Describing the motion of a linked body?

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Discussion Overview

The discussion revolves around the motion of linked bodies, particularly focusing on how to describe the angular acceleration of individual rigid bodies and the entire system when a force is applied. The context includes theoretical approaches, numerical solutions, and the implications of chaos in such systems.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose using the Lagrangian approach to describe the motion of linked bodies, suggesting it may simplify the analysis even for complex systems like a double pendulum.
  • Others argue that while the Lagrangian method can be effective, it often leads to numerical solutions rather than closed-form expressions, especially in more complex cases.
  • A participant questions the ability to achieve numerical solutions to any degree of accuracy, noting that chaos can complicate predictions and solutions.
  • Some participants discuss the conditions under which closed-form solutions may exist, particularly in simpler systems with fewer degrees of freedom, such as two masses connected by a joint.
  • There is interest in the nature of chaotic systems and the challenges in proving whether a system is chaotic or lacks symbolic solutions, with some noting that non-chaotic systems can also lack symbolic solutions.
  • A participant expresses curiosity about the potential for future solutions to well-known problems, such as the three-body problem involving the Sun, Moon, and Earth.
  • Another participant seeks guidance on applying the Lagrangian approach to a modified double pendulum scenario where the support pivot is removed.

Areas of Agreement / Disagreement

Participants express a mix of agreement and disagreement regarding the effectiveness of the Lagrangian approach and the nature of chaos in linked body systems. There is no consensus on whether closed-form solutions can generally be achieved, and the discussion remains unresolved on several points related to chaos and symbolic solutions.

Contextual Notes

Participants note that the complexity of linked body systems often leads to chaotic behavior, complicating the search for closed-form solutions. The discussion highlights the dependence on initial conditions and the specific configurations of the systems being analyzed.

Who May Find This Useful

This discussion may be of interest to those studying dynamics, chaos theory, or the application of Lagrangian mechanics in complex systems.

greswd
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A general example of a linked body is an object that is made up of rigid bodies joined together by pivots, such as hinges and ball-socket joints.

If the pivots are frictionless, and I apply a force to one rigid body, how can I go about describing the subsequent angular acceleration of the individual rigid bodies, and also the entire linked body about its barycenter?
 
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I would use the Lagrangian approach. Even for something as simple as a double pendulum it winds up being easier.
 
Which, with exception of a few simple cases, will usually produce something that can only be solved numerically. So if you hope for a closed-form expression, forget about it. But if you need it for a simulation, do what DaleSpam suggested. Write down the Lagrangian with an undetermined Lagrange Multiplier for every joint or other constraint you have. That will give you a system of equations for each [itex]\ddot{q_i}[/tex] to be solved for each time step, and then you can use Verlet or Runge-Kutta methods to integrate these.[/itex]
 
K^2 said:
Which, with exception of a few simple cases, will usually produce something that can only be solved numerically. So if you hope for a closed-form expression, forget about it. But if you need it for a simulation, do what DaleSpam suggested. Write down the Lagrangian with an undetermined Lagrange Multiplier for every joint or other constraint you have. That will give you a system of equations for each [itex]\ddot{q_i}[/tex] to be solved for each time step, and then you can use Verlet or Runge-Kutta methods to integrate these.[/itex]
[itex] <br /> So it's possible to get a numerical solution to any degree of accuracy? I've always wondered how mathematicians definitively prove that the system is inherently chaotic and that no closed form solutions exist.<br /> <br /> But even if a pattern exists it's difficult to find because the subsequent motion is so highly dependent on initial conditions.[/itex]
 
what about a very simple compound body?

Just one mass, floating in deep space, with a rod pivoted to it.
 
greswd said:
So it's possible to get a numerical solution to any degree of accuracy?
Not in general. There are going to be special cases where you can, but in general, these things tend towards chaos.

If you have just two masses connected by a single joint, you can use conservation of momentum and angular momentum to greatly reduce degrees of freedom, giving you a closed form solution. Everything past that would require some approximations, I believe.
 
K^2 said:
Not in general. There are going to be special cases where you can, but in general, these things tend towards chaos.

If you have just two masses connected by a single joint, you can use conservation of momentum and angular momentum to greatly reduce degrees of freedom, giving you a closed form solution. Everything past that would require some approximations, I believe.

Thanks. So in certain cases things are non-chaotic, but it's generally difficult to prove whether system is definitely chaotic and/or lacks a closed form solution.
 
Hmmm, I am interested in finding out how mathematicians prove that a system is chaotic and that no symbolic solutions exist.
 
  • #10
For instance, the three body problem of Sun-Moon-Earth might have a definite closed form solution that we just cannot find.
 
  • #11
greswd said:
Hmmm, I am interested in finding out how mathematicians prove that a system is chaotic and that no symbolic solutions exist.
These are two somewhat different properties. A system can be non-chaotic and still not have a symbolic solution.

However, I don't think that "no symbolic solutions" is something that is actually mathematically proven. It is simply that we don't know any such solutions. It also depends critically on what functions are admissible in your set of symbolic colutions.
 
  • #12
DaleSpam said:
A system can be non-chaotic and still not have a symbolic solution.
What kind of system is described as such?

DaleSpam said:
However, I don't think that "no symbolic solutions" is something that is actually mathematically proven. It is simply that we don't know any such solutions. It also depends critically on what functions are admissible in your set of symbolic colutions.
Interesting, it sort of opens the possibility that someday someone might solve the Sun-Earth-Moon problem.

Like the CMI problems.
 
  • #13
Hey DaleSpam,

Do you mind giving me a little direction on how to set up the problem described here using the Lagrangian approach? I just recently learned about and applied the Lagrangian approach to describe the motion of a double pendulum (in this case the set up is given by many sources online). What I want to do now is describe the motion of the double pendulum if the support pivot disappears and the connected rigid bodies are now flying through the air.

Thanks,
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