Reversible Reciprocal Relation of Thermoelectricity

TL;DR

This paper redefines thermoelectric coefficients based on reversible thermodynamics, deriving a reversible reciprocal relation that clarifies the Kelvin relation's validity beyond linear regimes and links it to fundamental thermodynamic principles.

Contribution

It introduces a reversible thermodynamic framework for thermoelectricity, deriving a reciprocal relation from Maxwell relations that extends the Kelvin relation beyond linear transport assumptions.

Findings

Reversible Seebeck and Peltier coefficients are defined without time derivatives.

The Kelvin relation is derived from reversible thermodynamics and Maxwell relations.

The framework applies to other coupled thermodynamic phenomena.

Abstract

The first Kelvin relation that states the Peltier coefficient should be equal to the product of temperature and Seebeck coefficient is a fundamental principle in thermoelectricity. It has been regarded as an important application and direct experimental verification of Onsager reciprocal relation (ORR) that is a cornerstone of irreversible thermodynamics. However, some critical questions still remain: why Kelvin's proof that omits all irreversibility within a thermoelectric transport process can reach the correct result, how to properly select the generalized-force-flux pairs for deriving the first Kelvin relation from ORR, and whether the first Kelvin relation is restricted by the requirement of linear transport regime. The present work is to answer these questions based on the fundamental thermodynamic principles. Since the thermoelectric effects are reversible, we can redefine the Seebeck and Peltier coefficients using the quantities in reversible processes with no time derivative involved, which are renamed as "reversible Seebeck and Peltier coefficients". The relation between them (called "the reversible reciprocal relation of thermoelectricity") is derived from the Maxwell relations, which can be reduced to the conventional Kelvin relation, when the local equilibrium assumption (LEA) is adopted. In this sense, the validity of the first Kelvin relation is guaranteed by the reversible thermodynamic principles and LEA, without the requirement of linear transport process. Additionally, the generalized force-flux pairs to obtain the first Kelvin relation from ORR can be proper both mathematically and thermodynamically, only when they correspond to the conjugate-variable pairs of which Maxwell relations can yield the reversible reciprocal relation. The present theoretical framework can be further extended to other coupled phenomena.