An Alternative Technique for Dielectrophoretic (DEP) Cell Manipulation: Contact-Less DEP

Author(s):  
Hadi Shafiee ◽  
Michael B. Sano ◽  
John Caldwell ◽  
Rafael V. Davalos

Dielectrophoresis (DEP), the motion of a particle due to its polarization in the presence of a non-uniform electric field, can be used as an alternative to current sample enrichment techniques [1]. While the technique has been proven effective, most DEP devices must be manufactured using complicated processes. Insulator-based dielectrophoresis (iDEP) is a practical method to obtain the selectivity of dielectrophoresis while overcoming the robustness issues associated with traditional dielectrophoresis platforms [2]. While both of these methods allow for the differentiation of cells based upon their intrinsic electrical properties, they require direct contact between electrodes and a sample fluid, which can induce fouling, bubble formation and unwanted electrochemical effects [3]. We have developed an alternative method to provide the spatially non-uniform electric field required for DEP in which electrodes are not in direct contact with the biological sample. In this method, an electric field is created in the sample microchannel using electrodes inserted into two other microchannels (filled with conductive solution), which are separated from the sample microchannel by thin insulating barriers. These insulating barriers exhibit a capacitive behavior and therefore an electric field can be produced in the main channel by applying an AC field across them. The absence of contact between electrodes and the sample fluid inside the channel prevents bubble formation and avoids any contaminating effects the electrodes may have on the sample.

2020 ◽  
Vol 215 ◽  
pp. 115451 ◽  
Author(s):  
Wei Zhang ◽  
Junfeng Wang ◽  
Bin Li ◽  
Hailong Liu ◽  
Christian Mulbah ◽  
...  

Micromachines ◽  
2021 ◽  
Vol 12 (3) ◽  
pp. 340
Author(s):  
Lu Tian ◽  
Zi Ye ◽  
Lin Gui

This study presents a dielectrophoresis-based liquid metal (LM) droplet control microfluidic device. Six square liquid metal electrodes are fabricated beneath an LM droplet manipulation pool. By applying different voltages on the different electrodes, a non-uniform electric field is formed around the LM droplet, and charges are induced on the surface of the droplet accordingly, so that the droplet could be driven inside the electric field. With a voltage of ±1000 V applied on the electrodes, the LM droplets are driven with a velocity of 0.5 mm/s for the 2.0 mm diameter ones and 1.0 mm/s for the 1.0 mm diameter ones. The whole chip is made of PDMS, and microchannels are fabricated by laser ablation. In this device, the electrodes are not in direct contact with the working droplets; a thin PDMS film stays between the electrodes and the driven droplets, preventing Joule heat or bubble formation during the experiments. To enhance the flexibility of the chip design, a gallium-based alloy with melting point of 10.6 °C is used as electrode material in this device. This dielectrophoresis (DEP) device was able to successfully drive liquid metal droplets and is expected to be a flexible approach for liquid metal droplet control.


Author(s):  
Cila Herman ◽  
Shinan Chang ◽  
Estelle Iacona

The objective of the research is to investigate the behavior of individual air bubbles injected through an orifice into an electrically insulating liquid under the influence of a static electric field. Situations were considered with both uniform and nonuniform electric fields. Bubble formation and detachment were visualized in terrestrial gravity as well as for several levels of reduced gravity (lunar, martian and microgravity) using a high-speed video camera. Bubble volume, dimensions and contact angles at detachment were measured. In addition to the experimental studies, a simple model, predicting bubble characteristics at detachment in an initially uniform electric field was developed. The model, based on thermodynamic considerations, accounts for the level of gravity as well as the magnitude of the uniform electric field. The results of the study indicate that the level of gravity and the electric field magnitude significantly affect bubble behavior as well as shape, volume and dimensions.


Author(s):  
Johnson J. Wong ◽  
Emil Geiger

Through COMSOL modeling and electrode design, positive dielectrophoretic (pDEP) cell trapping for media exchange has been demonstrated on live Chlamydomnas reinhardtii in regular growth medium in a PDMS-glass microfluidic MEMS device. Dielectrophoresis (DEP) is the force applied to dielectric particles in an alternating current (AC) non-uniform electric field. A DEP force toward the increasing electric field gradient is called positive (pDEP). There are several published DEP structures for various applications such as: simple interdigitated structures for particle sorting in flow, DEP tweezers for single cell manipulation, and spiral structures for general cell manipulation. pDEP trapping over large areas (area pDEP) has been demonstrated with the use of low conductivity suspending media, but for higher conductivity suspending media, such as growth media, the pDEP force is reduced, and less likely to trap and hold microalgae against the hydrodynamic forces during media exchange. Multiphysics software, COMSOL, was used to model repeating structures suited for trapping of cells over the bottom area of a microfluidic device, which is useful and necessary for media exchange of a cell culture in a simple microfluidic device. The theoretical model of dielectrophoretic (DEP) force on a homogenous sphere in a homogenous medium in an electric field is a function of the sphere radius and conductivity, medium permittivity, and the gradient of the electric field. By assuming the conductivities, permittivities, and the particle geometry remains constant, the gradient of the electric field is the determining factor for the strength of the pDEP force. Modeling the electric fields and the resulting electric field gradient of various interdigitated electrode configurations allowed for the optimization of an electrode structure’s area of higher electric field gradients. The completed microfluidic device consisted of a single channel and a wide growth chamber overlaid over patterned gold-chrome electrodes. The MEMS device was fabricated using soft lithography and photolithography on the etched chrome-gold glass slides. The pDEP trapping was successful in trapping C. reinhardtii for media exchange. Media exchange allows for nutrient replenishment and waste removal, allowing for control of the growth conditions.


Author(s):  
Erin A. Henslee ◽  
Mike B. Sano ◽  
Eva M. Schmelz ◽  
Rafael V. Davalos

Dielectrophoresis (DEP) has become a promising technique to separate and identify cells and microparticles suspended in a medium based on their physical and electrical properties. DEP is the motion of a particle in a suspending medium due to the presence of a nonuniform electric field [1]. We have recently developed a robust, simple, and inexpensive technique, contactless dielectrophoresis (cDEP), to provide non uniform electric fields in microfluidic channels required for DEP cell manipulation without direct contact between the electrodes and the sample [2]. In this method, an electric field is created in the sample microchannel using electrodes inserted into two conductive microchambers, which are separated from the sample channel by thin insulating barriers. These insulating barriers exhibit a capacitive behaviour and therefore an electric field can be produced in the main channel by applying an AC field across the barriers [2]. The absence of contact between electrodes and the sample fluid inside the channel prevents bubble formation and avoids any contaminating effects the electrodes may have on the sample. Furthermore, reduced joule heating and a simplified inexpensive fabrication process are the other noticeable advantages of this new technique.


1997 ◽  
Vol 117 (11) ◽  
pp. 1109-1114
Author(s):  
Yoshiyuki Suda ◽  
Kenji Mutoh ◽  
Yosuke Sakai ◽  
Kiyotaka Matsuura ◽  
Norio Homma

2008 ◽  
Vol 128 (12) ◽  
pp. 1445-1451
Author(s):  
Takanori Yasuoka ◽  
Tomohiro Kato ◽  
Katsumi Kato ◽  
Hitoshi Okubo

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