Abstract

Although the Harman method evaluates the thermoelectric figure-of-merit in a rapid and simple fashion, the accuracy of this method is affected by several electrical and thermal extrinsic factors that have not been thoroughly investigated. Here, we study the relevant extrinsic effects and a correction scheme for them. A finite element model simulates the electrical potential and temperature fields of a sample, and enables the detailed analysis of electrical and thermal transport. The model predicts that the measurement strongly depends on the materials, sample geometries, and contact resistance of the electrodes. To verify the model, we measure the thermoelectric properties of Bi2-Te3 based alloys with systematically varied sample geometries and either with a point or a surface current source. By comparing the model and experimental data, we understand how the measurement conditions determine the extrinsic effects, and, furthermore, able to extract the intrinsic thermoelectric properties. A correction scheme is proposed to eliminate the associated extrinsic effects for an accurate evaluation. This work will help the Harman method be more consistent and accurate and contribute to the development of thermoelectric materials.

Highlights

  • Accurate evaluation of thermoelectric figure-of-merit, ZT =α2T/ρk, is of great importance to the development of thermoelectric materials, where α is the Seebeck coefficient, ρ is the electrical resistivity, k is the thermal conductivity, and T is the absolute temperature[1,2,3,4,5,6]

  • We investigate the electrical and thermal extrinsic effects associated with the Harman method, and seek to obtain the intrinsic ZT from measured ZT

  • We studied the electrical and thermal extrinsic effects on the Harman method

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Summary

Introduction

Accurate evaluation of thermoelectric figure-of-merit, ZT =α2T/ρk, is of great importance to the development of thermoelectric materials, where α is the Seebeck coefficient, ρ is the electrical resistivity, k is the thermal conductivity, and T is the absolute temperature[1,2,3,4,5,6]. The model simulates the Harman measurement by calculating the thermal and electrical potential distributions over the sample and lead wires. To find appropriate input values of ρ for the test materials, we fit ρs to the measured resistivity (ρm) for all the sample shapes and current source types.

Results
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