Passing the finite-axis zoom sequence to its limit #
Elementary limit lemmas for eq:aniso:zoom:finite:limit, the equation obeyed by the locally
uniform limit Ω_∞ of the rescaled potential vorticities Ω_n of eq:aniso:zoom:fields, along a
sequence of zoom scales λ_n → 0⁺:
λ_n → 0⁺forcesδ_n = λ_n^{2h} → 0and, for any sequence uniformly bounded byM,δ_n² · (\text{that sequence}) → 0— the mechanism removingδ_n² ∂_{ZZ} Ω_nfrom the equation (tendsto_zoomDeltaSq_nhdsWithin_zero,tendsto_zoomDeltaSq_mul_of_bounded).- the force term
G_nofeq:interior:force:scaledtends to zero uniformly in the point along every scale sequence (eventually_forall_abs_zoomForce_lt), transporting the scale limittendsto_zoomForce_bound_nhdsWithin_zeroofCIV.Zoom.FiniteLiftalong an arbitraryλ_n → 0⁺. - the algebraic divergence identity
div_{X,Z} B_n = 2 V_n / RofCIV.Zoom.FiniteAxisBounds(zoomDriftDivergence_eq) holds for every finiten, so it passes to the limit onceV_n / Rdoes (tendsto_zoomDriftDivergence_of_tendsto_zoomV_div): this is the "With div_{X,Z} B = 2 V / R" clause ofeq:aniso:zoom:finite:limit. - the products
B_n Ω_nand(V_n/R) Ω_npass to the limit under an integral against a fixed test function by dominated convergence, given almost-everywhere convergence of the pointwise product and a uniform domination (tendsto_integral_mul_of_ae_tendsto).
The limit equation itself, CIV.IsDistributionalDriftDiffusion 5 4 (Set.Iio (-1)) B divB Ω_∞
with an admissible drift, is CIV.exists_admissibleDrift_zoomOmegaLimit.
δ_n → 0 removes the δ_n² ∂_{ZZ} Ω_n term #
δ = λ^{2h} → 0 as the zoom scale λ → 0⁺, for any positive anisotropy exponent h.
δ² = (λ^{2h})² → 0 as λ → 0⁺.
δ_n² · D_n → 0 whenever D_n is uniformly bounded and λ_n → 0⁺: the mechanism that
removes δ_n² ∂_{ZZ} Ω_n from eq:aniso:zoom:finite:equation in the limit, given the uniform
bound on ∂_{ZZ} Ω_n as an explicit hypothesis.
The force term G_n → 0 uniformly along a scale sequence #
The force term G_n = zoomForce of eq:interior:force:scaled tends to zero uniformly in
the point along every scale sequence λ_n → 0⁺: composing the scale limit
tendsto_zoomForce_bound_nhdsWithin_zero of CIV.Zoom.FiniteLift along λ_n with the
uniform-in-the-point bound abs_zoomForce_le (reproved directly from
abs_potentialVorticity_force_le so the same bounding constant is used at every n). This is
the "G_n → 0 uniformly" clause of eq:aniso:zoom:finite:limit.
The exact algebraic identity zoomDriftDivergence_eq of CIV.Zoom.FiniteAxisBounds,
div_{X,Z} B_n = 2 V_n / R, holds at every finite n, so it passes to the limit outright as
soon as V_n / R converges: the "With div_{X,Z} B = 2 V / R" clause of
eq:aniso:zoom:finite:limit, conditioned only on the convergence of V_n / R.
Passing a product of two convergent sequences to the limit under an integral #
The pointwise mechanism of "passing the products B_n Ω_n and (V_n/R) Ω_n to the limit":
if two sequences converge at a point, so does their product against a fixed third factor.
Passing the product Ω_n B_n to the limit inside a fixed integral against φ, by the
Lebesgue dominated convergence theorem: given almost-everywhere convergence of the pointwise
product and a uniform domination by M |φ|, the paired integrals converge. This is the
integral-level mechanism of "the weak-* convergence of B_n against the strong convergence of
Ω_n … passes the products B_n Ω_n and (V_n/R) Ω_n to the limit" of
eq:aniso:zoom:finite:limit.