Calculate number microstates? Why not include acceleration?

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To calculate the number of microstates in a system of indistinguishable particles in a 3D box, one typically uses the positions and velocities of the particles. While some discussions suggest including acceleration, it is generally unnecessary as the state of the system is defined by the canonical coordinates—positions and momenta. In classical Newtonian physics, higher derivatives like acceleration are determined by the equations of motion, but this approach changes in relativistic theory, where interactions cannot be described by simple differential equations. In relativistic contexts, the state of interacting particles requires more complex considerations beyond just positions and momenta. The discussion emphasizes keeping the analysis within the realm of classical mechanics for clarity.
llisuhrtgslir
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I want to calculate the number of microstates in a system for, say, n indistinguishable particles in a 3D box. Some examples I see just represent one microstate as a list of positions. Other examples use a list of positions and a list of velocities (translational and rotational). And if you're supposed to use position and velocity, why not acceleration too? I can maybe see why you wouldn't use "jerk" and fifth derivatives of position and so on.
 
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Because the state of such is system is completely described by the canonical coordinates of the particles. Specifying the position and momentum of all the particles uniquely locates it in phase space.
 
llisuhrtgslir said:
I want to calculate the number of microstates in a system for, say, n indistinguishable particles in a 3D box. Some examples I see just represent one microstate as a list of positions. Other examples use a list of positions and a list of velocities (translational and rotational). And if you're supposed to use position and velocity, why not acceleration too? I can maybe see why you wouldn't use "jerk" and fifth derivatives of position and so on.

Those examples work within Newtonian statistical physics, where the state of many-particle system is specified by stating coordinates and their first derivatives. Higher derivatives are then determined by the equations of motion.

This is not valid in relativistic theory, where the interaction of the particles is no longer describable by such ordinary differential equations.
 
The acceleration on each particle is calculated from the force on the particles, which you can determine from a snapshot of the system, whereas the velocity is just a free parameter.
 
Jano L. said:
This is not valid in relativistic theory, where the interaction of the particles is no longer describable by such ordinary differential equations.

States of individual particles of a system in classical relativistic stat mech are given (in flat space-time) by the phase space of 4-positions and 4-momenta with the latter constrained to lie on the mass hyperboloid so it isn't much different from the Newtonian case.
 
Only if the particles are non-interacting. State of a system of interacting particles in relativistic theory is not specified by their positions and momenta only, because forces acting on them cannot be functions of the positions and momenta only.
 
Let's wait for the OP to come back before going into the intricacies of relativity theory. As the question was posed, no relativity theory was needed, so let us keep it nice and elementary.
 
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