitational force)
  • Ability to visualize and sketch physical phenomena
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  • Study the implications of normal force in dynamic systems
  • Learn about the motion of connected systems in classical mechanics
  • Explore advanced topics in particle dynamics and chain mechanics
  • Review examples of similar problems involving variable mass systems
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Physics students, educators, and anyone interested in classical mechanics, particularly those studying dynamics involving variable mass systems and force interactions.

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1. A particle of mass m is tied on one end of a very long chain which has a linear density μ (kg/m) and lies on a surface with the chain wound next to it. The particle is thrown upwards with an initial velocity V. Find the maximum height the particle is going to reach. My question is not what the exercise asks, it has more of a philosophical essence to it. You can read it in part 3.



2. Relevant equations:
We just take Newton's Second Law, F = dp/dt, so we have
-(m+μx)g = d[(m+μx)υ]/dt
and we solve the problem.



3. Studying the particle's motion, my teacher said that while the particle is going upwards (υ>0), we consider m+μx as its mass. BUT when it is going downwards, that is when it starts falling, (υ<0) we consider m as its mass. I find this reasonable by instict (I mean when I visualize the phenomenon in my head) because the chain is supported by the surface/ground when the particle falls. Even my teacher told me that it is because of a normal force N applied to the chain by the ground thus neutralizing the weight of the chain. But my question is isn't the normal force N applied to the chain by the surface in the upwards motion, too? I don't see the differences in the forces that can convince me to say the downwards motion is different than the upwards one. I'd like someone to draw all the forces appearing in this problem in a sketch, so I can understand the phenomenon.

Thanks in advance.

EDIT:
Here's a sketch. The circle is the particle and the line which ends up in a spiral is the chain.
nV6aB.png
 
Last edited:
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Anyone?

Please, I just need a sketch of the forces applied to the particle and the chain. :'(
 

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