LZT

LZT

LZT

Product catalog summary
Introduction to Thermoelectricity: Thermoelectricity involves the conversion between temperature and electricity, characterized by three effects: Seebeck, Peltier, and Thomson. These effects often occur simultaneously, facilitating the conversion of temperature differences into electrical energy.
Seebeck Effect: Discovered by Thomas Johann Seebeck in 1821, this effect generates an electrical potential from a temperature difference across a metal or semiconductor. The Seebeck coefficient (S) quantifies this effect, calculated as USeebeck = S ∙ ΔT.
Peltier Effect: Identified by Jean Peltier in 1834, this effect is the reverse of the Seebeck Effect, where an external current induces heat transport changes between two conductors with different electric heat capacities.
Figure of Merit (ZT): Defined by Altenkirch, ZT is a measure of thermoelectric material quality, combining Seebeck coefficient, electrical conductivity, and thermal conductivity. High ZT values (2-3) indicate competitive performance against mechanical energy generators.
Innovative LZT-Analyzer: The LZT-Analyzer is the first commercial instrument to measure the Figure of Merit in a single measurement, enhancing efficiency in thermoelectric applications such as portable coolers and waste heat recovery systems.
Thermoelectric Generators (TEGs): TEGs convert heat directly into electrical energy using the Seebeck effect, with efficiencies around 5-10%. They are reliable, durable, and require low maintenance, commonly using materials like Bismuth telluride (Bi2Te3).
Measurement System Design: The system includes a Laser flash and Seebeck and Electric Resistivity Analyzer, measuring Seebeck coefficient, electric resistivity, and thermal conductivity to calculate ZT values. The design incorporates thermocouples, current electrodes, and a primary furnace.
Thermal Conductivity Measurement: Using the Laser Flash method, thermal diffusivity and specific heat are measured to calculate thermal conductivity, adhering to international standards like ASTM E-1461 and DIN 30905.
Applications: The LZT-Analyzer evaluates samples like (BiSb)2Te3, determining the optimal chemical mixture and production process for the best figure of merit. Diagrams illustrate thermal diffusivity, heat conductivity, resistivity, and Seebeck coefficient measurements.
Specifications: The LZT-Meter operates in a temperature range from -150°C to 1500°C, using static DC and four-terminal methods for measurement. It requires cooling water and supports various sample sizes and shapes.
Contact Information: LINSEIS GmbH and its international branches provide contact details for further inquiries and services.
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Catalog excerpts

LZT-2

Thermoelectricity describes the reciprocal interaction of temperature and electricity and their conversion into one another. There are three different effects—the Seebeck-Effect (Thermoelectric-Effect), the The Peltier-Effect is the inverted effect of the Seebeck-Effect. An exte- Peltier-Effect and the Thomson-Effect, which describe a reversible in- rior current produces a change of heat transport. This discovery was teraction between the both values. Nearly always these effects appear made 13 years after the Seebeck-Effect from Jean Peltier (1834). This effect appears, if two conductors with...

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LZT-3

In recent years, thermoelectricity has been increasingly used in ap- Altenkirch (1909, 1911) showed that good thermoelectric materials plications such as portable refrigerators, beverage coolers, electronic should possess large Seebeck coefficients, high electrical conductivity component coolers, and metal alloy sorting devices. Furthermore it and low thermal conductivity. These three values define the so called is used in thermoelectric generators for waste heat recovery (for ex- ample in cars to decrease CO2 emission) and solid state cooling or peltier-elements. Thermoelectric generators (TEG)...

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LZT-4

Measurement principle Seebeck Effect and Electric Resistivity The following picture shows the design of the measurement system. The sample is in a vertical way between the upper and the lower block. The lower block includes a secondary heater that causes a tempe- rature gradient. For the determination of the Seebeck-Coefficient the temperature difference and the thermo-electromotoric force dE (vol- With determination of the sample geometry and the distance of the tage) will be measured. The Seebeck-Coefficient can now be calcula- thermocouples the electric resistivity can be calculated. ted with...

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LZT-5

Thermal Conductivity / Thermal Diffusivity Principal of Measurement: Laser Flash The sample is positioned on a sample holder, located in a furnace. The Correspondence with International Standards. The LINSEIS LFA and XFA furnace is then held at a predetermined temperatures. At this tempera- operate in agreement with national and international standards such ture the sample surface is then irradiated with a programmed energy pulse (laser or xenon flash). This energy pulse results in a homogeneous temperature rise at the sample surface. The resulting temperature LINSEIS is offering an unparalleled...

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LZT-6

Measurement of a sample of the tellur family A batch of samples of the tellur family enriched with bismuth and an- tivity K in relation to temperature. The thermal diffusivity can directly be timony (BiSb)2Te3 was evaluated. As an example this can be a test measured with the LFA (Laser Flash system), and with the density (from series with changes in the chemical mixture and changes in the way the Dilatometer measurement) and the specific heat Cp (from the DSC the samples are manufactured. With the determination of the figure of measurement) the heat conductivity λ can be calculated. merit one...

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LZT-7

Figure of Merit (calculation) above temperature of (BiSb)2Te3 0.6 A4 Figure of Merit 0.4 From the LFA and LSR measurement an calculation: ZT=

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LZT-9

LINSEIS GmbH Vielitzerstr. 43 95100 Selb Germany Tel.: (+49) 9287–880 - 0 Fax: (+49) 9287–70488 E-mail: [email protected] LINSEIS Inc. 109 North Gold Drive Robbinsville, NJ 08691 USA Tel.: (+1) 609 223 2070 Fax: (+1) 609 223 2074 E-mail: [email protected] LINSEIS France Bureaux Paris 52 Boulevard Sébastopol 75003 Paris Tel.: (+33) 173-028 272 www.linseis.com Products: DIL, TG, STA, DSC, HDSC, DTA, TMA, MS/FTIR, In-Situ EGA, Laser Flash, Seebeck Effect, Thin Film Analyzer, Hall-Effect Services: Service Lab, Calibration Servi

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All Linseis Thermal Analysis catalogs and technical brochures

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