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Bioelectric signals are important biophysical factors contributing to governing cell behavior. The most famous example is the action potential in neurons and heart cells, which transmit electrical signals over long distances (up to a meter) and at high frequencies (up to hundreds of Hertz)1. Electrical pulses applied with electrodes can be used to stimulate action potential firing and is useful in research and medical applications2. Endogenous bioelectric signals in slow physiological processes such as development, wound healing, and homeostasis3,4,5,6,7,8 have also been measured9,10 over periods of hours to days. An important example is confluent epithelial layers which actively maintain a transepithelial potential difference (TEPD) ranging from a few to tens of millivolts4,11. A cut or wound in these confluent layers generates a short-circuit current, driven by the electrical activity of the tissue12,13. Wound currents up to tens of µA/cm2 and electric fields up to hundreds of mV/mm have been reported with different techniques. Studies suggest that these electric signals produce a directional cue for cells to migrate toward wound or infection sites that is important for the healing process3,6,14. In general, both static (or slow-varying) and fast-varying electric signals are important and trigger different cell or tissue responses.
Within the realm of slow-varying signals, one important phenomenon is the electrically-driven migration process termed "galvanotaxis". Controlled in-plane galvanic currents can be applied in microfluidic devices with simple channels to mimic the wound currents while cell migration is investigated as a function of current density15,16. Electric fields of 0.1-1000 V/m (corresponding current density of 0.1-1000 A/m2) are found to drive cell migration in many cell types in this in vitro setting17, while signaling pathways canonical to chemotaxis (cell migration guided by chemical gradients), such as PI3K, have been implicated in galvanotaxis7,18. "Bare-bones" microfluidic devices for galvanotaxis study can be fabricated with standard soft lithography and microfabrication techniques19. These devices typically comprise a single-channel polydimethyl-siloxane (PDMS) substrate bonded to a glass slide (channel cross-sectional size: hundreds of micrometers, length: centimeters). Electrodes used to supply the static current are installed far away from the cell region, and connected with or without salt bridges. The salt bridge connection may be made by punched holes through the PDMS substrate, microfluidic connectors, and tubings filled with agar. The simple glass slide (typically 170 µm thick) beneath the channel also supports high-resolution live-cell imaging during the galvanotaxis experiments, which is a crucial feature for studying the process.
The role of endogenous electric signals in the maintenance of tissue homeostasis is much less understood than that in wound healing. One important reason is the lack of appropriate tools to study these effects in intact tissues. The microfluidic device for galvanotaxis is not suitable for this purpose due to its geometry, which only supports in-plane electric currents. In the context of epithelial homeostasis, a new device is needed to control and perturb the TEPD or out-of-plane currents across a confluent epithelial layer. To achieve the aim of applying a relatively uniform ion current density across a monolayer, we have designed and fabricated a microfluidic device with innovations in device geometry, material usage, and in situ biomechanical measurement capabilities4. The latter capability is important as electric effects may be affecting cell behavior through coupling with biomechanics and mechanobiology pathways, which can be studied with this feature.
This new device exhibits multiple innovative features. It is designed with two layers instead of the single channel found in the galvanotaxis devices (innovation in geometry), while keeping the connection to the electrode chambers similar to that in the latter. The first microfluidic layer has channels to direct ion currents to (or away from) the tissue region, while the second layer has an opening that will direct this current perpendicularly across the epithelium sitting on top of this second microfluidic layer (Figure 1A,B). Microfabrication techniques are used for producing sufficiently thin layers such that high-resolution confocal imaging is possible despite the stacking of microfluidic layers that increases sample thickness. For the other important innovations, a polyacrylamide (PA) synthetic hydrogel is incorporated into the middle of the device, which plays a crucial role (Figure 1A,B). The physico-chemical properties of this gel, such as available chemistry to coat extracellular matrix proteins, permeability to ions, as well as known elasticity, are respectively essential for cell attachment and growth, application of out-of-plane currents, and measurement of mechanical stress20 during electric stimulation. Barrier structures are incorporated in Layer 1 of the tissue region for confinement of the PA gel precursor solution, as done in previous microfluidic devices21 (Figure 1A,B). Last but not least, since PA gel polymerization is oxygen-inhibited at PDMS surfaces permeable to oxygen gas, another material22 is used for device fabrication, which can allow polymerization and tight bonding of PA gel. All the innovative features are crucial for the new device to work.
Overall, the in-depth study of static or slowly varying bioelectric signals in the homeostasis of intact tissues is made possible with this new device, the protocol for which will be detailed below. The protocol and results referred to here are focused on the Madin Darby Canine Kidney II (MDCK II) epithelial cell line, including the cell events (proliferation, death, and extrusion, and migration) and tissue structural changes that are induced by the electric current. These studies are also instructive for researchers who are interested in applying this technique to study the electrical regulation of epithelial transport and induction of cell events and cell fate changes in cell layers and more complex systems, such as primary cells and 2D organoids.