Abstract

A thermodynamic approach to mechanical motion is presented, and it is shown that dissipation of energy is the key process through which mechanical motion becomes observable. By studying charged particles moving in conservative central force fields, it is shown that the process of radiation emission can be treated as a frictional process that withdraws mechanical energy from the moving particles and that dissipates the radiation energy in the environment. When the dissipation occurs inside natural (eye) or technical photon detectors, detection events are produced which form observational images of the underlying mechanical motion. As the individual events, in which radiation is emitted and detected, represent pieces of physical action that add onto the physical action associated with the mechanical motion itself, observation appears as a physical overhead that is burdened onto the mechanical motion. We show that such overheads are minimized by particles following Hamilton’s equations of motion. In this way, trajectories with minimum curvature are selected and dissipative processes connected with their observation are minimized. The minimum action principles which lie at the heart of Hamilton’s equations of motion thereby appear as principles of minimum energy dissipation and/or minimum information gain. Whereas these principles dominate the motion of single macroscopic particles, these principles become challenged in microscopic and intensely interacting multi-particle systems such as molecules moving inside macroscopic volumes of gas.

Highlights

  • The basis of analytical mechanics was laid in the 18th century by Joseph Louis Lagrange and by SirWilliam Rowan Hamilton

  • Building on the above considerations, we present a thermodynamic approach to mechanical motion which explicitly takes into account those dissipative effects that are connected with the radiation damping and the conversion of the emitted radiation into observations

  • Studying examples of macroscopic mechanical motion, we show that the principle of least action, which lies at the heart of Hamilton’s equations of motion [1,2], minimizes the physical action that is associated with the particle motion itself but that it minimizes those physical overheads that are connected with the radiation damping and the observation of the particle motion

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Summary

Introduction

As these vibrating electrons reach their upper and lower turning points, pulses of radiation are emitted which extract mechanical energy from the vibrating electrons and which carry this energy from the sites of emission to a detector which is placed at some distance Once arrived there, this energy is dissipated and converted into low-temperature heat while intermittently producing macroscopically observable events which represent observational images of the electron motion inside the antenna rod. In the course of our discussion, we develop the idea that the mechanical motion of charged particles is burdened with an observational overhead that can be measured in terms of physical action generated and energy dissipated during the processes of radiation emission and radiation detection. Very small but finite, dissipative overheads are burdened onto the mechanical motion

Thermodynamic Approach to Classical Mechanical Motion
Mechanical Motion in the Quantum Domain
Least Action and Observational
Least Action Principles and Observational Overhead
Q vx 1
Dissipative Overhead and Irreversibility
Molecule–ion
Summary and Conclusions
Full Text
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