Abstract

The Nernst thermopower usually is considered far too weak in most metals for waste heat recovery. However, its transverse orientation gives it an advantage over the Seebeck effect on non-flat surfaces. Here, we experimentally demonstrate the scalable generation of a Nernst voltage in an air-cooled metal wire coiled around a hot cylinder. In this geometry, a radial temperature gradient generates an azimuthal electric field in the coil. A Galfenol (Fe0.85Ga0.15) wire is wrapped around a cartridge heater, and the voltage drop across the wire is measured as a function of axial magnetic field. As expected, the Nernst voltage scales linearly with the length of the wire. Based on heat conduction and fluid dynamic equations, finite-element method is used to calculate the temperature gradient across the Galfenol wire and determine the Nernst coefficient. A giant Nernst coefficient of -2.6 μV/KT at room temperature is estimated, in agreement with measurements on bulk Galfenol. We expect that the giant Nernst effect in Galfenol arises from its magnetostriction, presumably through enhanced magnon-phonon coupling. Our results demonstrate the feasibility of a transverse thermoelectric generator capable of scalable output power from non-flat heat sources.

Highlights

  • Thermoelectric power generation is considered an environmentally friendly approach to convert waste heat into electrical energy

  • Due to the orthogonality of the Nernst electric field to the thermal gradient, the Nernst thermopower can be increased linearly with the thermoelectric generator length without introducing the conventional thermopile structure

  • The total Nernst effect consists of ordinary (EONE) and anomalous (EANE) components: EONE = NONE μ0 H × ∇T, (1)

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Summary

Introduction

Thermoelectric power generation is considered an environmentally friendly approach to convert waste heat into electrical energy. The heater generates a radial temperature gradient, ∇T = ∇Trr, throughout the Galfenol wire and a magnetic field in the axial direction, H = Hzz, is applied.

Results
Conclusion
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