“…Because the result in was the case ν , η > 0, κ = 0 and α = β = 1, g 1 ≡ g 2 ≡1, our result indicates that the powers of α may be shifted to γ and therefore represents a complete generalization in this sense. The proof of Theorem was inspired by the recent developments on the two‐dimensional generalized MHD system with β = 1, and in particular in which the authors showed that the two‐dimensional generalized MHD system with ν , η > 0, β = 1, α > 0, g 1 ≡ g 2 ≡1 admits the global regularity result. Therefore, Theorem also represents an extension of the result in to the magnetic Bénard problem, interestingly without requiring −Δ θ but only Λ 2 γ , γ = 1− α , α > 0. - The proof of Theorem was inspired by the recent work on the two‐dimensional generalized MHD system with ν = 0, and in particular in which the authors showed that the two‐dimensional generalized MHD system with ν = 0, η > 0, β > 1, g 2 ≡1 allows the global regularity result to hold.
…”