Abstract

Since the 1970s, contact geometry has been recognized as an appropriate framework for the geometric formulation of thermodynamic systems, and in particular their state properties. More recently it has been shown how the symplectization of contact manifolds provides a new vantage point; enabling, among other things, to switch easily between the energy and entropy representations of a thermodynamic system. In the present paper, this is continued towards the global geometric definition of a degenerate Riemannian metric on the homogeneous Lagrangian submanifold describing the state properties, which is overarching the locally-defined metrics of Weinhold and Ruppeiner. Next, a geometric formulation is given of non-equilibrium thermodynamic processes, in terms of Hamiltonian dynamics defined by Hamiltonian functions that are homogeneous of degree one in the co-extensive variables and zero on the homogeneous Lagrangian submanifold. The correspondence between objects in contact geometry and their homogeneous counterparts in symplectic geometry, is extended to the definition of port-thermodynamic systems and the formulation of interconnection ports. The resulting geometric framework is illustrated on a number of simple examples, already indicating its potential for analysis and control.

Highlights

  • This paper is concerned with the geometric formulation of thermodynamic systems

  • Starting from Gibbs’ fundamental relation, contact geometry has been recognized since the 1970s as an appropriate framework for the geometric formulation of thermodynamics; see in particular [1,2,3,4,5,6,7,8]

  • Most of the work is on the geometric formulation of the equations of state, through the use of Legendre submanifolds [1,2,3,5,8], while less attention has been paid to the geometric definition and analysis of non-equilibrium dynamics

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Summary

Introduction

This paper is concerned with the geometric formulation of thermodynamic systems. While the geometric formulation of mechanical systems has given rise to an extensive theory, commonly called geometric mechanics, the geometric formulation of thermodynamics has remained more elusive and restricted. We show how the symplectization point of view unifies the energy and entropy representation, but is very helpful in describing the dynamics of thermodynamic processes, inspired by the notion of the contact control system developed in [11,12,13,17,18,19]; see [16] It yields a direct and global definition of a metric on the submanifold describing the state properties, encompassing the locally-defined metrics of Weinhold [26] and Ruppeiner [27], and providing a new angle to the equivalence results obtained in [3,5,7,10]. All this will be illustrated by a number of simple, but instructive, examples, primarily serving to elucidate the developed framework and its potential

Thermodynamic Phase Space and Geometric Formulation of the Equations of State
The Metric Determined by the Equations of State
Dynamics of Thermodynamic Processes
Port-Thermodynamic Systems
Examples of Port-Thermodynamic Systems
Controllability of Port-Thermodynamic Systems
Interconnections of Port-Thermodynamic Systems
Discussion
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