Table 1.

Fractional increase in magnetic energy, |$\mathcal {E}_{\rm mag}^{\rm str}/\mathcal {E}_{\rm mag}^0$|⁠, as a function of position of superconducting shell |$\mathcal {R}$|⁠. We consider a plausible range of values of |$\mathcal {R}$| in increments of |$0.05R_*$|⁠, and also the ‘fiducial’ model with |$\mathcal {R}=0.79R_*$|⁠. In the dimensionless units used in the calculation, the pre-condensation magnetic energy |$\mathcal {E}_{\rm mag}^0=5.4937$|⁠.

Position of |$\mathcal {R}$|0.90.850.80.790.750.7
|$\mathcal {E}_{\rm mag}$| increase from field lines stretched towards equator0.53800.62670.72120.74110.82330.9271
|$\mathcal {E}_{\rm mag}$| increase from field lines stretched towards pole0.50290.54360.59300.60580.67040.7817
Position of |$\mathcal {R}$|0.90.850.80.790.750.7
|$\mathcal {E}_{\rm mag}$| increase from field lines stretched towards equator0.53800.62670.72120.74110.82330.9271
|$\mathcal {E}_{\rm mag}$| increase from field lines stretched towards pole0.50290.54360.59300.60580.67040.7817
Table 1.

Fractional increase in magnetic energy, |$\mathcal {E}_{\rm mag}^{\rm str}/\mathcal {E}_{\rm mag}^0$|⁠, as a function of position of superconducting shell |$\mathcal {R}$|⁠. We consider a plausible range of values of |$\mathcal {R}$| in increments of |$0.05R_*$|⁠, and also the ‘fiducial’ model with |$\mathcal {R}=0.79R_*$|⁠. In the dimensionless units used in the calculation, the pre-condensation magnetic energy |$\mathcal {E}_{\rm mag}^0=5.4937$|⁠.

Position of |$\mathcal {R}$|0.90.850.80.790.750.7
|$\mathcal {E}_{\rm mag}$| increase from field lines stretched towards equator0.53800.62670.72120.74110.82330.9271
|$\mathcal {E}_{\rm mag}$| increase from field lines stretched towards pole0.50290.54360.59300.60580.67040.7817
Position of |$\mathcal {R}$|0.90.850.80.790.750.7
|$\mathcal {E}_{\rm mag}$| increase from field lines stretched towards equator0.53800.62670.72120.74110.82330.9271
|$\mathcal {E}_{\rm mag}$| increase from field lines stretched towards pole0.50290.54360.59300.60580.67040.7817
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