“…It is evident that the flow pattern in the melt under no magnetic field is characterized by a large scale turbulent convective cell, however, a flow transition from large scale buoyancy driven to small scale magnetically driven turbulence occurs when rotating magnetic field is applied [10]. Here, we can see from 1 and case 2 is opposite to that of case 3, this is because the large convective cell below the crystal is controlled by the rotation of crystal.…”
Section: Resultsmentioning
confidence: 77%
“…The results showed that the flow motion consists of a primary flow in the azimuthal direction and a secondary flow in a meridional plane, which have three-dimensional and time-dependent structures, and that the strength and frequency of the rotating magnetic fields affect the time-dependent structure of the flow. Grants and Gerbeth [10] demonstrated experimentally in a low temperature model that a RMF has the potential to stabilize the inverse temperature gradient in a medium scale Czochralski facility with a high initial melt level. It means that the inverse temperature gradient is conducive to make flow unstable, however, under the influence of RMF the stabilization occurs as a result of a flow transition from large scale buoyancy driven to small scale magnetically driven turbulence.…”
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