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Table 2.

Differential rotation parameters and the maximum meridional flow U ¯ mer max $ \overline{U}_{\mathrm{mer}}^{\mathrm{max}} $ from all the simulations.

Run ΔΩ(r) Δ Ω ( θ ¯ ) ( 60 ° ) $ \Delta_\Omega^{(\overline{\theta})}(60\circ) $ Δ Ω ( θ ¯ ) ( 75 ° ) $ \Delta_\Omega^{(\overline{\theta})}(75\circ) $ ΔΩCZ(r) Δ Ω CZ ( θ ¯ ) ( 60 ° ) $ \Delta_\Omega^{\mathrm{CZ}(\overline{\theta})}(60\circ) $ Δ Ω CZ ( θ ¯ ) ( 75 ° ) $ \Delta_\Omega^{\mathrm{CZ}(\overline{\theta})}(75\circ) $ U ¯ mer max [ m / s ] $ \overline{U}_{\mathrm{mer}}^{\mathrm{max}}~\mathrm{[m/s]} $
MHDr1 0.1579 −0.0001 −0.0011 0.3801 0.2650 0.4073 7.7
MHDr2 0.0505 −0.0001 −0.0006 0.1131 0.0699 0.1142 6.0
MHDr2*I 0.0405 −0.0001 −0.0007 0.0941 0.0607 0.0937 3.2
MHDr2*II 0.0538 −0.0000 −0.0006 0.1209 0.0734 0.1265 3.3
MHDr3 0.0251 −0.0000 −0.0004 0.0538 0.0295 0.0484 3.2
MHDr3* 0.0224 −0.0001 −0.0006 0.0489 0.0283 0.0438 2.1
MHDr4 0.0197 −0.0000 −0.0003 0.0405 0.0213 0.0350 2.5
MHDr4* 0.0169 −0.0001 −0.0006 0.0387 0.0208 0.0333 2.3

zMHDr1 0.3742 0.2442 0.3729 7.8
zMHDr2 0.1290 0.0739 0.1294 6.4
zMHDr3 0.0511 0.0282 0.0440 4.4
zMHDr4 0.0434 0.0214 0.0377 2.7

Notes. Run MHDr2* includes the parameters before (I) and after (II) the dynamo migration. The differential rotation parameters follow Eqs. (32) and (33).

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