Energy
generation through nanofluidics is a topic of great nanotechnological
relevance. Here, we conduct all-atom molecular dynamics (MD) simulations
of the transport of water and ions in a pressure-driven flow in nanochannels
grafted with charged polyelectrolyte (PE) brushes and discover the
possibility of simultaneous electrokinetic energy generation and flow
enhancement (henceforth denoted as the electroslippage effect). Such PE-brush-functionalized nanochannels have been recently shown
to demonstrate an overscreening (OS) effect (characterized by the
presence of a greater number of screening counterions within the PE
brush layer than needed to screen the PE brush charges), a consequent
presence of excess co-ions within the PE brush-free bulk, and a co-ion-driven
electroosmotic (EOS) transport in the presence of small to moderate
applied axial electric fields. In this study, however, we find that
the streaming current, which represents the current generated by the
flow-driven downstream advection of the charge imbalance present within
the electric double layer (EDL) that screens the PE brush charges,
is governed by the migration of the counterions. This stems from the
fact that the highest contribution to the overall streaming current
arises from the region near the PE brush–water interface (where
there is an excess of counterions), while the brush-free bulk yields
a hitherto unreported, but small, co-ion-dictated streaming current.
This downstream advection of the charge imbalance (and the resultant
counterion-driven streaming current) eventually leads to the development
of an electric field (streaming electric field) in the direction that
is opposite the direction of the counterion-driven streaming current.
The streaming current and the streaming electric field interact to
generate the electrokinetic energy. Equally important, this streaming
electric field induces an EOS transport, which becomes co-ion-driven,
due to the presence of excess co-ions in the brush-free bulk. For
the case of nanochannels grafted with negatively charged PE brushes,
the streaming electric field will be in a direction that is opposite
that of the pressure-driven transport, and hence the co-ion (or anion)
driven EOS flow will be in the same direction as the pressure-driven
transport. On the other hand, for the case of nanochannels grafted
with positively charged PE brushes, the streaming electric field will
be in the same direction as the pressure-driven flow, and hence the
co-ion (or cation) driven EOS flow, will again be in the same direction
as the pressure-driven flow. Therefore, whenever there occurs a presence
of the OS and the resulting co-ion-driven EOS transport in PE brush
grafted nanochannels, regardless of the sign of the charges of the
PE brushes, this EOS transport will always aid the
pressure-driven transport and will cause the most fascinating increase
in the net volume flow rate across the nanochannel cross section,
which is the electroslippage effect.