Classical Statistics
In classical mechanics all the particles (fundamental and composite particles, atoms, molecules, electrons, etc.) in the system are considered distinguishable. This means that one can label and track each individual particle in a system. As a consequence changing the position of any two particles in the system leads to a completely different configuration of the entire system. Furthermore there is no restriction on placing more than one particle in any given state accessible to the system. Classical statistics is called Maxwell–Boltzmann statistics (or M–B statistics).
Read more about this topic: Particle Statistics
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