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Figure 12.9 shows an alternate two-dimensional geometry that applies to simulations of high-power plasma or metal pinches. Here, an axial current flows through a cylindrical system. Azimuthal symmetry implies that there is only one component of magnetic field, Bθ. Therefore, it is most convenient to cast the diffusion equation directly in terms of this quantity. For pinch applications we make two simplifying assumptions: the medium is nonmagnetic (μr=1) and there are no internal applied currents (Jo=0). Equation 12.42 becomes
()
Jc=1μo∇×B.