3DT Equivalent Circuit Model
Consider
a domain composed by Normal Conducting (NC),
Superconducting (SC)
and Magnetizable (M)
materials which do not intersect, placed in empty space. The magnetizable bodies
are assumed as having an assigned M-B relation (in
the most general case non linear and hysteretic) as constitute law and null
electric conductivity. In the SC domain the power law is
assumed as the local constitutive relation between vectors E and J.
When HTS materials are considered, the power law is utilized only with reference
to the directions in the a-b plane of the crystal lattice; on the c-axis
direction a linear constitutive equation, with a low value of the conductivity,
is utilized. The current distribution inside the NC
regions
is denoted with Jext.
·
A continuous non-linear anisotropic E-J
characteristic is utilized.
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Copper
cylindrical wire with AC transport current
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Current Density |
Power Losses |
SC cylindrical wire with
time-varying transport current
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Current Density |
Power Losses |
¨ Experimental validation of the model in collaboration with CESI (Milano) is going on.