Statistical behaviour of ideal particles in a closed box

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Discussion Overview

The discussion centers around the statistical behavior of ideal particles in a closed box, focusing on their velocities and interactions. Participants explore theoretical aspects of particle dynamics, statistical mechanics, and the implications of idealized conditions on the behavior of the system.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • Harald proposes a model of N ideal particles in an enclosure, questioning how to estimate the average squared difference in velocities between pairs of particles.
  • Harald notes that the velocities are constant in magnitude but random in direction, and he seeks clarification on the implications of the enclosure on his calculations.
  • Some participants suggest that the scenario resembles a micro-canonical ensemble from statistical mechanics, with implications for entropy.
  • dgOnPhys provides a mathematical simplification for estimating the average squared difference in velocities, suggesting it may yield a result proportional to the square of the constant speed.
  • Harald acknowledges a potential solution that approximates the average squared difference but notes that it may not fully satisfy the condition of zero net velocity.
  • A later reply presents a detailed mathematical derivation for the average squared difference in velocities, arriving at a result that appears to confirm the earlier estimates.

Areas of Agreement / Disagreement

Participants express varying degrees of agreement on the mathematical approaches and interpretations of the model, but no consensus is reached regarding the implications of the enclosure or the accuracy of the approximations used.

Contextual Notes

There are limitations regarding the assumptions made about the randomness of velocity directions and the implications of the enclosure on the statistical behavior of the particles. The discussion does not resolve these complexities.

birulami
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Suppose I have N ideal particles in an enclosure, be it a ball or a cube or some other form. The particles shall bounce off the walls of the enclosure and against each other without losing speed. The velocity of each particle i shall be such that it fullfills |v_i|=\rho, where \rho is constant, i.e. the speed is always the same, but of course the direction in 3D differs.

Further, on the average, the whole ensemble of points shall not move, i.e.

(*) \sum_{i=1}^N v_i = 0

or at least the sum is very close to zero.

Apart from this, the velocities' directions shall be completely random. What exactly this would mean may need to be further defined.

My questions are:
1) How can I estimate \frac{1}{N^2}\sum_{i<j} (v_i-v_j)^2?
2) Is the "boxed" condition used in the derivation or does (*) contain all we need?

Maybe this is not really a physics question, because the setup is too idealised, but I assume that is still closer to physics than to pure math.

Harald.
 
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Naty1 said:
You might find this interesting:

http://en.wikipedia.org/wiki/Particles_in_a_box

An interesting link that I will certainly take a closer look at. But on first glance it seems to relate to quantum physics, which is certainly not what I am after here.

Harald.
 
Hi birulamy,

it looks very much like a micro-canonical ensemble so I would expect you will get the basic results of statistical mechanics.

1) can be simplified by
- extending sum over all i,j and dividing by two
- expanding the square of the binomial
the results I think is rho^2 (or whatever letter you use for the particles' constant speed)
2) not sure what you mean

Let me know if you need details
 
Hi dgOnPhys,

thanks for the hint about the micro-canonical ensemble. In particular the connection to entropy is interesting for me.

It seems like I got a solution myself which is most likely the same as you state. By setting d_{ij}=v_i-v_j and assuming that the sum can be approximated by taking (N^2-N)/2 times the expected value of the d_{ij}, I got the result (1-1/N)\rho^2. The discrepancy is most likely that this estimation does not enforce the condition (*), but only converges to it for large N.

Harald.
 
Hi Harald,

without approximations:
\frac{1}{N^2}\sum_{i<j} (v_i-v_j)^2=
=\frac{1}{2N^2}\sum_{i,j} (v_i-v_j)^2=
=\frac{1}{2N^2}\sum_{i,j} (v_i^2+v_j^2-2 v_i . v_j)=
=\frac{1}{2N^2}\sum_{i,j} (2 \rho^2-2 v_i . v_j)=
=\frac{1}{2N^2}(2 N^2 \rho^2 - 2 \sum_{i,j} (v_i . v_j))=
=\frac{1}{N^2}( N^2 \rho^2 - \sum_{i} (v_i . \sum_{j}v_j))=\rho^2
 

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