Figure 3
Change of volume-averaged magnetic energy in the r, θ and ϕ components of the magnetic field normalized to the initial magnetic energy in a shell from rout/40 to rout as a function of time in model H1. In this model, the magnetic field is amplified by the MRI. The growth of each component of the magnetic field is defined as δB2r,θ,ϕ = (〈B2r,θ,ϕ〉V−B2r,θ,ϕ,0), where 〈〉V denotes volume average and B0 is the initial field strength.

Change of volume-averaged magnetic energy in the r, θ and ϕ components of the magnetic field normalized to the initial magnetic energy in a shell from rout/40 to rout as a function of time in model H1. In this model, the magnetic field is amplified by the MRI. The growth of each component of the magnetic field is defined as δB2r,θ,ϕ = (〈B2r,θ,ϕVB2r,θ,ϕ,0), where 〈〉V denotes volume average and B0 is the initial field strength.

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