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Figure 4. Diagram illustrates the inductive coupling of the RF field to a wire loop. The quantity B1 represents the strength and direction of the RF field with frequency ( ) in the presence of a conductive loop with area A. The time-varying magnetic field produced by the RF coils will induce an electromotive force (emf) in the coil, which will in turn cause a current flow. The magnitude of the force is given by: emf = B1 A sin , where is the angle between the direction of the B1 field and the plane of the coil. The maximum induced electromotive force occurs when the B1 field is perpendicular to the plane of the coil. For maximum patient safety, nonconducting fiber-optic cables should be used instead of conductors whenever possible.
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