The symmetry of Dirac-Maxwell equations permits a steady current of magnetic monopoles to produce a static curled electric field around the current. An electric charge placed in it experiences an electrical force along the direction of the field about which the field is asymmetric. This asymmetry should reflect into the resulted motion of the charge. The usual electrical force equation F = qE; expressed in terms of the test charge and the applied electric field and may be referred as charge-field interaction; do not account this asymmetry. Therefore; it needs a generalization permitting the exertion of the force by the applied electric field on the electric field of the test charge; referred as field-field interaction. It accounts the asymmetry in the applied electric field. The possible effects of such generalization are analyzed. It is found that the behavior of an electric charge placed in a static curled electric field is similar to the behavior of the charge when placed in a static magnetic field. Therefore; it suggests that the true face of magnetic field can be curled electric field. It supports not only to the absence of magnetic monopoles in the universe but also provides a means to remove the magnetic field stuck to the electric charges.
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