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If the magnetic field is formed by an external source, the conditions for the development of the interchange instability are not satisfied. However, it can be excited by a relatively weak field in the plasma when the conditions for the transformation of the plasma particles into the magnetic field are satisfied.
The interchange instability was discovered by Langmuir in 1920. He found that the mode of the instability could be modified by a variety of factors such as the density, temperature and speed of the plasma. He concluded that the instability must be more complex than the development of small perturbations of a plasma and that the initial disturbance can grow into a moving plasma that carries a new magnetic field. He also found that the instability is more efficient in a gas with a low density, whereas a higher density layer is required to excite the instability.
The interchange instability can also be used to produce an electrostatic shock wave in a plasma. This shock is used in the physics of high energy density physics to study the behavior of a medium in conditions which are difficult to study with traditional methods. A shock wave occurs when an electrically conducting medium is suddenly heated. A shock wave is produced on a sample that is charged when it is brought into contact with a high voltage pulse. The hot sample undergoes a phase transition and undergoes a rapid cooling. The sample is left in an electrically neutral state.
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