Thermoelectric properties of Co substituted synthetic tetrahedrite

被引:99
作者
Chetty, R. [1 ]
Bali, A. [1 ]
Naik, M. H. [2 ]
Rogl, G. [3 ,4 ]
Rogl, P. [3 ,4 ]
Jain, M. [2 ]
Suwas, S. [5 ]
Mallik, R. C. [1 ]
机构
[1] Indian Inst Sci, Dept Phys, Thermoelect Mat & Devices Lab, Bangalore 560012, Karnataka, India
[2] Indian Inst Sci, Dept Phys, Bangalore 560012, Karnataka, India
[3] Univ Vienna, Inst Mat Chem & Res, A-1090 Vienna, Austria
[4] Vienna Univ Technol, Christian Doppler Lab Thermoelect, A-1090 Vienna, Austria
[5] Indian Inst Sci, Dept Mat Engn, Bangalore 560012, Karnataka, India
关键词
Tetrahedrite; X-ray diffraction (XRD); Scanning electron microscopy (SEM); Transport properties; Elastic properties; RAY PHOTOELECTRON-SPECTROSCOPY; THERMAL-CONDUCTIVITY; PERFORMANCE; CRYSTAL; NICKEL;
D O I
10.1016/j.actamat.2015.08.040
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Transition metal atom (Co) substituted synthetic tetrahedrite compounds Cu12-xCoxSb4S13 (x = 0, 0.5, 1.0, 1.5, 2.0) were prepared by solid state synthesis. X-Ray Diffraction (XRD) patterns revealed tetrahedrite as the main phase, whereas for the compounds with x = 0, 0.5 a trace of impurity phase Cu3SbS4 was observed. The surface morphology showed a large grain size with low porosity, which indicated appropriate compaction for the hot pressed samples. The phase purity, as monitored by Electron Probe Micro Analysis (EPMA) is in good agreement with the XRD data. The elemental composition for all the compounds almost matched with the nominal composition. The X-ray Photoelectron Spectroscopy (XPS) data showed that Cu existed in both +1 and +2 states, while Sb exhibited +3 oxidation states. Elastic modulus and hardness showed a systematic variation with increasing Co content. The electrical resistivity and Seebeck coefficient increased with increase in the doping content due to the decrease in the number of carriers caused by the substitution of Co2+ on the Cu1+ site. The positive Seebeck coefficient for all samples indicates that the dominant carriers are holes. A combined effect of resistivity and Seebeck coefficient leads to the maximum power factor of 1.76 mW m(-1) K-2 at 673 K for Cu11.5Co0.5Sb4S13. This could be due to the optimization in the carrier concentration by the partial substitution of Co2+ on both the Cu1+ as well as Cu2+ site at the same doping levels, which is also supported by the XPS data. The total thermal conductivity systematically decreased with increase of doping content as it is mainly influenced by the decrease of carrier thermal conductivity. The maximum thermoelectric figure of merit zT = 0.98 was obtained at 673 K for Cu11.5Co0.5Sb4S13. (C) 2015 Acta Materialia Inc. Published by Elsevier Ltd. All rights reserved.
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页码:266 / 274
页数:9
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