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LeanPool.NavierStokesAndEuler.Euler.SmoothFieldSobolevTime

Pointwise evolution of smooth L² fields upgrades to genuine strong Sobolev evolution when all spatial L² jets of the field and its prescribed time derivative are continuous. The ordinary field is represented by its isometric, angle-independent lift to the unit cylinder.

Sobolev path, given by ⟨fun t => ordinarySobolev q (A t).toLp (A t).translation_contDiff,continuous_sobolev A hA q⟩.

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    theorem EulerSmoothFieldSobolevTime.sobolevPath_hasDerivWithinAt_of_three_le (T : ) (hT : 0 T) (A B : (Set.Icc 0 T)EulerLpTranslation.SmoothL2Field EulerSmoothLimit.Space) (hA : ∀ (n : ), Continuous fun (t : (Set.Icc 0 T)) => (A t).jetLp n) (hB : ∀ (n : ), Continuous fun (t : (Set.Icc 0 T)) => (B t).jetLp n) (hd : ∀ (t : ) (ht : t Set.Ioo 0 T) (x : EulerSmoothLimit.Space), HasDerivAt (fun (r : ) => (A (Set.projIcc 0 T hT r)).field x) ((B t, ).field x) t) (q : ) (hq : 3 q) (t : (Set.Icc 0 T)) :
    theorem EulerSmoothFieldSobolevTime.sobolevPath_hasDerivWithinAt (T : ) (hT : 0 T) (A B : (Set.Icc 0 T)EulerLpTranslation.SmoothL2Field EulerSmoothLimit.Space) (hA : ∀ (n : ), Continuous fun (t : (Set.Icc 0 T)) => (A t).jetLp n) (hB : ∀ (n : ), Continuous fun (t : (Set.Icc 0 T)) => (B t).jetLp n) (hd : ∀ (t : ) (ht : t Set.Ioo 0 T) (x : EulerSmoothLimit.Space), HasDerivAt (fun (r : ) => (A (Set.projIcc 0 T hT r)).field x) ((B t, ).field x) t) (q : ) (t : (Set.Icc 0 T)) :
    theorem EulerSmoothFieldSobolevTime.sobolevPath_hasDerivAt (T : ) (hT : 0 T) (A B : (Set.Icc 0 T)EulerLpTranslation.SmoothL2Field EulerSmoothLimit.Space) (hA : ∀ (n : ), Continuous fun (t : (Set.Icc 0 T)) => (A t).jetLp n) (hB : ∀ (n : ), Continuous fun (t : (Set.Icc 0 T)) => (B t).jetLp n) (hd : ∀ (t : ) (ht : t Set.Ioo 0 T) (x : EulerSmoothLimit.Space), HasDerivAt (fun (r : ) => (A (Set.projIcc 0 T hT r)).field x) ((B t, ).field x) t) (q : ) (t : ) (ht : t Set.Ioo 0 T) :