  We study the phantom fluid in the late universe, thus assuming the equation
of state parameter $w$ to be less than $-1$. The fluid is assumed to consist of
two components, one laminar component $\rho$ and one turbulent component
$\rho_T$, the latter set proportional to $\rho$ as well as to the Hubble
parameter, $\rho_T =3\tau H\rho$ with $\tau$ a positive constant associated
with the turbulence. The effective energy density is taken to be $\rho_e= \rho
+ \rho_T$, and the corresponding effective pressure is $p_e=w \rho_e$, with $w$
constant. These basic assumptions lead to a Big Rip universe; the physical
quantities diverging during a finite rip time $t_s$. We then consider the mass
accretion of a black hole in such a universe. The most natural assumption of
setting the rate $dM/dt$ proportional to $M^2$ times the sum $\rho_e+p_e$,
leads to a negative mass accretion, where $M(t)$ goes to zero linearly in
$(t_s-t)$ near the singularity. The Hubble parameter diverges as
$(t_s-t)^{-1}$, whereas $\rho_e$ and $p_e$ diverge as $(t_s-t)^{-2}$. We also
discuss other options and include, for the sake of comparison, some essential
properties of mass accretion in the early (inflationary) universe.
