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We study the unforced viscous Katz–Pavlović dyadic model with non-negative smooth initial data for two shell settings. For super-exponential scales , with and , we prove that is the sharp dissipation threshold: every such datum produces a globally smooth solution at and above this value, whereas suitable compactly supported data lose regularity in finite time below it. For geometric scales , global regularity holds when and . In particular, for , the result reaches and, together with the known classical blow-up theorem, identifies the sharp threshold in classical shell ratios.

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