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Thermoelectric Materials - application brochure

Thermoelectric Materials - application brochure
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Thermoelectric Materials - application brochure

Product catalog summary
Introduction to Thermoelectricity
Thermoelectricity involves the conversion between temperature differences and electric potential, encompassing the Seebeck, Peltier, and Thomson effects. Key materials include metals and semiconductors, with bismuth telluride (Bi2Te3) being commonly used.

Figure of Merit (ZT)
Efficiency in thermoelectric materials is measured by the figure of merit, ZT, which depends on high Seebeck coefficients, high electrical conductivity, and low thermal conductivity. ZT is calculated as ZT = (S2σ/λ)T.

Thermoelectric Generation and Cooling
Thermoelectric generators convert temperature gradients into electricity using p-type and n-type semiconductors, while thermoelectric cooling transfers heat using an electric current.

Thermophysical Properties and Measurement Techniques
Thermal properties like stability and conductivity are crucial for thermoelectric materials. Techniques such as Laser Flash Analysis (LFA) measure thermal diffusivity and specific heat.

Advanced Measurement Systems
The LFA 467 HyperFlash and LFA 457 MicroFlash® systems measure thermal properties across a wide temperature range, featuring automatic sample changers and vacuum-tight designs.

Software and Analysis
Proteus® software provides sophisticated analysis capabilities for LFA systems, including thermal diffusivity models and heat-loss corrections.

Thermal Analysis Techniques
Differential Scanning Calorimetry (DSC) and Simultaneous Thermal Analysis (STA) study energetic effects and material properties, providing insights into specific heat capacity and thermal stability.

Standards and Applications
DSC and STA systems comply with international standards, ensuring reliable measurements for research and industrial applications.
Overview
This document analyzes dilatometry and thermomechanical analysis (TMA) techniques for measuring thermal properties of materials, focusing on thermoelectric applications. It discusses NETZSCH instruments and presents data on materials like bismuth telluride and lead telluride.

Dilatometry and Thermomechanical Analysis
Describes the use of dilatometers, such as the DIL 402 C and DIL 402 CD, for measuring dimensional changes with temperature. The TMA 402 F1 and F3 Hyperion® instruments are noted for their modular design and force measurement capabilities.

Key Specifications and Procedures
  • Interchangeable furnaces and pushrods optimize measurements for specific applications.
  • Adherence to standards like DIN EN 821, ASTM E831, and ISO 11359 in NETZSCH instrument design.

Thermal Conductivity and Figure of Merit
Discusses measuring thermal conductivity and ZT for thermoelectric materials, highlighting phonon scattering and nanostructured bulk thermoelectrics.

Material Analysis
  • Ag1-xPb18MTe20: Data on thermal conductivity and lattice conductivity influenced by temperature.
  • PbTe-Ge and PbTe-Ge1-xSix: Analysis of Ge and Si alloying effects on lattice conductivity.
  • Skutterudite materials: Nanoparticles in La0.9CoFe3Sb12 reduce thermal conductivity and improve ZT.

Thermal Expansion and Specific Heat
Measurements for bismuth telluride materials show composition differences do not significantly impact thermal expansion.

Conclusion
Emphasizes the importance of characterizing materials like PbTe for thermoelectric applications, focusing on thermal diffusivity and conductivity measurements.
Characterization of PbTe

Thermal Stability Analysis:
Analyzed using STA 409 CD with a mass spectrometer via the SKIMMER® system, showing PbTe decomposition at around 600°C with various gaseous products detected.

Mass Spectrometer Data:
Presented alongside TGA, DTG, and/or DSC curves, showing a low mass loss of 0.08% due to impurities and Pb and Te fragments.

Additional Observations:
Mass number 80 u attributed to stable isotope 80Se, with other mass numbers linked to organic impurities and substrate material.

Company Information:
NETZSCH-Gerätebau GmbH specializes in thermal analysis and thermophysical property determination, offering a broad product line and services globally.
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Catalog excerpts

Thermoelectric Materials - application brochure-1

Analyzing & Testing Thermoelectric Materials Material Characterization, Phase Changes, Thermal Conductivity Leading Thermal Analysis

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Thermoelectric Materials - application brochure-2

Thermoelectricity - Thermoelectric Materials and Devices Thermoelectricity refers to a class of phenomena in which a temperature difference creates an electric potential or an electric potential creates a temperature difference. In modern technical usage, the term refers collectively to the Seebeck effect, Peltier effect, and the Thomson effect. Various metals and semiconductors are generally employed in these applications. One of the most commonly used materials in such applications is bismuth telluride (Bi2Te3). Over recent decades, efforts have been made to improve the efficiency of thermal...

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Thermoelectric Materials - application brochure-3

PbTe TAGS ZT is a very convenient figure for comparing the potential efficiency of devices constructed of different materials. Values of ZT = 1 are considered good, but values in at least the 3-4 range would be considered essential in order to be competitive in terms of efficiency with regards to mechanical energy generation and refrigeration. To date, however, such values have not been achieved; the best reported ZT values have been in the 2-3 range. Approximate figure of merit (ZT) for various p-type and n-type thermoelectric materials. Source: G. Jeffrey Snyder, California Institute of Technology...

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Thermoelectric Materials - application brochure-4

Thermoelectric Materials - The Focal Point for Energy Savings Novel thermoelectric materials have already resulted in a new consumer product: a simple, efficient way of cooling car seats in hot climates. The devices, similar to the more familiar car seat heaters, provide comfort directly to the individual rather than cooling the entire car, saving on air-conditioning and energy costs. To optimize a thermoelectric device, its thermal properties must be known. The thermal conductivity (analyzed with LFA) is directly related to the efficiency of a thermoelectric material. The thermal stability (analyzed...

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Thermoelectric Materials - application brochure-5

The LFA method is illustrated in the figure on page 4, on the left. The front surface of a plane-parallel sample is heated by a short light or laser pulse. The resulting temperature rise on the rear surface is measured versus time using an IR detector. The thermal diffusivity (a) and in most cases also the specific heat (cp) can be determined from the measured signal. If the density (p) is known, the thermal conductivity (A) can be determined as follows: A(T) = a (T) ■ cp(T) ■ p(T) where: A = thermal conductivity [W/(m-K)] p = bulk density [g/cm3] cp = specific heat [J/(g-K)]. The Laser Flash...

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Thermoelectric Materials - application brochure-6

The LFA 457 MicroFlash® incorporates the latest state-of-the-art technology for laser flash systems. This bench-top instrument allows for measurements from -125°C to 1100°C using two different interchangeable furnaces. The temperature increase on the back surface of the sample can be measured at very low sub-ambient temperatures thanks to the innovative infrared sensor technology. The instrument accommodates both smaller and larger sample sizes (of up to 25.4 mm in diameter) and with the integrated sample changer, measurements can be run on several samples at the same time. The vacuum-tight design...

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Thermoelectric Materials - application brochure-7

The Laser Flash systems run under Proteus® software on a Windows® operating system. The combination of easy-to-understand menus and automated routines makes this software very user-friendly while still allowing for sophisticated analysis. The LFA software includes: Calculation models for thermal diffusivity: Adiabatic Cowan Improved Cape-Lehman (via consideration of multidimensional heat loss and non-linear regression) 2-/3-layer models (analysis by means of non-linear regression and consideration of heat loss) In-plane Radiation correction (for transparent and semi-transparent samples) Heat-loss...

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Thermoelectric Materials - application brochure-8

Thermal Analysis – DSC and STA; Coupling to Evolved Gas Analysis Heat Flow DSC Method Differential Scanning Calorimetry Thermogravimetric Analysis and Simultaneous Thermal Analysis Based on a homogeneous temperature field in the DSC furnace, equal heat flows along the disc-shaped sensor are directed to the sample and reference crucibles. If the heat capacities on the sample and reference sides differ, or if the sample shows a changed heat absorption or resulting difference in heat flow causes temperature gradients at the sensor. Sensitive sensors record these temporary deviations, which are then...

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Thermoelectric Materials - application brochure-9

STA Analysis Information Combines Analysis Information from DSC and TGA DSC Analysis Information Specific heat capacity (cp) Melting/crystallization behavior Solid-solid transitions Polymorphism Degree of crystallinity Glass transitions Cross-linking reactions Oxidative stability Purity Determination DSC data as base for thermokinetic analysis (NETZSCH Thermokinetics software program) Mass changes Temperature stability Oxidation/reduction behavior Decomposition Corrosion studies Compositional analysis TGA data as base for thermokinetic analysis (NETZSCH Thermokinetics software program) Coupling...

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Thermoelectric Materials - application brochure-10

Dilatometry and Thermomechanical Dilatometer Method Analysis Dilatometry (DIL) is used to measure the expansion or shrinkage of solids, powders, pastes or liquids under negligible load. It is closely related to thermomechanical analysis (TMA), which determines dimensional changes under a defined mechanical force. We offer dilatometer systems for measurements in the temperature range between approx. -260°C and 2800°C. For the investigation of thermoelectric materials, either our DIL 402 C or our dual/differential DIL 402 CD (-180°C to 2000°C) may be used. The specific needs of this application...

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Thermoelectric Materials - application brochure-11

Irrespective of the selected type of deformation (expansion, compression, penetration, tension or bending), any length change in the sample is communicated to a highly sensitive inductive displacement transducer (LVDT) via a pushrod and transformed into a digital signal. The pushrod and corresponding sample holders of fused silica or aluminum oxide can be quickly and easily changed out to optimize the system to a given application. Linear thermal expansion Coefficient of thermal expansion (CTE) Volumetric expansion Shrinkage steps Glass transition temperature Phase transitions Sintering temperature/sintering...

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