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Related Concept Videos

Superconductor01:24

Superconductor

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A substance that reaches superconductivity, a state in which magnetic fields cannot penetrate, and there is no electrical resistance, is referred to as a superconductor. In 1911, Heike Kamerlingh Onnes of Leiden University, a Dutch physicist, observed a relation between the temperature and the resistance of the element mercury. The mercury sample was then cooled in liquid helium to study the linear dependence of resistance on temperature. It was observed that, as the temperature decreased, the...
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A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
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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.
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Theory of Metallic Conduction01:17

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The Carnot engine works between two heat reservoirs of fixed temperatures. The Carnot cycle begs the following question: Is it possible to devise a heat engine that is more efficient than a Carnot engine between two fixed temperatures? The answer lies in designing a Carnot refrigerator.
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The second law of thermodynamics can be stated in several different ways, and all of them can be shown to imply the others. The Clausius’ statement of the second law of thermodynamics is based on the irreversibility of spontaneous heat flow. It states that heat will not flow from the colder body to the hotter body unless some other process is involved. Additionally, as per the Kelvin’s statement, it is impossible to convert the heat from a single source into work without any other...
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Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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Resolving thermoelectric "paradox" in superconductors.

Connor D Shelly1, Ekaterina A Matrozova2, Victor T Petrashov1

  • 1Department of Physics, Royal Holloway, University of London, Egham, Surrey TW20 0EX, UK.

Science Advances
|March 3, 2016
PubMed
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This study resolves a century-old physics paradox concerning thermoelectricity in superconductors. Researchers reconciled theoretical predictions with experimental data, enabling new investigations into thermoelectric phenomena.

Keywords:
physicsquantum interference devicessuperconductorsthermoelectricity

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Area of Science:

  • Condensed Matter Physics
  • Quantum Materials

Background:

  • Thermoelectricity in superconductors has been a debated topic for nearly a century.
  • Early research questioned the existence of these effects, with later work suggesting they might occur in inhomogeneous superconductors.

Purpose of the Study:

  • To resolve the long-standing discrepancies between theoretical predictions and experimental observations of thermoelectric effects in superconductors.
  • To address the inconsistencies that led to a stalemate in the field.

Main Methods:

  • The study likely involved advanced theoretical modeling and precise experimental measurements to re-evaluate thermoelectric phenomena in superconducting systems.
  • Reconciliation of conflicting data through rigorous analysis.

Main Results:

  • The research successfully resolved the "paradox" by aligning theoretical frameworks with experimental findings.
  • Established a consistent understanding of thermoelectricity in superconductors.

Conclusions:

  • This work overcomes a major hurdle in understanding superconductivity and thermoelectricity.
  • Opens new avenues for exploring recently predicted novel thermoelectric phenomena in superconductors.