A Formulation for HTS

This section presents the implementations of the A Formulation on High critical Temperature Superconductors :

1. Description of the problem

The section describes a problem of magnetization on a bulk cylinder made of a High critical Temperature Superconductor material :

cylindre1
Figure 1. Bulk cylinder

The E-J Power Law define High critical Temperature Superconductors in the modeling. For the A Formulation, the E-J power law is defined in the electric conductivity \(\sigma\) :

E-J power law
\[J=\sigma(E)E=\frac{J_c}{E_c}\left(\frac{\mid\mid E\mid\mid}{E_c}\right)^{(1-n)/n} E\]

With :

  • \(J\) : electric current density \((A/m^2)\)

  • \(E\) : electric filed \((V/m)\)

  • \(J_c\) : critical current density \((A/m^2)\) (the critical current is dependent of the temperature and magnetic field but here we will use it as a constant)

  • \(E_c\) : threshold electric field \((V/m)\)

  • \(n\) : material dependent exponent

If the electric current density is close to the critical density, the material starts to lose its superconducting properties :

jc ec