Uniquely Defined Accelerations

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Discussion Overview

The discussion revolves around the interpretation of a statement from Landau's book regarding the determination of accelerations in a physical system when positions and velocities are known. Participants explore the implications of this assertion in the context of classical mechanics, questioning the completeness of the information provided by positions and velocities alone.

Discussion Character

  • Exploratory
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions how knowing positions and velocities at a moment can uniquely determine accelerations, suggesting that additional information, such as forces, is necessary.
  • Another participant interprets Landau's statement as implying that classical forces depend on the first derivative of position, thus suggesting that accelerations can be inferred from positions and velocities.
  • Some participants express a shared understanding of the complexities in Landau's conclusions, indicating that they may require deeper analysis than initially presented.
  • A later reply emphasizes the importance of understanding how these concepts emerge from the principle of extremizing the action in classical mechanics.

Areas of Agreement / Disagreement

Participants generally express differing views on the completeness of the information provided by positions and velocities in determining accelerations, indicating that multiple competing interpretations remain unresolved.

Contextual Notes

There is an acknowledgment that the discussion may hinge on the definitions of terms like "forces" and "accelerations," as well as the assumptions underlying classical mechanics. The nuances in Landau's writing are noted as potentially leading to varied interpretations.

LukasMont
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From Landau's book, here's the following extract:

"If all the co-ordinates and velocities are simultaneously specified, it is known from experience that the state of the system is completely determined and that its subsequent motion can, in principle, be calculated. Mathematically this means that, if all the co-ordinates q and q˙ are given at some instant, the accelerations q¨ at that instant are uniquely defined".

I don't understand how that can be the case. Knowing the positions and velocities in a given moment allow me to calculate the new positions at a dt time afterwards, if accelerations are all zero. If not, I'll need to know the accelerations from some other source, like knowing the forces acting on the system, etc. I don't see how merely having positions and accelerations in a given moment gives you the accelerations in that moment as well.
 
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I think in this case Landau has a little more in the back of his mind. I would interpret "from experience" to mean something like all the classical forces we know depend on at most the first derivative of position. In that sense, any acceleration at a particular time is determined by the position or velocity at that time.
 
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Haborix said:
I think in this case Landau has a little more in the back of his mind. I would interpret "from experience" to mean something like all the classical forces we know depend on at most the first derivative of position. In that sense, any acceleration at a particular time is determined by the position or velocity at that time.
@Haborix, that was my interpretation as well...but I thought it would be better to bring the topic into discussion, since sometimes in Landau's books he makes this fast, "simple" conclusions which are actually deeper than his tone may convey. Thanks for your input!
 
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LukasMont said:
@Haborix, that was my interpretation as well...but I thought it would be better to bring the topic into discussion, since sometimes in Landau's books he makes this fast, "simple" conclusions which are actually deeper than his tone may convey. Thanks for your input!
That's definitely a good instinct to have when you go through Landau, but I think in this instant he's just getting the reader primed to see how these facts fall out naturally from extremizing the action.
 

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