Solution
= Solution
Adding inward side flux and outward end-cap flux gives the net inward angular-momentum advection
$$
\mathcal A={8πρz_0ω_0ν^2\over α}[1-(1+s_0)e^{-s_0}],\qquad s_0={αr_0^2\over2ν}.
$$
It is positive because $e^{s_0}>1+s_0$, and tends to the stated value.