import OAI.MathematicalPhysics.NavierStokes.ForcedComputation.Programs.BalancedLoader import OAI.MathematicalPhysics.NavierStokes.ForcedComputation.Programs.StartupEffective import OAI.MathematicalPhysics.NavierStokes.ForcedComputation.Flow.CompactEuclideanEnergy namespace OAI /-! The compact Euclidean velocity is the input loader followed by the machine-only periodic processor. Its full Navier--Stokes residual is affine in viscosity and has the same fixed compact spatial support. -/ noncomputable section namespace ForcedComputation.BalancedVelocity open ShearFlows Set Filter open scoped ContDiff Topology BigOperators def velocity (I : Alternating.MachineInput) (hI : Alternating.ValidInput I) : Velocity := BalancedLoader.velocity (BalancedPlanar.inputCode I hI) + BalancedBody.activated I.1 hI.1 def support : Set Space := BalancedLoader.support ∪ BalancedBody.support theorem support_compact : IsCompact support := BalancedLoader.support_compact.union BalancedBody.support_compact theorem smooth (I : Alternating.MachineInput) (hI : Alternating.ValidInput I) : ContDiff ℝ ∞ (velocity I hI) := (BalancedLoader.velocity_smooth _).add (BalancedBody.activated_smooth _ _) theorem supported (I : Alternating.MachineInput) (hI : Alternating.ValidInput I) (t : ℝ) : tsupport (fun x => velocity I hI (t, x)) ⊆ support := by change tsupport ((fun x => BalancedLoader.velocity (BalancedPlanar.inputCode I hI) (t,x)) + (fun x => BalancedBody.activated I.1 hI.1 (t,x))) ⊆ support exact (tsupport_add _ _).trans (union_subset_union (BalancedLoader.velocity_support _ t) (BalancedBody.activated_support _ _ t)) theorem before (I : Alternating.MachineInput) (hI : Alternating.ValidInput I) {t : ℝ} (ht : t ≤ 1) (x : Space) : velocity I hI (t, x) = BalancedLoader.velocity (BalancedPlanar.inputCode I hI) (t, x) := by simp only [velocity, Pi.add_apply, BalancedBody.activated_before _ _ ht, add_zero] theorem tail (I : Alternating.MachineInput) (hI : Alternating.ValidInput I) {t : ℝ} (ht : 1 ≤ t) (x : Space) : velocity I hI (t, x) = BalancedBody.velocity I.1 hI.1 (t, x) := by simp only [velocity, Pi.add_apply, BalancedBody.activated_tail _ _ ht, BalancedLoader.velocity_after _ (show (1 : ℝ) / 4 ≤ t by linarith), zero_add] theorem zero_before (I : Alternating.MachineInput) (hI : Alternating.ValidInput I) {t : ℝ} (ht : t ≤ 1 / 8) (x : Space) : velocity I hI (t, x) = 0 := by rw [before I hI (by linarith), BalancedLoader.velocity_before _ ht] theorem solenoidal (I : Alternating.MachineInput) (hI : Alternating.ValidInput I) : Solenoidal (velocity I hI) := by intro t x have hL : ContDiff ℝ ∞ (fun z : Space => BalancedLoader.velocity (BalancedPlanar.inputCode I hI) (t,z)) := (BalancedLoader.velocity_smooth (BalancedPlanar.inputCode I hI)).comp (contDiff_const.prodMk contDiff_id) have hB : ContDiff ℝ ∞ (fun z : Space => BalancedBody.activated I.1 hI.1 (t,z)) := (BalancedBody.activated_smooth I.1 hI.1).comp (contDiff_const.prodMk contDiff_id) unfold divergence derivative change (∑ j, (fderiv ℝ ((fun z => BalancedLoader.velocity (BalancedPlanar.inputCode I hI) (t,z)) + (fun z => BalancedBody.activated I.1 hI.1 (t,z))) x) (basis j) j) = 0 rw [fderiv_add (hL.differentiable (by simp) x) (hB.differentiable (by simp) x)] simp only [add_apply, Pi.add_apply, Finset.sum_add_distrib] change divergence (fun z => BalancedLoader.velocity (BalancedPlanar.inputCode I hI) (t,z)) x + divergence (fun z => BalancedBody.activation I.1 hI.1 t • BalancedBody.velocity I.1 hI.1 (t,z)) x = 0 rw [BalancedLoader.velocity_divergence, divergence_smul, BalancedBody.velocity_divergence, mul_zero, add_zero] theorem bounded (I : Alternating.MachineInput) (hI : Alternating.ValidInput I) : BoundedMixedDerivatives (velocity I hI) := boundedMixed_of_compact_tail (smooth I hI) (BalancedBody.velocity_smooth _ _) support_compact (supported I hI) (fun t => (BalancedBody.velocity_support _ _ t).trans subset_union_right) (BalancedBody.velocity_periodic _ _) (fun _ ht x => zero_before I hI (by linarith) x) (fun _ ht x => tail I hI ht.le x) private theorem residual_zero (ν : ℝ) : residual ν (fun _ : SpaceTime => (0 : Space)) = 0 := by have hd : derivative (fun _ : Space => (0 : Space)) = fun _ _ => 0 := by funext j x simp [derivative] have hl (x : Space) : laplacian (fun _ : Space => (0 : Space)) x = 0 := by simp only [laplacian, hd] apply Finset.sum_eq_zero intro j _ rw [fderiv_const_apply] rfl funext y simp [residual, timeDerivative, advection, hl] private theorem residual_supported {V : Velocity} {K : Set Space} (hK : IsClosed K) (hs : ∀ t, tsupport (fun x => V (t,x)) ⊆ K) (ν t : ℝ) : tsupport (fun x => residual ν V (t,x)) ⊆ K := by apply closure_minimal _ hK intro x hx by_contra hn have ho : {y : SpaceTime | y.2 ∉ K} ∈ 𝓝 (t,x) := (hK.isOpen_compl.preimage continuous_snd).mem_nhds hn have he : V =ᶠ[𝓝 (t,x)] fun _ => 0 := by filter_upwards [ho] with y hy exact image_eq_zero_of_notMem_tsupport (f := fun x : Space => V (y.1,x)) (fun hm => hy (hs y.1 hm)) apply hx change residual ν V (t,x) = 0 rw [residual_congr_germ he ν, residual_zero] rfl theorem residual_periodic {V : Velocity} (hV : ContDiff ℝ ∞ V) (hp : TimePeriodic V) (ν : ℝ) : TimePeriodic (residual ν V) := by intro t x rw [residual_eq_force_add, Pi.add_apply, force_time_periodic hV hp] congr 1 simp only [convectiveField_eq_mixed hV] apply Finset.sum_congr rfl intro j _ rw [hp t x, mixedDerivative_time_periodic hV hp [j.succ] t x] theorem force_supported (I : Alternating.MachineInput) (hI : Alternating.ValidInput I) (ν t : ℝ) : tsupport (fun x => residual ν (velocity I hI) (t,x)) ⊆ support := residual_supported support_compact.isClosed (supported I hI) ν t theorem force_bounded (I : Alternating.MachineInput) (hI : Alternating.ValidInput I) (ν : ℝ) : BoundedMixedDerivatives (residual ν (velocity I hI)) := by apply boundedMixed_of_compact_tail (residual_smooth (smooth I hI) ν) (residual_smooth (BalancedBody.velocity_smooth _ _) ν) support_compact (force_supported I hI ν) (residual_supported support_compact.isClosed (fun t => (BalancedBody.velocity_support _ _ t).trans subset_union_right) ν) (residual_periodic (BalancedBody.velocity_smooth _ _) (BalancedBody.velocity_periodic _ _) ν) · intro t ht x have he : velocity I hI =ᶠ[𝓝 (t,x)] fun _ => 0 := by filter_upwards [(continuous_fst.tendsto (t,x)).eventually (eventually_lt_nhds ht)] with y hy exact zero_before I hI (by linarith) y.2 rw [residual_congr_germ he ν, residual_zero] rfl · intro t ht x apply residual_congr_germ filter_upwards [(continuous_fst.tendsto (t,x)).eventually (eventually_gt_nhds ht)] with y hy exact tail I hI hy.le y.2 def force₀ (I : Alternating.MachineInput) (hI : Alternating.ValidInput I) : Velocity := residual 0 (velocity I hI) def force₁ (I : Alternating.MachineInput) (hI : Alternating.ValidInput I) : Velocity := fun y => -laplacian (fun x => velocity I hI (y.1,x)) y.2 theorem force_affine (I : Alternating.MachineInput) (hI : Alternating.ValidInput I) (ν : ℝ) : residual ν (velocity I hI) = force₀ I hI + ν • force₁ I hI := by funext y simp only [residual, force₀, force₁, Pi.add_apply, Pi.smul_apply, zero_smul, sub_zero, smul_neg] rfl end ForcedComputation.BalancedVelocity end end OAI