Fig. 14.

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Components of the mass fluxes, Ṁ, in terms of the dependence of the anomalous resistive coefficient, αm, for different strengths of the stellar magnetic field in the cases with fastest stellar rotation in our simulations, Ω⋆ = 0.2Ωbr. The values of Ṁout and Ṁd are both computed at R = 12R⋆, where the flow is most stable. The latter is computed across the disk height, and corresponds to the total mass accretion rate available for distribution in the system. The component ṀSW at the same stellar rotation rate is shown together with corresponding torques in Fig. 9. Note: the y-label multiplication factor is given in the left upper corner of the panels.
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