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LeanPool.NavierStokesAndEuler.Euler.CompactProjectedEulerLaw

The Comparator solution satisfies the weak projected Euler equation #

The test family is the dense family of compact smooth solenoidal fields. Only pointwise identification of the supplied smooth fields with the Comparator velocity is assumed; no time regularity of those fields is used.

The Euler equation tested against compact vector fields #

Differentiation under the compact spatial integral uses joint smoothness on positive times. It does not assume an time derivative or any pressure decay.

Pressure cancellation against compactly supported solenoidal vector tests.

The scalar pressure needs only ordinary smoothness. In particular, neither the pressure nor its gradient is assumed to be globally square integrable.

Integration by parts with compact support on the vector test, rather than on the scalar potential.

An arbitrary smooth scalar pressure cancels against a compact smooth divergence-free vector test.

theorem Euler.EulerExistenceAndSmoothnessR3.velocity_test_pairing_hasDerivAt {u₀ : EuclideanSpace (Fin 3)EuclideanSpace (Fin 3)} {v : EuclideanSpace (Fin 3)EuclideanSpace (Fin 3)} {p : EuclideanSpace (Fin 3)} (h : EulerExistenceAndSmoothnessR3 u₀ v p) (φ : EuclideanSpace (Fin 3)EuclideanSpace (Fin 3)) ( : Continuous φ) (hφc : HasCompactSupport φ) (t₀ : ) (ht₀ : 0 < t₀) :
HasDerivAt (fun (t : ) => (x : EuclideanSpace (Fin 3)), inner (φ x) (v x t)) ( (x : EuclideanSpace (Fin 3)), inner (φ x) (-(fderiv (fun (x : EuclideanSpace (Fin 3)) => v x t₀) x) (v x t₀) - gradient (fun (x : EuclideanSpace (Fin 3)) => p x t₀) x)) t₀

The pointwise Euler equation differentiates every compactly supported continuous vector test pairing. Pressure is retained in this first identity.

theorem Euler.EulerExistenceAndSmoothnessR3.velocity_solenoidal_test_pairing_hasDerivAt {u₀ : EuclideanSpace (Fin 3)EuclideanSpace (Fin 3)} {v : EuclideanSpace (Fin 3)EuclideanSpace (Fin 3)} {p : EuclideanSpace (Fin 3)} (h : EulerExistenceAndSmoothnessR3 u₀ v p) (φ : EuclideanSpace (Fin 3)EuclideanSpace (Fin 3)) ( : ContDiff (↑) φ) (hφc : HasCompactSupport φ) (hdiv : ∀ (x : EulerSmoothLimit.Space), EulerSmoothLimit.divergence φ x = 0) (t₀ : ) (ht₀ : 0 < t₀) :
HasDerivAt (fun (t : ) => (x : EuclideanSpace (Fin 3)), inner (φ x) (v x t)) (- (x : EuclideanSpace (Fin 3)), inner (φ x) ((fderiv (fun (x : EuclideanSpace (Fin 3)) => v x t₀) x) (v x t₀))) t₀

Pressure disappears from the test-pairing derivative when the compact smooth vector test is divergence-free.

Replacing the Comparator velocity by any pointwise equal smooth representatives preserves the tested time equation, including its clamped interval parameterization. No time regularity of the representatives is assumed.

Compact smooth solenoidal tests determine ordinary L² solenoidal fields #

The curl-curl identity reduces the orthogonal complement of compact smooth curls inside the solenoidal space to globally weakly harmonic L² fields.

A distributionally harmonic vector field on all of ℝ³ vanishes if it lies in L².

Taking the L² class of a compact smooth curl is a linear operation.

Equations
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Instances For

    Compact smooth curls span the entire solenoidal Hilbert space densely.

    Linearity makes the closure of the generator set itself the full solenoidal space.

    Every member is represented by an actual compact smooth divergence-free field.

    A bundled compact smooth solenoidal test has the prescribed L² class.

    The compact test fields form a dense subset of the actual solenoidal L² space.

    Pairings against compact smooth solenoidal tests determine a solenoidal field.

    Pairing the projected Euler right-hand side #

    A solenoidal test field removes the Helmholtz projection from the Euler right-hand side. For a smooth divergence-free test field, this gives the ordinary spatial integral against advection. Compactly supported smooth tests automatically satisfy the required assumption.

    In particular, every compactly supported smooth divergence-free test has the projected Euler pairing required by the Comparator bridge.

    An arbitrary compact smooth solenoidal representative has the clamped weak projected derivative used by the Sobolev time-upgrade theorem.

    The exact weak projected derivative on the dense compact solenoidal test family. This is derived from the Comparator Euler equation itself.