The endpoint argument on the meridional half-plane #
Let V W : ℝ × ℝ → ℝ be the radial and axial components of a divergence-free axisymmetric
meridional field on the closed half-plane {R ≥ 0}, of class C¹ on the open half-plane
{R > 0} and with V bounded there. Assume the two structural identities
Then V vanishes identically and both ∂_R V and ∂_Z W vanish identically. The three steps
are the three theorems endpoint_axial_const, endpoint_radial_eq and
endpoint_dz_axial_eq_zero:
∂_R W = 0on the connected half-line{R > 0}makesW (R, Z)independent ofR, hence∂_Z W (R, Z) = ∂_Z W (1, Z)is a functionc ZofZalone;- the divergence identity then reads
∂_R (R V) = −R · c Z, soR V (R, Z) + (R² / 2) · c Zis constant inR; boundedness ofVforces that constant to be0, i.e.V (R, Z) = −(R / 2) · c Z; - boundedness of
Von the whole half-line now forcesc Z = 0, byeq_zero_of_abs_mul_le_of_nonneg.
Derivatives are taken in the form produced by CIV.exists_subseq_tendstoUniformlyOn_c1: a
Fréchet derivative DV p : (ℝ × ℝ) →L[ℝ] ℝ at p : ℝ × ℝ, whose radial and axial partial
derivatives are DV p (1, 0) and DV p (0, 1).
The second half of the file transfers the conclusion to a C¹-convergent sequence: if
DV n → DV⁰ uniformly on a set on which the limiting radial derivative vanishes, then
∂_R V n → 0 uniformly there, and the radial quotients V n / R converge to 0 uniformly on
a segment [0, A] × {Z} of the closed half-plane, by the mean value theorem applied to
R ↦ V n (R, Z) on [0, R].
Elementary one-variable input #
Reading partial derivatives off a Fréchet derivative #
Step (a): the axial component does not depend on the radius #
If ∂_R W = 0 on the open half-plane, then ∂_Z W (R, Z) = ∂_Z W (1, Z) for every
R > 0: the axial derivative of W is a function of Z alone.
Step (b): the radial component is linear in the radius #
The divergence identity integrates from the axis: with c Z := ∂_Z W (1, Z) one has
V (R, Z) = −(R / 2) · c Z for every R > 0. The integration constant is killed by the
boundedness of V, which makes R · V (R, Z) tend to 0 as R → 0⁺.
Step (c): boundedness forces the endpoint field to vanish #
Boundedness of V on the whole half-plane forces the Z-derivative of W to vanish.
The radial component of the endpoint field vanishes on the open half-plane.
The axial derivative of the axial component vanishes on the open half-plane.
The radial derivative of the radial component vanishes on the open half-plane.
The full Fréchet derivative of the radial component vanishes on the open half-plane:
V is identically zero on the open set {R > 0}.
The endpoint conclusion, packaged: on the open half-plane the radial component, its radial derivative, and the axial derivative of the axial component all vanish.
Transfer to a C¹-convergent sequence #
Uniform convergence of continuous linear maps passes to their values at a fixed vector.
If the limiting derivative annihilates v on S, the values at v converge uniformly
to 0 on S.
A continuous function on [0, A] vanishing on (0, A] vanishes on all of [0, A]: the
value at the axis is recovered as a limit along A / (n + 1).
Uniform convergence of the radial quotients V n / R to 0 on the segment
[0, A] × {Z} of the closed half-plane. Each quotient is a value of the radial derivative at
an intermediate radius, by the mean value theorem applied to r ↦ V n (r, Z) on [0, R]; the
axis value R = 0 is covered because V n (0, Z) = 0.
The endpoint conclusion of Step 2 in uniform form on the segment [0, A] × {Z} of the
closed half-plane: along a sequence converging to the endpoint field in C¹, the radial
derivative of the radial component, the axial derivative of the axial component, and the
radial quotients all converge to 0 uniformly.