The first mathematically rigorous equilibrium statistical theory for three-
dimensional vortex filaments is developed here in the context of the simpli
fied asymptotic equations for nearly parallel vortex filaments, which have
been derived recently by Klein, Majda, and Damodaran. These simplified equa
tions arise from a systematic asymptotic expansion of the Navier-Stokes equ
ation and involve the motion of families of curves, representing the vortex
filaments, under linearized self-induction and mutual potential vortex int
eraction. We consider here the equilibrium statistical mechanics of arbitra
rily large numbers of nearly parallel filaments with equal circulations. Fi
rst, the equilibrium Gibbs ensemble is written down exactly through functio
n space integrals; then a suitably scaled mean held statistical theory is d
eveloped in the limit of infinitely many interacting filaments. The mean fi
eld equations involve a novel Hartree-like problem with a two-body logarith
mic interaction potential and an inverse temperature given by the normalize
d length of the filaments. We analyze the mean field problem and show vario
us equivalent variational formulations of it. The mean field statistical th
eory for nearly parallel vortex filaments is compared and contrasted with t
he well-known mean field statistical theory for two-dimensional point vorti
ces. The main ideas are first introduced through heuristic reasoning and th
en are confirmed by a mathematically rigorous analysis. A potential applica
tion of this statistical theory to rapidly rotating convection in geophysic
al flows is also discussed briefly. (C) 2000 John Wiley & Sons, Inc.