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Measuring devices for thermoelectrics

Waste heat recovery / Thermoelectric generators (TEG) / Peltier elements / Sensors

LSR-1

Seebeck coefficient and electrical resistance are measured fully automatically and simultaneously from -160°C to 200°C.

Details

LSR-3

Linseis LSR-3
  • Measurement of the Seebeck coefficient and electrical conductivity on solid materials and thin films
  • Temperature range from -100°C to +1500°C

Details

TEG-Tester

TIM-Tester new instrument

The Linseis TEG Tester is a measuring system for temperature-dependent efficiency evaluation of thermoelectric generators (TEGs).

Details

LZT-Meter

LZT-Meter
  • Combined LFA + LSR
  • Measurement of the Seebeck coefficient, resistivity and thermal diffusivity
  • Temperature range -100°C to +1100°C

for a complete ZT measurement

Details

HCS 1/10/100

Hall effect analyzer HCS 1

The HCS system enables the characterization of semiconductor devices and measures: the charge carrier mobility, the resistivity, the charge carrier concentration as well as the Hall constant

Details

TFA

Linseis TFA
  • Complete ZT characterization on thin films from nm to µm range
  • Optional measurement of Hall coefficient, charge carrier density and mobility
  • Temperature range -160°C to +280°C

Details

TF-LFA

Linseis TF-LFA

TF-LFA – Time Domain Thermoreflectance (TDTR) – Measurement of thermal diffusivity on thin films

Details

Seebeck, Peltier and Thomson effect

Short insight

Thermoelectricity generally describes the mutual influence of temperature and electricity in a material and is based on three fundamental effects: the Seebeck effect, the Peltier effect and the Thomson effect. The Seebeck effect was discovered in 1821 by Thomas J. Seebeck, a German physicist, and describes the occurrence of an electric field when a temperature gradient is applied in an electrically insulated conductor. The Seebeck coefficient S is defined as the quotient of negative thermoelectric voltage and temperature difference and is a purely material-specific quantity, usually given in the unit µV/K.

 

In the opposite case, this effect, then called the Peltier effect, causes the expression of a temperature gradient when an external current is applied to the conductor. This phenomenon is due to the different energy levels of the conduction bands of the materials involved. Thus, during the transition from one material to the other, the charge carriers must either absorb energy in the form of heat, causing the contact point to cool down, or they can release energy in the form of heat, causing the contact point to warm up.

In view of the ever increasing scarcity of fossil fuels and the recent findings on global warming due to rising carbon dioxide emissions, the field of thermoelectricity has once again become a focus of public interest due to its effective use of waste heat. The aim is to use the waste heat from heat engines, such as automobiles or conventional power plants, by thermoelectric generators (TEG) to increase their efficiency. However, efficient thermoelectric materials are also of great interest for cooling applications using the Peltier effect, such as the thermostatting of temperature-critical components in lasers.

The thermoelectric conversion efficiency of a material is usually compared using the dimmingless figure of merit ZT. This is calculated from the thermal conductivity, the Seebeck coefficient and the electrical conductivity.

To meet this trend, we have developed an instrument for simple and extremely precise material characterization. The Linseis LSR-3 can determine both the Seebeck coefficient and the electrical resistivity of a sample in a temperature range from -100° C to 1500°C in a single measurement.

 

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Overview of applications and samples

Below you will find an overview of the various measuring instruments for thermoelectrics. This should serve you as an orientation. If you have questions about a measurement or a material, you can always send us a message via the contact form.

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Green: Measurement possible

Yellow: Measurement possibly possible

Gray: Measurement not possible

Model LSR-3 LSR-4 LZT HCS TFA
Info Standard Plattform Harman Upgrade for LSR-3 Combination of LSR-3 + LFA 1000 additionally with Hall constant Thin films on Linsei’s chip
Measurements
Seebeck coefficient ja Smiley ja Smiley ja Smiley ja Smiley ja Smiley
Resistivity/Conductivity ja Smiley ja Smiley ja Smiley ja Smiley ja Smiley
Hall Konstante/ Hall mobility / Load carrier nein Smiley nein Smiley nein Smiley ja Smiley ja Smiley
Thermal diffusivity nein Smiley nein Smiley ja Smiley nein Smiley ja Smiley
Thermal conductivity nein Smiley ja Smiley*Hinweis beachten nein Smiley nein Smiley ja Smiley
Complete ZT characterization nein Smiley ja Smiley ja Smiley nein Smiley ja Smiley
Atmosphere ja Smiley
ja Smiley ja Smiley
ja Smiley ja Smiley
Temperature range -100 up to +1500°C -100 up to +1500 (Harman -100 bis 300) -100 up to +1100 -150 up to +600 -170 up to +300°C
Price $$ $$ $$$ $ $$$
Samples
solid ja Smiley ja Smiley ja Smiley ja Smiley nein Smiley
Thin films ja Smiley eventuell smiley**Hinweis beachten eventuell smiley***Hinweis beachten nein Smiley ja Smiley

* Calculated thermal conductivity from the Harman method for direct ZT measurement. The Harman method is only applicable for good thermoelectric samples from -100°C to +300°C.

** Seebeck and resistivity of thin films can be measured, but the Harman method is only applicable to solids, not thin films.

*** Seebeck and thin film resistivity can be measured, but the LFA method is only applicable to solids and thicker films (> 100 µm).

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Linseis Produktbroschüre Thermal Electrics

LSR, LZT, LFA, TF-LFA, TFA, Hall Effect
Product brochure (PDF)

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Linseis Product Overview English

Product Overview
ENGLISH (PDF)

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