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Related Concept Videos

Efficiency of The Carnot Cycle01:16

Efficiency of The Carnot Cycle

The hypothetical Carnot cycle consists of an ideal gas subjected to two isothermal and two adiabatic processes. Since the internal energy of an ideal gas depends only on its temperature, which is the same before and after the completion of the Carnot cycle, there is no change in its internal energy. Hence, using the first law of thermodynamics, the total heat exchanged by the ideal gas equals the total work done. Thus, we can quantify the efficiency of the Carnot cycle via the heat exchanged...
The Joule and Joule–Thomson Experiments01:23

The Joule and Joule–Thomson Experiments

Consider an adiabatic system composed of two chambers, A and B, designed such that no heat flows into or out of the system. Initially, chamber A is filled with a gas at a fixed temperature T1, pressure p1, and volume V1, while chamber B is evacuated. The gas is then gradually forced through a rigid, porous barrier to chamber B, ultimately reaching temperature T2, pressure p2, and volume V2. A piston on the right side maintains a constant pressure (p2), which is lower than p1. The significant...
Joule-Thomson Effect01:21

Joule-Thomson Effect

The Joule-Thomson effect, also known as the Joule-Kelvin effect, describes the temperature change of a fluid when it is forced through a valve or porous plug while keeping it in a thermally insulated environment. This experiment is called a throttling process. This is an important effect widely used in refrigeration and the liquefaction of gases.
This experiment forces high-pressure gas through a throttle valve or a porous plug to a lower-pressure region. The gas expands as it passes through to...
Carnot Cycle and Efficiency01:26

Carnot Cycle and Efficiency

The Second Law of Thermodynamics asserts that it's impossible for any heat engine to achieve 100% efficiency. While contemplating the maximum possible efficiency, Nicolas Sadi Carnot conceptualized an ideal heat engine. This engine gets its energy from a high-temperature reservoir. It then performs some work and releases the remaining energy into a low-temperature reservoir.The Carnot cycle, named after Sadi Carnot, is fully reversible. The cycle consists of four distinct stages. In the first...
Thermodynamic Potentials01:26

Thermodynamic Potentials

Thermodynamic potentials are state functions that are extremely useful in analyzing a thermodynamic system. They have dimensions of energy. The four important thermodynamic potentials are internal energy, enthalpy, Helmholtz free energy, and Gibbs free energy. These thermodynamic potentials can be expressed using two of the following variables: pressure, volume, temperature, and entropy. These two variables are expressed as the rate of change of the thermodynamic potential with respect to other...
The Carnot Cycle01:30

The Carnot Cycle

Converting work to heat is an irreversible process, and the purpose of a heat engine is to reverse the effect partially. Heat engines aim to increase the efficiency of the reversal, that is, maximize the work retrieved from heat. If the efficiency of a heat engine were 100%, it would imply reversing the process completely without introducing any other effect. Thus, it would violate the second law of thermodynamics.
What could be the theoretical limit to the efficiency of a heat engine? The...

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Related Experiment Video

Updated: Jun 19, 2026

Synthesis of Non-uniformly Pr-doped SrTiO3 Ceramics and Their Thermoelectric Properties
11:07

Synthesis of Non-uniformly Pr-doped SrTiO3 Ceramics and Their Thermoelectric Properties

Published on: August 15, 2015

Thermoelectric properties and efficiency measurements under large temperature differences.

A Muto1, D Kraemer, Q Hao

  • 1Department of Mechanical Engineering, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.

The Review of Scientific Instruments
|October 2, 2009
PubMed
Summary

This study introduces a new method to accurately measure thermoelectric material properties. The technique reduces uncertainties in the dimensionless figure of merit (ZT) for improved generator efficiency.

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Area of Science:

  • Materials Science
  • Thermoelectric Energy Conversion
  • Solid State Physics

Background:

  • Thermoelectric generator efficiency relies on the material's dimensionless figure of merit (ZT).
  • Accurate ZT determination is challenging due to temperature-dependent properties and measurement uncertainties from using multiple tools and samples.
  • Existing methods often lead to significant uncertainties in reported ZT values.

Purpose of the Study:

  • To present a novel experimental technique for precise characterization of thermoelectric materials.
  • To reduce uncertainties in measuring thermoelectric properties and conversion efficiency.
  • To provide a reliable method for material evaluation before thermoelectric generator implementation.

Main Methods:

  • A single experimental setup measures Seebeck coefficient, electrical conductivity, and thermal conductivity of a single thermoelectric leg.
  • Measurements are performed under a large temperature difference (2-160 °C).
  • The technique involves a single mounting of the thermoelectric leg, ensuring consistent measurement direction and corroboration via efficiency measurements.

Main Results:

  • The new technique minimizes uncertainties associated with individual property measurements.
  • Directly measured power and efficiency closely match values calculated from the measured properties, with agreement within 0.4% and 2%, respectively.
  • The experimental approach validates the accuracy of the measured thermoelectric parameters.

Conclusions:

  • The developed experimental technique offers a more reliable method for thermoelectric material characterization.
  • It provides accurate ZT values and efficiency data under realistic operating conditions.
  • This method is ideal for pre-implementation material assessment in thermoelectric generators.