Toward On-Chip Processes using Redox-
Magnetohydrodynamic Microfluidics without
Channels
Vishal Sahore, Christena K. Nash, Melissa C. Weston,
Matthew D. Gerner, and Ingrid Fritsch
University of Arkansas
Department of Chemistry and Biochemistry
Fayetteville, AR 72701
Controlling localized motion of small volumes of
fluid with redox-magnetohydrodynamics (redox-MHD)
will be discussed, with an emphasis on performing
multiple steps for chemical analysis processes on a chip.
Redox-MHD has the unique capability to do this without
the need for traditional channels that physically confine
and direct fluid flow on the small scale.
The phenomenon of MHD is well-known in fields
distant from electrochemistry. This includes plasma
physics and metallurgy, where a highly conductive fluid
(ionized gases and liquid metals, respectively) moving in
a magnetic field produces a current, which then further
affects the movement and shape of the fluid. The MHD
body force, F
B
, which determines the direction and
magnitude of the fluid flow, is best described through the
right-hand rule as the cross product of the charge or ion
flux, j, with the magnetic flux density, B: F
B
= j × B.
Liquid solutions (aqueous and non-aqueous), which
are much more resistive than ionized gases and liquid
metals, exhibit subtler MHD effects because of the lower
magnitude of j. The addition of a chemical (redox)
species to an electrolyte solution that can be easily
oxidized and reduced through electron transfer processes
at electrodes allows current to pass without electrode
dissolution and bubble formation from solvent
electrolysis, unlike in early attempts to use MHD as a
microfluidic pump.
1, 2
This redox-MHD approach has now
been explored for microfluidics on a chip.
3-5
Redox-MHD on a chip containing individually-
addressable microband electrodes in the presence of a
permanent magnet placed beneath the chip has
demonstrated several interesting microfluidic
capabilities.
4
Localized flow can be started, stopped, and
easily reversed simply by turning on, off, and reversing
the polarity of the electrodes, respectively. The fluid can
be pumped in separate or larger single loops depending on
the distance, size, and current at the electrodes.
Oppositely polarized electrodes reinforce the flow,
increasing the speed for the same given current. In
addition, a flat flow profile is achievable, which is of
great interest in performing efficient chemical
separations. The fluid speed for a given cell geometry is
proportional to the applied current, allowing fine-tuning
of flow simply by tuning the electrode current.
6
A concern about redox-MHD had been the presence
of high concentrations of redox species. Originally, such
high concentrations were thought necessary for the
solution to exhibit MHD in low B-fields generated by
small permanent magnets that would be of interested in
hand-held devices. This is because evidence of MHD
convection was often followed by measuring a change in
current under applied potential conditions,
7-10
thus
requiring high currents from large redox concentrations.
However, with the ability to monitor fluid flow by
tracking microbeads with video microscopy, redox
concentrations as low as 5 mM can be shown to be
enough to achieve sufficient speeds of 30 μm/s in the
small volumes on a chip.
11
This concentration does not
significantly affect the enzymatic reaction of alkaline
phosphatase (AP) with the substrate p-aminophenyl
phosphate (PAPP). This is important because AP is an
enzyme label used in enzyme-linked immunosorbant
assays (ELISAs), suggesting that redox-MHD should be
compatible with immunoassay analysis. The low redox
concentration allows for not only pumping, but also
simultaneous electrochemical detection of the species p-
aminophenol that is enzymatically generated from the
PAPP. This has been performed under circumstances
where a fluid segment or plug was directed to the
electrochemical detector with redox-MHD pumping
alone, without channel sidewalls. These outcomes suggest
that redox-MHD could be used to perform the
microfluidics in carrying out the multiple steps of an
ELISA on a chip and without the need for channels. A
chip without channels would be easier to fabricate and
could be reprogrammed for different applications, having
different microfluidic needs.
In our presentation, we will include new studies that
take these concepts to the next level. Extremely straight
fluid flow will be shown between microband electrodes
across much longer stretches, > 2 cm. Fluid manipulation
using other electrode geometries, including concentric
disk and ring electrodes, will illustrate different
approaches to stir and trap small segments of solution. We
will also provide updates on new strategies to insure
compatibility of the pumping method with the application.
We will discuss how these results can lead to the design
of chips based on the right-hand rule to achieve complete
analysis processes.
It is hoped that the high level of complexity of this
topic is well-suited for initiating the kind of intense
scientific discussions that W. Ves Childs would have
enjoyed. We present our research to honor his memory
and with thanks to him for stimulating intellectual
excitement on many other topics in the past.
ACKNOWLEDGMENTS
Research was supported through the National Science
Foundation (NSF) (CHE-0719097) and the Arkansas
Biosciences Institute.
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