Magnetic Quincke rollers show both standard clockwise helical paths and anomalous counterclockwise motion under a rotating magnetic field, with the reversal explained by initial dipole orientation, field frequency, and starting velocity in a theoretical model.
The torque on the magnetic dipole, or the magnetic torque, therefore, becomes ๐ป๐ = ๐ ร ๐ฉ
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Regular and Anomalous Motion of Individual Magnetic Quincke Rollers Under Rotating Magnetic Field
Magnetic Quincke rollers show both standard clockwise helical paths and anomalous counterclockwise motion under a rotating magnetic field, with the reversal explained by initial dipole orientation, field frequency, and starting velocity in a theoretical model.