Table 1.
Expected compass responses for a torque detector based on magnetic remanence and anisotropic susceptibility, respectively. Realization of a polar compass requires a remanence-based detector that transduces both magnitude and rotational sense of the torque, m × H (equation (2.1a)). Without transducing the sign (i.e. the rotational sense) of the torque, a remanence-based detector produces axial output information only. |m × H|, magnitude of torque and |m × H| = 0, null-detector principle according to Edmonds (1992).
remanence, m |
anisotropic susceptibility χ |
|||
---|---|---|---|---|
m × H | |m × H| | |m × H| = 0 | χH × H | |
polar compass | + | − | − | − |
axial compass | − | + | + | + |