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| | Symbolic Analysis of Magnetic Field with |
 | | r x J dv is the magnetic moment of the current distribution (m =iA in the case of a filamentary one-turn coil of area A), relation which shows the decrease of the field inversely proportional to the cube of the distance to the source. |
 | | The vector potential given by (4) is solenoidal (has div A = 0), if the divergence of the current density is zero in the whole conducting domain (respectively, if the normal component of the current density, Jn, is zero on the surface of the conductor). |
 | | In this case, the vector potential has only one component, normal to the problem's plane (A is represented by a scalar rather than a vector), and the magnetic field lines coincide with the equipotential lines. |
| www.ewh.ieee.org /soc/es/May2001/03/bsl1.html (1266 words) |
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