PhysicsLogic / Prandtl 1904

Fixed Wall Data and a Singular Layer

Follow exact viscous balances without confusing residual control, outer recovery, and uniform convergence.

Definitions and assumptions

Scope and physical limitations

This independently constructed nondimensional periodic flow has an impermeable wall, the same oscillating wall velocity for every positive viscosity parameter, and a fluid at rest at infinity. It is not Prandtl's steady flat plate or separated wake, and not a fixed-initial-data inviscid-limit theorem.

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Examples and distinctions

Constructed examples of this model; each answer includes the Lean statement.

Exact root statement

(∀ (epsilon : ℝ),
    0 < epsilon →
      ∀ (time x y : ℝ),
        (layer epsilon).FullPlanarFlowAt time x y ∧ (layer epsilon).retainedTangentialResidual time x y = 0) ∧
  (∀ (epsilon time x : ℝ), (layer epsilon).tangential time x 0 = Real.cos time ∧ (layer epsilon).normal time x 0 = 0) ∧
    Filter.Tendsto (fun epsilon => (layer epsilon).viscosity) (nhdsWithin 0 (Set.Ioi 0)) (nhds 0) ∧
      (∀ (time y : ℝ),
          0 < y → Filter.Tendsto (fun epsilon => velocity epsilon time y) (nhdsWithin 0 (Set.Ioi 0)) (nhds 0)) ∧
        ¬TendstoUniformlyOn (fun epsilon y => velocity epsilon 1 y) (fun x => 0) (nhdsWithin 0 (Set.Ioi 0)) (Set.Ioi 0)
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Structures, classes, and inductive alternatives

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Constructors, projections, and other meaning dependencies

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