In plasma separation by membrane, the blood flows tangentially along a
microporous membrane while the plasma crosses the membrane under the
action of a transmembrane pressure gradient. As in other cross flow fi
ltrations of suspensions, the permeate flux increases linearly at low
transmembrane pressure and reaches a plateau at high transmembrane pre
ssure due to concentration polarization and membrane fouling. Concentr
ation polarization consists in the formation of a high particle concen
tration boundary layer near the membrane which is assumed to occur rap
idly, in less than one minute. In the case of plasma filtration from b
lood, this layer consists of cells which are rejected by the membrane
and it forms a reversible secondary membrane which becomes the limitin
g filtration mechanism. In this condition, the permeate flux becomes a
pproximately independent of transmembrane pressure and is controlled m
ostly by the shear rate. In order to study the kinetics and time scale
s of establishment of these phenomena, we have investigated the transi
ent response of microporous membrane under stepped charges in transmem
brane pressure. When the pressure is suddenly raised from the unpolari
zed regime to a level corresponding to complete concentration polariza
tion, the permeate flux reaches a peak in 0.4-0.6 s, which supasses th
e equilibrium level by 60 to 80% depending upon the pressure, returnin
g to the concentration polarization equilibrium level in 3 to 4 s. The
se data show that the membrane retains its original permeability only
during the first 0.5 s of the pressure change and that concentration p
olarization takes about 3 to 4 s to build-up. This formation time decr
eases with increasing pressure. When the pressure returns to its initi
al level, the concentration polarization disappears instantaneously an
d the process can be repeated at a frequency up to 0.7 Hz. However, wh
en a stepped pressure increase is applied in the concentration polariz
ation regime, with initial pressure above 150 mmHg, the permeate flux
hardly changes, which confirms that once concentration polarization is
established, the system membrane-polarization layer ceases to behave
as a porous medium even with increased resistance. These data can expl
ain the permeate increase observed when pressure and flow pulsations a
t 1 Hz are superimposed on the retentate.