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Phase Transformation Contributions to Heat Capacity and Impact on Thermal Diffusivity, Thermal Conductivity, and Thermoelectric Performance
Author(s) -
Agne Matthias T.,
Voorhees Peter W.,
Snyder G. Jeffrey
Publication year - 2019
Publication title -
advanced materials
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 10.707
H-Index - 527
eISSN - 1521-4095
pISSN - 0935-9648
DOI - 10.1002/adma.201902980
Subject(s) - heat capacity , thermal diffusivity , thermal conductivity , materials science , thermodynamics , thermoelectric materials , volumetric heat capacity , phase transition , thermoelectric effect , phase (matter) , thermal effusivity , thermal , heat transfer , condensed matter physics , thermal resistance , heat flux , composite material , thermal contact conductance , physics , quantum mechanics
The accurate characterization of thermal conductivity κ, particularly at high temperature, is of paramount importance to many materials, thermoelectrics in particular. The ease and access of thermal diffusivity D measurements allows for the calculation of κ when the volumetric heat capacity, ρc p , of the material is known. However, in the relation κ = ρc p D , there is some confusion as to what value of c p should be used in materials undergoing phase transformations. Herein, it is demonstrated that the Dulong–Petit estimate of c p at high temperature is not appropriate for materials having phase transformations with kinetic timescales relevant to thermal transport. In these materials, there is an additional capacity to store heat in the material through the enthalpy of transformation Δ H . This can be described using a generalized model for the total heat capacity for a materialρ c p = C p ϕ + Δ H ( ∂ ϕ / ∂ T ) pwhere φ is an order parameter that describes how much latent heat responds “instantly” to temperature changes. Here, C pφ is the intrinsic heat capacity (e.g., approximately the Dulong–Petit heat capacity at high temperature). It is shown experimentally in Zn 4 Sb 3 that the decrease in D through the phase transition at 250 K is fully accounted for by the increase in c p , while κ changes smoothly through the phase transition. Consequently, reports of κ dropping near phase transitions in widely studied materials such as PbTe and SnSe have likely overlooked the effects of excess heat capacity and overestimated the thermoelectric efficiency, zT .