Uniform energy bounds for regularized solutions #
The energy equality in thm:regularised controls every time slice and the
full positive-time dissipation, uniformly in the regularization parameter.
The spatial L² field represented by a CKN vector-valued function.
Equations
- CKN.Leray.regUniformSpatialField f x = WithLp.toLp 2 (f x.ofLp)
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A time slice of the velocity, represented on the Euclidean spatial carrier.
Equations
- CKN.Leray.regUniformVelocitySlice u t x = WithLp.toLp 2 (u (x.ofLp, t))
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The mollified initial velocity as a pointwise CKN vector field.
Equations
- CKN.Leray.regUniformMollifiedInitial ρ ε hε a x = (CKN.Leray.regMollifyVector ρ ε hε (CKN.Leray.regUniformSpatialField a) (WithLp.toLp 2 x)).ofLp
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The regularized transport velocity J_ε u on positive-time slices.
Equations
- CKN.Leray.regUniformMollifiedVelocity ρ ε hε u z = (CKN.Leray.regMollifyVector ρ ε hε (CKN.Leray.regUniformVelocitySlice u z.2) (WithLp.toLp 2 z.1)).ofLp
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Lebesgue measure on all positive space-time, used for global energy bounds.
Equations
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Dissipation up to time T, measured on the positive-time carrier.
Equations
- One or more equations did not get rendered due to their size.
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The energy equality in thm:regularised implies the uniform slice-energy
bound and the full positive-time dissipation bound.
The regularized transport field has no larger slice L² norm than the
velocity, by the convolution contraction in lem:reg-mollifier-bounds.