Ordinary spatial covariance of the mean Gram inverse #
These identities act at one actual time slice in ordinary solenoidal L². They identify the continuous acceleration family with translation of the original acceleration, including endpoint time values.
theorem
EulerMeanPointwiseGramTranslation.frameAdjoint_translation
(a : EulerSmoothLimit.Space)
(F : ↥EulerMeanSolenoidal.L2 →L[ℝ] ↥EulerMeanSolenoidal.L2)
(f : ↥EulerMeanSolenoidal.L2)
:
(ContinuousLinearMap.adjoint
(EulerMeanOperatorTranslation.translateOperator a F ∘SL EulerMeanSolenoidal.solenoidalSpace.subtypeL))
((EulerMeanSolenoidal.translation a) f) = (EulerMeanTimeTranslation.solenoidalTranslation a)
((ContinuousLinearMap.adjoint (F ∘SL EulerMeanSolenoidal.solenoidalSpace.subtypeL)) f)
theorem
EulerMeanPointwiseGramTranslation.gram_translation
(a : EulerSmoothLimit.Space)
(F : ↥EulerMeanSolenoidal.L2 →L[ℝ] ↥EulerMeanSolenoidal.L2)
(v : ↥EulerMeanSolenoidal.solenoidalSpace)
:
(EulerTransverseGramInverse.gram
(EulerMeanOperatorTranslation.translateOperator a F ∘SL EulerMeanSolenoidal.solenoidalSpace.subtypeL))
((EulerMeanTimeTranslation.solenoidalTranslation a) v) = (EulerMeanTimeTranslation.solenoidalTranslation a)
((EulerTransverseGramInverse.gram (F ∘SL EulerMeanSolenoidal.solenoidalSpace.subtypeL)) v)
theorem
EulerMeanPointwiseGramTranslation.translated_lower
(a : EulerSmoothLimit.Space)
(F : ↥EulerMeanSolenoidal.L2 →L[ℝ] ↥EulerMeanSolenoidal.L2)
(c : ℝ)
(hF :
∀ (v : ↥EulerMeanSolenoidal.solenoidalSpace),
c * ‖v‖ ^ 2 ≤ ‖(F ∘SL EulerMeanSolenoidal.solenoidalSpace.subtypeL) v‖ ^ 2)
(v : ↥EulerMeanSolenoidal.solenoidalSpace)
:
theorem
EulerMeanPointwiseGramTranslation.gramInverse_translation
(a : EulerSmoothLimit.Space)
(F : ↥EulerMeanSolenoidal.L2 →L[ℝ] ↥EulerMeanSolenoidal.L2)
(c : ℝ)
(hc : 0 < c)
(hF :
∀ (v : ↥EulerMeanSolenoidal.solenoidalSpace),
c * ‖v‖ ^ 2 ≤ ‖(F ∘SL EulerMeanSolenoidal.solenoidalSpace.subtypeL) v‖ ^ 2)
(g : ↥EulerMeanSolenoidal.solenoidalSpace)
:
(EulerTransverseGramInverse.gramInverse
(EulerMeanOperatorTranslation.translateOperator a F ∘SL EulerMeanSolenoidal.solenoidalSpace.subtypeL) c hc ⋯)
((EulerMeanTimeTranslation.solenoidalTranslation a) g) = (EulerMeanTimeTranslation.solenoidalTranslation a)
((EulerTransverseGramInverse.gramInverse (F ∘SL EulerMeanSolenoidal.solenoidalSpace.subtypeL) c hc hF) g)
noncomputable def
EulerMeanPointwiseGramTranslation.acceleration
(F F₁ : ↥EulerMeanSolenoidal.L2 →L[ℝ] ↥EulerMeanSolenoidal.L2)
(c : ℝ)
(hc : 0 < c)
(hF :
∀ (v : ↥EulerMeanSolenoidal.solenoidalSpace),
c * ‖v‖ ^ 2 ≤ ‖(F ∘SL EulerMeanSolenoidal.solenoidalSpace.subtypeL) v‖ ^ 2)
(v : ↥EulerMeanSolenoidal.solenoidalSpace)
(f : ↥EulerMeanSolenoidal.L2)
:
The actual one-time acceleration operator from the strong mean equation.
Equations
- One or more equations did not get rendered due to their size.
Instances For
theorem
EulerMeanPointwiseGramTranslation.acceleration_translation
(a : EulerSmoothLimit.Space)
(F F₁ : ↥EulerMeanSolenoidal.L2 →L[ℝ] ↥EulerMeanSolenoidal.L2)
(c : ℝ)
(hc : 0 < c)
(hF :
∀ (v : ↥EulerMeanSolenoidal.solenoidalSpace),
c * ‖v‖ ^ 2 ≤ ‖(F ∘SL EulerMeanSolenoidal.solenoidalSpace.subtypeL) v‖ ^ 2)
(v : ↥EulerMeanSolenoidal.solenoidalSpace)
(f : ↥EulerMeanSolenoidal.L2)
:
acceleration (EulerMeanOperatorTranslation.translateOperator a F) (EulerMeanOperatorTranslation.translateOperator a F₁)
c hc ⋯ ((EulerMeanTimeTranslation.solenoidalTranslation a) v) ((EulerMeanSolenoidal.translation a) f) = (EulerMeanTimeTranslation.solenoidalTranslation a) (acceleration F F₁ c hc hF v f)
Simultaneously translating all data gives the actual translated acceleration.