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    Superconductivity

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    • Introduction to Superconductivity
      • 1.1History and Discovery of Superconductivity
      • 1.2Basic Concepts and Definitions
      • 1.3Importance and Applications of Superconductivity
    • Theoretical Foundations
      • 2.1Quantum Mechanics and Superconductivity
      • 2.2BCS Theory
      • 2.3Ginzburg-Landau Theory
    • Types of Superconductors
      • 3.1Conventional Superconductors
      • 3.2High-Temperature Superconductors
      • 3.3Unconventional Superconductors
    • Superconducting Materials
      • 4.1Metallic Superconductors
      • 4.2Ceramic Superconductors
      • 4.3Organic Superconductors
    • Superconducting Phenomena
      • 5.1Meissner Effect
      • 5.2Josephson Effect
      • 5.3Flux Quantization
    • Superconducting Devices
      • 6.1SQUIDs
      • 6.2Superconducting Magnets
      • 6.3Superconducting RF Cavities
    • Superconductivity and Quantum Computing
      • 7.1Quantum Bits (Qubits)
      • 7.2Superconducting Qubits
      • 7.3Quantum Computing Applications
    • Challenges in Superconductivity
      • 8.1Material Challenges
      • 8.2Technological Challenges
      • 8.3Theoretical Challenges
    • Future of Superconductivity
      • 9.1Room-Temperature Superconductivity
      • 9.2New Superconducting Materials
      • 9.3Future Applications
    • Case Study: Superconductivity in Energy Sector
      • 10.1Superconducting Generators
      • 10.2Superconducting Transformers
      • 10.3Superconducting Cables
    • Case Study: Superconductivity in Medical Field
      • 11.1MRI Machines
      • 11.2SQUID-based Biomagnetism
      • 11.3Future Medical Applications
    • Case Study: Superconductivity in Transportation
      • 12.1Maglev Trains
      • 12.2Electric Vehicles
      • 12.3Future Transportation Applications
    • Review and Discussion
      • 13.1Review of Key Concepts
      • 13.2Discussion on Current Research
      • 13.3Final Thoughts and Course Wrap-up

    Types of Superconductors

    Conventional Superconductors: An In-depth Study

    electrical conductivity with exactly zero resistance

    Electrical conductivity with exactly zero resistance.

    Superconductivity, a phenomenon characterized by the complete disappearance of electrical resistance in certain materials when cooled below a critical temperature, has been a subject of intense study since its discovery in 1911. The materials that exhibit this phenomenon are known as superconductors, and they are broadly classified into two categories: conventional and unconventional. This article focuses on conventional superconductors, their characteristics, materials, and the theories explaining their superconductivity.

    Definition and Characteristics of Conventional Superconductors

    Conventional superconductors, also known as low-temperature superconductors, are materials that become superconducting at temperatures close to absolute zero (around -273.15 degrees Celsius). They were the first type of superconductors to be discovered and studied, hence the name 'conventional'.

    The primary characteristics of conventional superconductors include zero electrical resistance, the expulsion of magnetic fields (Meissner effect), and the quantization of magnetic flux. These properties make them ideal for applications such as magnetic resonance imaging (MRI), particle accelerators, and magnetic levitation trains.

    Low-Temperature Superconductors: Materials and Properties

    The most common materials that exhibit conventional superconductivity are pure metals like mercury, lead, and tin, and metallic alloys like niobium-titanium (NbTi) and niobium-tin (Nb3Sn). These materials become superconducting at very low temperatures, typically below 30 Kelvin (-243.15 degrees Celsius).

    The properties of these materials, such as their critical temperature (the temperature below which they become superconducting), critical magnetic field (the maximum magnetic field they can withstand while remaining superconducting), and critical current density (the maximum electrical current they can carry while remaining superconducting), are well understood and can be accurately predicted using established theories.

    Theories and Models Explaining Conventional Superconductivity

    The phenomenon of superconductivity in conventional superconductors is well explained by the BCS (Bardeen–Cooper–Schrieffer) theory. Proposed in 1957, the BCS theory describes how electrons in a superconductor form pairs, known as Cooper pairs, and move through the lattice structure of the material without scattering off impurities or lattice vibrations, thus resulting in zero electrical resistance.

    The BCS theory has been extremely successful in explaining the properties of conventional superconductors and has been a cornerstone in the field of superconductivity. However, it fails to explain the behavior of high-temperature and unconventional superconductors, which has led to the development of new theories and models.

    In conclusion, conventional superconductors, with their unique properties and well-understood behavior, continue to play a crucial role in many technological applications. The ongoing research in this field aims to discover new materials and improve the properties of existing ones, paving the way for more efficient and practical uses of superconductivity.

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    Next up: High-Temperature Superconductors