IOP PUBLISHING JOURNAL OF MICROMECHANICS AND MICROENGINEERING
J. Micromech. Microeng. 17 (2007) 1467–1478 doi:10.1088/0960-1317/17/8/008
In situ analysis of bacterial capture in a
microfluidic channel
Ashwin K Balasubramanian
1
, Ali Beskok
2
and Suresh D Pillai
3
1
Mechanical Engineering Department, Texas A&M University, College Station,
TX, USA
2
BioMicroFluidics Laboratory, Old Dominion University, Norfolk, VA, USA
3
Poultry Science Department, Texas A&M University, College Station, TX, USA
E-mail: abeskok@odu.edu
Received 7 March 2007, in final form 10 May 2007
Published 29 June 2007
Online at stacks.iop.org/JMM/17/1467
Abstract
We present a microfluidic approach for the continuous capture of Salmonella
Newport cells suspended in a phosphate buffer using externally applied
electric fields. The effects of flow rate, applied electric field and wall shear
stress on cell capture in the device are analyzed using particle tracking via
fluorescent microscopy techniques. Analyzing capture across multiple
locations on the electrode surface enabled the estimation of average capture
over the entire electrode area as a function of time. The device exhibits
approximately a constant capture rate over an extended time frame, which is
verified independently using the cell culture methods. An increased capture
rate with an increased electric field is observed. The capture rate dependence
on the flow rate and capture rate at various locations with different wall
shear stress magnitudes does not exhibit statistically significant variations.
The capture trends presented in this study can be utilized for designing
microfluidic systems for biosensors, designed bacterial bio-films and
devices for bacterial sample concentration from large volumes.
(Some figures in this article are in colour only in the electronic version)
Introduction
Microorganisms adversely impact man-made and natural
ecosystems by forming biofilms and bio-fouling [1–3]. Rapid
isolation and detection of bacterial cells are crucial in medical
diagnosis, water distribution lines, space exploration missions
and bioterrorism-related events. Initial attachment of bacterial
cells to the substrate is obviously the primary step in the
formation of biofilms. When bacterial cells are in close
proximity to a solid surface (<100 nm from surface), various
interaction processes including van der Waals interactions,
hydrophobic interactions and electrostatic interactions play an
important role in determining the adhesion process. However,
electrophoretic transport and electrostatic interactions between
charged surfaces play a vital role in attraction of bacterial cells
toward the surfaces, so that other interactions and adhesion
can occur. Systematic studies of capture and immobilization
of bacterial cells on a surface are essential to gain a better
understanding of bacterial attachment to charged substrates in
flow-based systems.
Several researchers have used flow-based systems to study
bacterial adhesion to surfaces in micro-scale devices. These
include parallel plate and stagnation point flow chambers,
rotating disk systems and cylindrical channels [4–9]. Design
of such systems requires careful consideration of the time
scales involved in fluid and particle motion. These systems
often neglect various electrochemistry effects that arise due
to the presence of electric fields. Quantification of adhesion
in these systems was primarily based on microscopy, which
requires an efficient particle tracking algorithm [10]. In situ
quantification methods are often more reliable than indirect
methods that involve removing the substrate from the flow
chamber, washing off cells that did not adhere to the electrode
and counting the captured cells under a microscope. One of
the main advantages of the in situ microscopy analysis is that
adhesion and desorption characteristics of cells can be studied
as a function of flow parameters in detail.
In this study, in situ quantification of microbial capture
was studied by applying pressure-driven flow in a parallel plate
microfluidic chamber with an external potential difference.
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