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Figure 1:
Contours of
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Figure 2:
For r0=0.64, variations of parity ( top: solid for P1,
broken for P0) and modal energies ( bottom: E0 is upper long-dashed, E1is solid, E2 is lower long-dashed, E4 short-dashed) for
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Figure 3:
Snapshot of contours of surface field strength for
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Figure 4:
Snapshot of contours of surface field strength for
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Figure 5:
For r0=0.77, variations of parity ( top - solid for P1,
broken for P0) and modal energies ( bottom - E0 is upper long-dashed, E1is solid, E2 is lower long-dashed, E4 short-dashed) for
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Figure 6: Cross-sections of poloidal field lines for a) S1 field ("perpendicular dipole-like''); b) A1 field. The vertical line denotes the rotation axis. |
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Figure 7:
A sketch of superimposed magnetic fields of S0-type (solid) and S1-type
(broken). With the fields directed as indicated, the latitudinally
averaged field has a maximum at longitude ![]() ![]() |
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Figure 8:
Space-time diagram of longitudinally integrated surface field strength
for the solution with r0=0.64,
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Figure 9:
The longitude of maximum integrated squared surface field strength
as a function of time for the
N hemisphere, r0=0.64,
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Figure 10:
Space-time diagram of longitudinally integrated squared surface field strength
for the solution with r0=0.64,
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Figure 11:
Space-time diagrams of longitudinally integrated squared surface field strength for
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Figure 12:
The lower panel shows
the longitude of maximum squared surface field as a function of time for the
S hemisphere, r0=0.64,
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