The inviscid limit of vorticity in steady Navier-Stokes flows in two d
imensions containing regions of closed streamlines (eddies) is studied
. Prandtl [International Mathematical Congress, Heidelberg, Teubner, L
eipzig, 1904, pp. 484-491; see also Gesammelte Abhandlungen zur angewa
ndten Mechanik, Hydro- und Aerodynamik, vol. 2, Springer-Verlag, Berli
n, 1961, pp. 575-584] and Batchelor [J. Fluid Mech., 1 (1956), pp. 177
-190] showed that, in the limit of large Reynolds number R, the vortic
ity in such a region becomes constant. For the circular domain, Batche
lor and Wood [J. Fluid Mech., 2 (1957), pp. 77-87] gave a formula whic
h computes the constant vorticity. To study the effect of finite Reyno
lds number R on this formula, a matched asymptotic expansion of the ve
locity in two parameters, epsilon (the perturbation parameter) and R,
is calculated up to order of O(epsilon(2) = root R) and compared with
the numerical results. For the resulting vorticity, including the corr
ection for finite R, omega(full), we obtain values in reasonably good
agreement with the numerical results.