The Meissner effect is a fundamental phenomenon observed in superconductors, which are materials that exhibit zero electrical resistance and the expulsion of magnetic fields when cooled below a certain critical temperature. The effect was first discovered by physicists Walther Meissner and Robert Ochsenfeld in 1933.
When a superconductor is cooled below its critical temperature, it undergoes a phase transition, entering a state of perfect conductivity for electric current and perfect diamagnetism for magnetic fields. In other words, it expels almost all magnetic flux from its interior, causing magnetic fields to be excluded from the bulk of the superconductor. This expulsion of magnetic fields results in the levitation of the superconductor in the presence of an external magnetic field, a phenomenon commonly known as "magnetic levitation" or "quantum locking."
The Meissner effect is a consequence of the formation of pairs of electrons, known as Cooper pairs, in the superconducting material. These Cooper pairs interact with lattice vibrations (phonons) and are able to move through the lattice without scattering, leading to the complete absence of electrical resistance. Additionally, these pairs also interact with magnetic fields in such a way that the expulsion of magnetic flux occurs, giving rise to the Meissner effect.
The Meissner effect is a crucial property of superconductors and has practical applications in various fields, including in the development of high-performance magnets for applications like magnetic resonance imaging (MRI) machines, particle accelerators, and magnetic levitation transportation systems (maglev trains).