We investigated the and effects in a rotating spherical plasma system relevant to astrophysical environments. These coefficients were derived using three different approaches based on the large-scale magnetic field , turbulent velocity , and turbulent magnetic field , yielding , , , and . Using raw data from direct numerical simulations (DNS), we constructed the magnetic induction equation incorporating the and coefficients. We then reproduced the field and compared the results with the DNS data. In the kinematic regime, where is weak, all models exhibit good agreement with the DNS results. However, in the nonlinear regime, the field, reproduced using , deviates from the DNS and exhibits unbounded growth. To address this discrepancy, we added , which represents the contribution of turbulent magnetic fields, to . This addition suppresses the divergent growth of in the nonlinear regime. We then assessed the actual influence of and on the evolution of by applying weighted combinations of the two coefficients. Our results show that magnetic diffusion plays a dominant role throughout the entire process. In contrast, the effect is minor in the kinematic regime but becomes essential for sustaining the field in the nonlinear regime. We also discussed the underlying physical mechanism responsible for this behavior.

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