Interesting differential equation

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The discussion revolves around a differential equation comparing the average speed of multiple points to their individual speeds, expressed through a specific mathematical formulation. The original equation is scrutinized for accuracy, with a correction noted regarding a constant factor in the second formula. A transformation of the equation suggests a relationship involving the velocities of the points and their interactions. The conversation also hints at exploring solutions through the framework of Lie groups, particularly focusing on the special orthogonal group in three dimensions. The participants are seeking effective methods to solve for x(t) without resorting to potentially complicated integrations.
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Comparing the average speed of a bunch of points with the individual points' speeds, I came across the following equation:

\left(\frac{dx(t)}{dt}\right)^2 <br /> = \frac{1}{N^2} c^2 \sum_{i\neq j} \left(1-\frac{v_i(t) v_j(t)}{c^2}\right)

where the v_i are the velocity vectors (3 dimensions) of the N points. They fulfil the equation |v_i(t)|^2 = c^2. If I didn't loose some constant factor, the equation above should be the same as

\left(\frac{dx(t)}{dt}\right)^2 <br /> = \frac{1}{N^2} \sum_{i&lt; j} (v_i - v_j)^2

Any chance to solve one or the other for x(t)? I hesitate to take the square root and try to integrate the square root of the sum. Are there better ways to solve this?

Harald.
 
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There is a mistake in the second formula which should be ##\left( \frac{dx(t)}{dt}\right)^2 = \frac{1-c^2}{N^2} \sum_{i< j} (v_i - v_j)^2##. It can be rewritten as
$$
\dfrac{N^2}{1-c^2}\, \ddot{x}(t)^2 = \left|\left|\begin{pmatrix}v_1\\v_2\\v_3\end{pmatrix}\times \begin{pmatrix}1\\1\\1\end{pmatrix}\right|\right|^2 =\left|\left|\begin{pmatrix}0&-1&1\\1&0&-1\\-1&1&0\end{pmatrix}.\mathbf{v}\right|\right|^2
$$
So the entire equation looks a bit like ##\gamma \,||\dot{\mathbf{v}}||^2 = ||\mathbf{A.v}||^2## or ##\mathbf{\dot v} = \dfrac{\sqrt{1-c^2}}{N}\mathbf{A.v}## with an exponential function as solution.

This leads to another idea, namely to consider ##x(t)## as path in a Lie group, presumably ##\operatorname{SO}(3)##.
 
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