Setting Boundaries for Statistical Mechanics
Bob Eisenberg

TL;DR
This paper argues that statistical mechanics for charged particles must include finite boundaries and boundary conditions, challenging the traditional unbounded models and emphasizing the importance of structures for accurate physical descriptions.
Contribution
It demonstrates that unbounded statistical mechanics is incomplete for charged systems and highlights the necessity of finite boundaries and boundary conditions for a proper theoretical foundation.
Findings
Unbounded models are insufficient for charged particles.
Finite boundaries are essential for defining electromagnetic fields.
Classical statistical mechanics needs to incorporate boundary conditions.
Abstract
Statistical mechanics has grown without bounds in space. Statistical mechanics of point particles in an unbounded perfect gas is commonly accepted as a foundation for understanding many systems, including liquids like the concentrated salt solutions of life and electrochemical technology, from batteries to nanodevices. Liquids, however, are not gases. Liquids are filled with interacting molecules and so the model of a perfect gas is imperfect. Here we show that statistical mechanics without bounds (in space) is impossible as well as imperfect, if the molecules interact as charged particles, as nearly all atoms do. The behavior of charged particles is not defined until boundary structures and values are defined because charges are governed by the Maxwell partial differential equations. Partial differential equations require boundary conditions to be computable or well defined. The…
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Taxonomy
TopicsStochastic processes and statistical mechanics · Scientific Research and Discoveries · Theoretical and Computational Physics
