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The Laminar-to-Turbulent-Detonation Transition: Hot Spots ... · P + ∇· ˆ τ =0, ∂E ∂t + ∇· ((E + P) U)+ ∇· (U · ˆ τ)+ ∇· (K ∇ T)=0, ∂ (ρY) ∂t + ∇· (ρY
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