The one-dimensional hydrodynamic theory for superfluid turbulent flow
of He II developed recently by one of the authors is extended to the t
hree-dimensional case. The impulse density of the entangled mass of qu
antised vortices continues to play an important part in the analysis.
The non-dissipative equations of motion are derived from an appropriat
e form of Hamilton's variational principle, while the dissipative effe
cts are taken into account systematically according to the thermodynam
ics of irreversible processes. A number of helicity conservation theor
ems appears to be valid in the case of non-dissipative flow. Particula
r attention is paid to homogeneous superfluid turbulence. It turns out
that the two states allowed in one-dimensional homogeneous flow, viz.
the state in which the direction of the vortex tangle impulse is para
llel and the one in which it is anti-parallel to the counterflow veloc
ity, are, respectively, stable and metastable. The analysis might assi
st in clarifying the one-dimensional free decay of homogeneous superfl
uid turbulence.