Figure 1
Evolution of the volume-averaged magnetic energy in both the r and ϕ components of the magnetic field normalized to the initial magnetic energy in a shell from rout/40 to rout in model L1. In this model, the magnetic field is amplified only by flux freezing. As vθ∼ 0, there is almost no amplification of the θ component of the field, so it is not shown. The growth of each component 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.

Evolution of the volume-averaged magnetic energy in both the r and ϕ components of the magnetic field normalized to the initial magnetic energy in a shell from rout/40 to rout in model L1. In this model, the magnetic field is amplified only by flux freezing. As vθ∼ 0, there is almost no amplification of the θ component of the field, so it is not shown. The growth of each component 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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