Solving the Movement of a Cart with a Man on Top

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Discussion Overview

The discussion revolves around a physics problem involving the movement of a cart with a man on top, focusing on the dynamics of the system as the man moves relative to the cart. Participants explore concepts related to angular momentum, forces, and the implications of a massless platform and frictionless wheels. The scope includes theoretical reasoning and conceptual clarification.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants question the interesting nature of the problem, suggesting it may confuse students due to its intertwined insights.
  • There is a discussion about the implications of having a massless platform and the absence of friction, with some finding it artificial.
  • Participants propose using angular momentum to analyze the problem, while others challenge this approach, questioning the axis of rotation.
  • One participant highlights the reaction forces and torques involved when the man moves, suggesting a conflict between the man's acceleration and the cart's movement.
  • Concerns are raised about the conservation of momentum in the context of massless wheels and the potential misconceptions it may create for students.
  • Some participants express that the concepts required to solve the problem are not advanced, while others argue for a more rigorous derivation of the formulas involved.
  • There is a suggestion to include additional factors, such as viscous friction, to make the problem more relevant to standard classes.

Areas of Agreement / Disagreement

Participants express differing views on the problem's educational value and the appropriateness of the assumptions made (massless platform, no friction). There is no consensus on the best approach to analyze the problem, with multiple competing views on the use of angular momentum and the implications of the system's dynamics.

Contextual Notes

Participants note that the problem may not be suitable for all educational contexts, particularly for students who may not grasp the underlying principles easily. The discussion reveals a tension between informal reasoning and the need for rigorous mathematical derivation in dynamics.

wrobel
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Is this an interesting problem what do you think?
9ef91c7ad043.png

A cart consists of a massless platform and two wheels. Each wheel is a disk of mass M.
The cart stands on a horizontal road and a man of mass m stands upon the platform. Then the man started to go along the cart and after passing the distance L (relatively the cart) he stopped also relatively the cart. The wheels do not slip over the road and there is no friction in the axes.
Which distance the cart passed?
(warning: do not think that the center of mass keeps its position :)
 
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Hello Wrobel,
Well, depends on what you consider 'interesting'. I don't know the context of your question, though. To me it seems the insights needed to see through this exercise are somewhat unnecessarily intertwined. Good students pick up the angular momentum part instantly and not so good students will be left in greater confusion than before they got the exercise presented to them, I fear.
I also find it a bit artificial to have a massless platform on massive wheels - and no friction.
 
wrobel said:
Is this an interesting problem what do you think?
9ef91c7ad043.png

A cart consists of a massless platform and two wheels. Each wheel is a disk of mass M.
The cart stands on a horizontal road and a man of mass m stands upon the platform. Then the man started to go along the cart and after passing the distance L (relatively the cart) he stopped also relatively the cart. The wheels do not slip over the road and there is no friction in the axes.
Which distance the cart passed?
(warning: do not think that the center of mass keeps its position :)
Yes, I like it. ##\frac{Lm}{3M+m}## right?
 
BvU said:
Hello Wrobel,
Well, depends on what you consider 'interesting'. I don't know the context of your question, though. To me it seems the insights needed to see through this exercise are somewhat unnecessarily intertwined. Good students pick up the angular momentum part instantly and not so good students will be left in greater confusion than before they got the exercise presented to them, I fear.
I also find it a bit artificial to have a massless platform on massive wheels - and no friction.
Angular momentum? That does not seem to me to be the way to approach it. About what axis?
 
About the axes where there is no friction ! Like in wheels that rotate.
 
BvU said:
About the axes where there is no friction ! Like in wheels that rotate.
Pick one axle. What forces have moments about that axle? What is the man's angular momentum about it? Would you like to know how tall the man is?
 
Am I misreading this ? Man wants to accelerate by stepping to the right, platform wants to move to the left. Road stays where it is so reaction force from road is torque on wheel.
 
BvU said:
Am I misreading this ? Man wants to accelerate by stepping to the right, platform wants to move to the left. Road stays where it is so reaction force from road is torque on wheel.
Yes, but now you are working with accelerations and torques, as I did. Not any momentum conservation.
 
I see. I only brought it up because with massless wheels total momentum conservation leaves center of mass in place and poster warned against that misconception for massive wheels.
So in a PF context this (apparently) is interesting; in a teaching environment I would not recommend it.
 
  • #10
BvU said:
I see. I only brought it up because with massless wheels total momentum conservation leaves center of mass in place and poster warned against that misconception for massive wheels.
So in a PF context this (apparently) is interesting; in a teaching environment I would not recommend it.
It bothers me that there are certain standard questions that are churned out at a given level, like conservation of momentum for a boat on a lake, which can leave the student with the impression that that approach always works. Even if the student is not expected to solve this more advanced problem, it is a useful lesson. Anyway, it depends on the level.
 
  • #11
BvU said:
Well, depends on what you consider 'interesting'. I don't know the context of your question,
usually I propose this problem in the beginning of the Lagrangian mechanics studies. But what about undergraduate courses of physics?
BvU said:
I also find it a bit artificial to have a massless platform
You can impose weight of the platform but this will not bring any new idea in the solution
BvU said:
and no friction.
for example we can add an angular momentum of linear viscous friction in the axes. Then the question like that " where does the cart tend as ##t\to \infty##?" will not for standard classes I guess
haruspex said:
t. Lm3M+m\frac{Lm}{3M+m} right?
Yessss!
 
  • #12
None of the concepts required are very advanced. Just basic F=ma and τ=Iω, together with the understanding that if two objects have a fixed ratio of accelerations then the same ratio applies to their velocity changes and displacements. UK GCE A level maths, perhaps?
 
  • #13
haruspex said:
None of the concepts required are very advanced. Just basic F=ma and τ=Iω, together with the understanding that if two objects have a fixed ratio of accelerations then the same ratio applies to their velocity changes and displacement
yes, sure but this sounds as a little bit informal argument
 
  • #14
wrobel said:
yes, sure but this sounds as a little bit informal argument
Do you mean regarding displacement ratio? ##\ddot x_2=\lambda\ddot x_1##, ##\dot x_2=\lambda\dot x_1## (both initial velocity zero), ##\Delta x_2=\lambda \Delta x_1##.
 
  • #15
I mean that all the formulas must be derived (on mathematical level of rigor) from the fundamental equations of dynamics. And it seems to me that in our case such a derivation is not so trivial task for students. Some people regard such a demand as tediousness and excess.
 

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