Abstract

Based on the idea that different temperatures generate different conduction electron densities and the resulting carrier diffusion generates the thermal electromotive force (emf), a new formula for the Seebeck coefficient (thermopower) S is obtained: S=(2/3)ln2(qn)-1εFkBD0, where kB is the Boltzmann constant, and q, n, εF, D0 are charge, carrier density, Fermi energy, density of states at εF, respectively. Ohmic and Seebeck currents are fundamentally different in nature, and hence, cause significantly different behaviors. For example, the Seebeck coefficient S in copper (Cu) is positive, while the Hall coefficient is negative. In general, the Einstein relation between the conductivity and the diffusion coefficient does not hold for a multicarrier metal. Multi-walled carbon nanotubes are superconductors. The Seebeck coefficient S is shown to be proportional to the temperature T above the superconducting temperature Tc based on the model of Cooper pairs as carriers. The S follows a temperature behavior, , where Tg ’= constant, at the lowest temperatures.

Highlights

  • In 2003 Lu et al and Kang et al [1,2] observed a logarithmic temperature T -dependence of the seebeck coefficient S in multiwalled carbon nanotubes (MWNTs) at low temperatures

  • The Seebeck coefficient S is shown to be proportional to the temperature T above the superconducting temperature Tc based on the model of Cooper pairs as carriers

  • Where TF F is the Fermi energy, in Equation (7), we obtain. This formula for S is often quoted in materials handbook [4]

Read more

Summary

Introduction

In 2003 Lu et al and Kang et al [1,2] observed a logarithmic temperature T -dependence of the seebeck coefficient S in multiwalled carbon nanotubes (MWNTs) at low temperatures. The Seebeck coefficient S of highly oriented pyrolytic graphite (HOPG), single crystal, is shown. This S is negative (“electron”-like) at low temperatures and become positive (“hole”-like) and constant above 150 K: Sgraphite. Conduction electrons are denoted by quotation marked “electrons” (“holes”) whereas generic electrons are denoted without quotation marks

Theory of the Seebeck Coefficient in a Metal
Simple Applications
Graphene and Carbon Nanotubes
Conduction in Multi-Walled Carbon Nanotubes
Seebeck Coefficient in Multi-Walled Carbon Nanotubes
Conduction Electrons in Graphite
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.