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Fig. 8.
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Time evolution for ωrms2/2 and vorticity growth terms for a non-isothermal rotating run with R = 0.5 and forcing in acceleration form. The notation is the same as in Fig. 7, and similarly 2ν⟨S∇lnρ ⋅ q⟩ and ⟨(j × b/ρ)⋅q⟩ overlap near 0, also making ⟨Fvisc ⋅ q⟩ overlap with ν⟨q2⟩.
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