Over the last few decades, there has been growing interest for developing technologies aimed at providing cleaner and more sustainable energy sources. Great efforts are directed towards synthesis of newer functional materials and tailoring the existing ones with an aim to optimize their usability. As materials are being developed with various complexities in their physical properties and forms like single crystals, thin-films, nanostructure and composites, measurement of their basic physical properties is also getting equally challenging. This review deals with a brief summary of our efforts in developing the basic understanding of some functional materials, using experimental tools that are best known to us, viz. measurement of Seebeck coefficient and X-ray absorption fine structure spectroscopy (XAFS). In particular, we discuss the results of our investigation of magnetic shape memory alloy Ni 2 MnGa and multiferroic CdCr 2 Se 4 . Keywords: Magnetic shape memory alloys, XAFS, thermopower measurements, spin-phonon coupling, magnetic semiconductors.
IntroductionTHE present age research in materials science is largely focussed around providing alternative technologies aimed at cleaner and more sustainable energy sources. Hence the mention of thermoelectric power in the perspective of contemporary research generally implies new schemes for materials synthesis and device fabrication with enhanced performance. This article, however, focusses on thermopower and XAFS measurements as an investigative tool, used for understanding material properties, not limited to thermoelectrics.
What is thermoelectric power?In most simple terms, thermoelectric power or thermoelectricity is all about generating electrical power from heat, using a solid-state device without combustion or moving parts. It is an effect that involves interplay between electrical and thermal properties of a material with electrons acting as the active fluid. The two primary physical phenomena that are at play in thermoelectrics are the Seebeck effect and the Peltier effect.Discovered in 1821 by T. J. Seebeck and hence named after him, this effect describes how a temperature gradient (T) across a conductor leads to electric charge flow, causing a measureable potential gradient (V) across it. Thus, V = ST, where S is the Seebeck coefficient. The opposite effect, i.e. generation of temperature gradient upon passage of electric current (I) through a conductor was discovered by J. Peltier. The expression for heat absorbed/emitted being, Q = I, where is the Peltier coefficient. It was not until 1855, when W. Thomson (Lord Kelvin), using thermodynamics laws, showed that the Seebeck and Peltier effects are basically inter-linked. He also pointed out the need for the third effect to be considered, which is reversible heating or cooling when there is both a flow of electric current and a temperature gradient.Thus was the birth of a concept -a type of heat engine that could be used either as a device for generating electricity from heat or, alternatively, as a h...