Dielectrophoretic manipulation of cells with spiral electrodes.

Electrokinetic responses of human breast cancer MDA-MB-231 cells were studied in suspensions of conductivities 18, 56, and 160 mS/m on a microelectrode array consisting of four parallel spiral electrode elements energized with phase-quadrature signals of frequencies between 100 Hz and 100 MHz. At low frequencies cells were levitated and transported toward or away from the center of the spiral array, whereas at high frequencies cells were trapped at electrode edges. The frequencies of transition between these characteristic cell behaviors increased with increasing suspension conductivity. Levitation heights and radial velocities were determined simultaneously for individual cells as a function of the applied field magnitude and frequency. Results were compared with theoretical predictions from generalized dielectrophoresis theory applied in conjunction with cell dielectric parameters and simulated electric field distributions corrected for electrode polarization effects. It was shown that the conventional and traveling-wave dielectrophoretic force components dominated cell levitation and radial motion, respectively. Both theoretical predictions and experimental data showed that the cell radial velocity was very sensitive to the field frequency when the in-phase component of the field-induced polarization was close to zero. Applications of spiral electrode arrays, including the isolation of cells of clinical relevance, are discussed.     

Dielectric spectroscopy of single human erythrocytes at physiological ionic strength: dispersion of the cytoplasm.

Usually dielectrophoretic and electrorotation measurements are carried out at low ionic strength to reduce electrolysis and heat production. Such problems are minimized in microelectrode chambers. In a planar ultramicroelectrode chamber fabricated by semiconductor technology, we were able to measure the dielectric properties of human red blood cells in the frequency range from 2 kHz to 200 MHz up to physiological ion concentrations. At low ionic strength, red cells exhibit a typical electrorotation spectrum with an antifield rotation peak at low frequencies and a cofield rotation peak at higher ones. With increasing medium conductivity, both electrorotational peaks shift toward higher frequencies. The cofield peak becomes antifield for conductivities higher than 0.5 S/m. Because the polarizability of the external medium at these ionic strengths becomes similar to that of the cytoplasm, properties can be measured more sensitively. The critical dielectrophoretic frequencies were also determined. From our measurements, in the wide conductivity range from 2 mS/m to 1.5 S/m we propose a single-shell erythrocyte model. This pictures the cell as an oblate spheroid with a long semiaxis of 3.3 microns and an axial ratio of 1:2. Its membrane exhibits a capacitance of 0.997 x 10(-2) F/m2 and a specific conductance of 480 S/m2. The cytoplasmic parameters, a conductivity of 0.4 S/m at a dielectric constant of 212, disperse around 15 MHz to become 0.535 S/m and 50, respectively. We attribute this cytoplasmic dispersion to hemoglobin and cytoplasmic ion properties. In electrorotation measurements at about 60 MHz, an unexpectedly low rotation speed was observed. Around 180 MHz, the speed increased dramatically. By analysis of the electric chamber circuit properties, we were able to show that these effects are not due to cell polarization but are instead caused by a dramatic increase in the chamber field strength around 180 MHz. Although the chamber exhibits a resonance around 180 MHz, the harmonic content of the square-topped driving signals generates distortions of electrorotational spectra at far lower frequencies. Possible technological applications of chamber resonances are mentioned.     

Manipulation of herpes simplex virus type 1 by dielectrophoresis

The frequency-dependent dielectrophoretic behaviour of an enveloped mammalian virus, herpes simplex virus type 1 is described. It is demonstrated that over the range 10 kHz–20 MHz, these viral particles, when suspended in an aqueous medium of conductivity 5 mS m^?1, can be manipulated by both positive and negative dielectrophoresis using microfabricated electrode arrays. The observed transition from positive to negative dielectrophoresis at frequencies around 4.5 MHz is in qualitative agreement with a simple model of the virus as a conducting particle surrounded by an insulating membrane.     

Cell fission and formation of mini cell bodies by high frequency alternating electric field.

We report the use of high frequency alternating electric fields (AC) to induce deformation of sea urchin eggs, leading to budding of membrane vesicles or fission of cells. Several mini cell bodies can be prepared from a single egg by carefully manipulating the frequency and amplitude of the AC field and the ratio between the interelectrode spacing and the cell diameter, alpha. alpha values between 2.2 and 3.5 have been found to be optimal for inducing fission of sea urchin eggs. In a typical experiment, a sea urchin egg (diameter = 75 microns), suspended in a low ionic medium (conductance < 2 mS/m), was located under the microscope between two platinum wire electrodes, separated by a distance of approximately 200 microns. A medium strength AC field (< 100 V/cm at 2 MHz) was applied to attract the egg to one of the two electrodes via dielectrophoresis. This process took place in a few seconds. The voltage was then slowly increased to approximately 1000 V/cm over approximately 30 s. The cell elongated and separated into two fragments, the larger one containing the nucleus. When the field was turned off, the mother cell and the daughter vesicle retracted to form spherical mini cell bodies that appear to be stable as assessed by the absence of swelling for the duration of the experiment (approximately 15 min). This indicates that membranes of these mini cell bodies were not leaky to ions and small molecules. This procedure could be repeated a few times to make several mini cell bodies from a single egg.(ABSTRACT TRUNCATED AT 250 WORDS)     

Measurement of inherent particle properties by dynamic light scattering: introducing electrorotational light scattering.

Common dynamic light scattering (DLS) methods determine the size and zeta-potential of particles by analyzing the motion resulting from thermal noise or electrophoretic force. Dielectric particle spectroscopy by common microscopic electrorotation (ER) measures the frequency dependence of field-induced rotation of single particles to analyze their inherent dielectric structure. We propose a new technique, electrorotational light scattering (ERLS). It measures ER in a particle ensemble by a homodyne DLS setup. ER-induced particle rotation is extracted from the initial decorrelation of the intensity autocorrelation function (ACF) by a simple optical particle model. Human red blood cells were used as test particles, and changes of the characteristic frequency of membrane dispersion induced by the ionophore nystatin were monitored by ERLS. For untreated control cells, a rotation frequency of 2 s-1 was induced at the membrane peak frequency of 150 kHz and a field strength of 12 kV/m. This rotation led to a decorrelation of the ACF about 10 times steeper than that of the field free control. For deduction of ERLS frequency spectra, different criteria are discussed. Particle shape and additional field-induced motions like dielectrophoresis and particle-particle attraction do not significantly influence the criteria. For nystatin-treated cells, recalculation of dielectric cell properties revealed an ionophore-induced decrease in the internal conductivity. Although the absolute rotation speed and the rotation sense are not yet directly accessible, ERLS eliminates the tedious microscopic measurements. It offers computerized, statistically significant measurements of dielectric particle properties that are especially suitable for nonbiological applications, e.g., the study of colloidal particles.     

A chip for catching, separating, and transporting bio-particles with dielectrophoresis

This study aims at developing a 3D device for catching, separating, and transporting bio-particles based on dielectrophoresis (DEP). Target particles can be simultaneously caught and transported using the negative DEP method. In non-uniform electric fields, the levitation height or complex permittivity of certain particle may be different from that of another and this property can facilitate separation of particles. We have designed and constructed a 3D device consisting of two layers of electrodes separated by a channel formed by 50 μm thick photoresist. The electrodes can operate effectively with 10–15 V and 5–7 MHz to catch all particles in the channel, and can move particles after switching the electric field to 5–15 V and 500–1,000 KHz. Hence, particles experienced coupling force of two different directional twDEP forces, and tallied with our estimation to move along the coupling direction.     

Manipulation of microparticles for construction of array patterns by negative dielectrophoresis using multilayered array and grid electrodes

In this study, a useful method was developed to fabricate array patterns of microparticles not on electrode surfaces, but on arbitrary surfaces, using negative‐dielectrophoresis (n‐DEP). First, electrodes were designed and electric field simulations were performed to manipulate microparticles toward target areas. Based on the simulation results, multilayered array and grid (MLAG) electrodes, consisting of array electrodes surrounded by insulated regions and a grid electrode, were fabricated for the formation of localized, non‐uniform electric fields. The MLAG electrode was mounted to a target substrate in a face‐to‐face configuration with a spacer. When an AC voltage (4.60 V_rms and 1 MHz) was applied to the MLAG electrode, array patterns of 6 and 20 µm diameter microparticles were rapidly fabricated on the target substrate with ease. The results suggest that MLAG electrodes can be widely applied for the fabrication of biochips including cell arrays. Biotechnol. Bioeng. 2009; 104: 709–718 © 2009 Wiley Periodicals, Inc.     

Enhanced cell viability and cell adhesion using low conductivity medium for negative dielectrophoretic cell patterning

Negative dielectrophoretic (n-DEP) cell manipulation is an efficient way to pattern human liver cells on micro-electrode arrays. Maintaining cell viability is an important objective for this approach. This study investigates the effect of low conductivity medium and the optimally designed microchip on cell viability and cell adhesion. To explore the influence of conductivity on cell viability and cell adhesion, we have used earlier reported dielectrophoresis (DEP) buffer with a conductivity of 10.2 mS/m and three formulated media with conductivity of 9.02 (M1), 8.14 (M2), 9.55 (M3) mS/m. The earlier reported isotonic sucrose/dextrose buffer (DEP buffer) used for DEP manipulation has the drawback of poor cell adhesion and cell viability. A microchip prototype with well-defined positioning of titanium electrode arrays was designed and fabricated on a glass substrate. The gap between the radial electrodes was accurately determined to achieve good cell patterning performance. Parameters such as dimension of positioning electrode, amplitude, and frequency of voltage signal were investigated to optimize the performance of the microchip.     

Low frequency electrorotation of fixed red blood cells.

Electrorotation of fixed red blood cells has been investigated in the frequency range between 16 Hz and 30 MHz. The rotation was studied as a function of electrolyte conductivity and surface charge density. Between 16 Hz and 1 kHz, fixed red blood cells undergo cofield rotation. The maximum of cofield rotation occurs between 30 and 70 Hz. The position of the maximum depends weakly on the bulk electrolyte conductivity and surface charge density. Below 3.5 mS/m, the cofield rotation peak is broadened and shifted to higher frequencies accompanied by a decrease of the rotation speed. Surface charge reduction leads to a decrease of the rotation speed in the low frequency range. These observations are consistent with the recently developed electroosmotic theory of low frequency electrorotation.     

Spinning response of yeast cells to rotating electric fields

The frequency-dependent rotation or spinning motion of yeast cells subjected to a fourpole rotating electric field was examined over a very wide frequency range (500 Hz to 500 MHz). In the lower frequency range (500 Hz – 700 KHz) the yeast cells were observed to spin in a direction counter to the applied field, with a small peak at about 600 Hz and a more pronounced one at 20 KHz. For frequencies above 700 KHz the spinning of the cells switched direction from counter-field to co-field, with a maximum in the rotation rate at about 70 MHz and a subpeak at 20 MHz. The rate was also observed to exhibit a square dependence on the magnitude of the applied rotating field.     

Development of a 3D Graphene Electrode Dielectrophoretic Device

The design and fabrication of a novel 3D electrode microdevice using 50 µm thick graphene paper and 100 µm double sided tape is described. The protocol details the procedures to construct a versatile, reusable, multiple layer, laminated dielectrophoresis chamber. Specifically, six layers of 50 µm x 0.7 cm x 2 cm graphene paper and five layers of double sided tape were alternately stacked together, then clamped to a glass slide. Then a 700 μm diameter micro-well was drilled through the laminated structure using a computer-controlled micro drilling machine. Insulating properties of the tape layer between adjacent graphene layers were assured by resistance tests. Silver conductive epoxy connected alternate layers of graphene paper and formed stable connections between the graphene paper and external copper wire electrodes. The finished device was then clamped and sealed to a glass slide. The electric field gradient was modeled within the multi-layer device. Dielectrophoretic behaviors of 6 μm polystyrene beads were demonstrated in the 1 mm deep micro-well, with medium conductivities ranging from 0.0001 S/m to 1.3 S/m, and applied signal frequencies from 100 Hz to 10 MHz. Negative dielectrophoretic responses were observed in three dimensions over most of the conductivity-frequency space and cross-over frequency values are consistent with previously reported literature values. The device did not prevent AC electroosmosis and electrothermal flows, which occurred in the low and high frequency regions, respectively. The graphene paper utilized in this device is versatile and could subsequently function as a biosensor after dielectrophoretic characterizations are complete.     

Dielectrophoretic study of human erythrocytes

This paper is concerned with the dielectrophoretic study of human erythrocytes under cylindrical field geometry. The influence of physical variables such as the frequency and voltage of the applied electric field, conductivity of the medium in which the cells are suspended, cell concentration and exposure time of the cell to the non-uniform electric field on dielectrophoretic collection rate (DCR) is determined in a systematic manner. It is interesting to note from the DCR spectrum of human erythrocytes that the DCR is minimum at one frequency, maximum at another and there is practically no yield over a certain frequency range. This may be attributed to the variation of complex dielectric constant of the particle and medium over that frequency range. From the DCR spectrum of different groups, it is clear that DCR behaviour is different in the frequency range from 0.3–1.5 MHz, under similar conditions of temperature, conductivity and concentration of erythrocyte suspension and strength of applied AC field. The response of DCR with voltage of the applied field, concentration of cell suspension and square root of elapsed time of the cells confirms the theory of dielectrophoresis.     

Applications of dielectrophoretic/electrohydrodynamic "zipper" electrodes for detection of biological nanoparticles

A major problem for surface-based detection techniques such as surface plasmon resonance and quartz crystal microbalances is that at low concentrations, diffusion is an insufficient driving force to bring colloidal submicron-scale particles to the detection surface. In order to overcome this, it has previously been demonstrated that a combination of dielectrophoresis and AC-electro-hydrodynamic flow can be used to focus cell-sized particles from suspension onto a large metal surface, in order to improve the detection capabilities of such systems. In this paper we describe how the combination of these two phenomena, using the so-called "zipper" electrode array, can be used to concentrate a wide range of nanoparticles of biological interest, such as influenza virus, dissolved albumin, and DNA molecules as well as latex beads of various sizes. We also demonstrate that the speed at which particles are transported towards the centre of the electrode pads by dielectrophoresis and electro-hydrodynamic flow is not related to the particle size for colloidal particles.     

The periodic motion of lodgepole pine trees as affected by collisions with neighbors

The periodic sways of a group of ten Pinus contorta var. latifolia (lodgepole pine) trees with slender stems from the Two Creeks site (TW) and ten stout trees from the Chickadee site (CH) both in Alberta, Canada were quantified. Tree displacement at TW was measured during periods of consistent wind direction with three mean wind speeds (1.9, 4.6, and 5.4 m/s) and for two mean wind speeds at CH (5.0 and 7.9 m/s). Spectral analysis of sway displacement data showed a decrease in the frequency with wind speed for trees at TW, but remained unchanged for trees at CH. Significant correlations between tree sway frequency and amplitude during high winds at TW indicate a loss of sway energy concomitant with the occurrence of high collision intensity. These observations support the hypothesis that inter-crown collisions have an important influence on the sway frequency of trees and should be incorporated into efforts to model their sway dynamics. We also present a theoretical collision-damped sway model which supports our empirical findings.     

Homokaryons from animal and plant cells generated by electrofusion

A new apparatus was constructed which enables the use of the electrofusion method to obtain polynuclear cells of various mammalian cell lines, erythrocytes and plant protoplasts. This technique was applied to both suspensions and monolayers. Electrical and other physical parameters were monitored to find optimal conditions for mutual contact of cells (dielectrophoresis) and subsequent fusion. In the suspension technique, dielectrophoresis of mouse erythrocytes occurred at a field frequency of 20 kHz and a strength of 500 V.cm-1, whereas cultured mammalian cells and plant protoplasts required a frequency of 1-1.4 MHz and a strength of 250-800 V.cm-1. Fusion of cells was induced after the application of 1 to 10 high-voltage pulses of 1-5 kV.cm-1, 10-36 microseconds duration. After these high-voltage pulses were to the monolayer of mouse L cells, about 12% viable homokaryons were obtained.     

Proton magnetic relaxation dispersion in solutions of the cuproprotein diamine oxidase.

Proton nuclear magnetic resonance relaxation measurements were made over the range 4.7--220 MHz for aqueous solutions of hog kidney diamine oxidase. The values of 1/T1 give rise in two distinct dispersions, at 16 and 75 MHz, whereas 1/T2 displays a minimum at 20 MHz. The temperature dependence of relaxation rates in all cases yield apparent activation energies less than 0.6 kcal/mol. These data indicate to us that the two Cu(II) ions of diamine oxidase are intrinsically different in terms of their electronic relaxation characteristics and hence, chemical environments. Low field limits of the two electronic relaxation times are 2 and 10 ns, with one of these correlation times being frequency dependent. The value of the frequency-dependent electronic relaxation time is governed by interactions that are modulated by a process having a correlation time of 5 ps.     

Facilitated electrofusion of vacuolated x evacuolated oat mesophyll protoplasts in hypo-osmolar media after alignment with an alternating field of modulated strength

Electrofusion of evacuolated and vacuolated oat leaf protoplasts is difficult because of the different size and density of these cells which results in separation of the two fusion partners during dielectrophoresis. The fusion yield of this cell system was considerably enhanced by electrofusion in hypo-osmolar media containing 0.4 M mannitol, 0.1 mM calcium acetate and 0.1% bovine serum albumin. This increase in yield was only achieved if the dielectrophoretically induced membrane contact between the two fusion partners was enhanced by an initial short 'burst' of higher field strength (500 V/cm, peak to peak, for 5 s followed by a reduction of to 90 V/cm, peak to peak, for 20 s, frequency 1 MHz). Due to the high field strength of the alternating field at the beginning of cell chain formation separation of fusion partners of different size and density was mainly avoided. Simultaneously, the short duration of this high field 'burst' avoided the generation of lethal effects in the cell membranes. The subsequent low field strength of the alternating field was sufficient to keep the aligned cells in position. Optimum fusion was induced by a single square pulse of 750 V/cm and 30 musec duration. The time required for rounding up of the heterologous fusion products decreased with decreasing osmolarity. Fusion resulted in a 5.7 +/- 1.2% yield of heterologous fusion products (compared to 0.7% using the conventional electrofusion protocol) as determined by flow cytometric assay. About 50% of the vacuolated oat protoplasts and 20-50% of the heterologous fusion products regenerated their cell walls within 5 days after hypo-osmolar treatment, but no cell divisions could be observed. Evacuolated oat protoplasts died after 2-3 days in culture without any detectable cell wall regeneration.     

Absorbed energy distribution from radiofrequency electromagnetic radiation in a mammalian cell model: Effect of membrane-bound water

The spatial distributions of induced 27 or 2450 MHz radiofrequency (RF) electric fields (E-fields) and specific absorption rates (SARs) in a three-component spherical cell model (cytoplasm, membrane, extracellular space) were determined by Mie scattering theory. The results were compared to results for the same cell model but with 0.5 nm thick of bound water on the inner (cytoplasmic) and outer (extracellular) membrane surfaces (i.e., five-component cell model). The results provide insight regarding direct frequency-dependent RF radiation effects at the cellular level. Induced E-fields and SARs were calculated for two bound-water characteristic frequencies (400 or 1000 MHz) and ionic conductivities (1–1000 mS/m). In order to estimate the dependence of the results on bound water within the membrane per se, the model was revised to include bound water within the inner and outer membrane surfaces. The results were as follows: (1) On the x-axis, the y- and z-components of the induced E-field were of insignificant magnitude compared to the x-component for an incident E-field parallel to the x-axis; (2) the ratio of transmembrane E-fields induced by 2450 MHz vs. 27 MHz RF [i.e., E_x (2450 MHz)/E_x (27 MHz)] was 0.1; (3) for the three-component cell model, the corresponding SAR ratios [SAR (2450 MHz)/SAR (27 MHz)] in the cytoplasm and extracellular space were 1.66 and 5.0, respectively; (4) the SAR ratios [SAR (2450 MHz)/SAR (27 MHz)] for the cytoplasm and extracellular space for the five-component cell model were 1.66 and 5.0, respectively; (5) the ratio of the E-fields induced in the cytoplasmic and extracellular layers of bound water in the five-component cell model [E (2450 MHz)/E (27 MHz)] were 0.62 and 0.63, respectively; (6) the SAR ratios [SAR (2450 MHz)/SAR (27 MHz)] for the cytoplasmic and extracellular bound-water layers were 66 and 65.3, respectively; and (7) variation of bound-water characteristic frequency, ionic conductivity, or bound-water incorporation inside the membrane surfaces, per se, did not significantly affect the E-field or SAR ratios. These results indicate that frequency-dependent nonuniformities may occur in the distribution of induced RF E-fields and SARs at the cellular level. © 1995 Wiley-Liss, Inc.     

Dielectrophoretic trapping in microwells for manipulation of single cells and small aggregates of particles

In this work we present a novel concept of active microwells based on cylindrical wells able to vertically trap and control single particles by means of negative dielectrophoresis. The device is fabricated by drilling through holes on a polyimide substrate with copper-gold or aluminum metals, forming three annular electrodes within the well. A channel under the device provides a fluid flow filling the microwell by capillarity. Particles are delivered from the top by a microdispenser and applying sinusoidal signals to the electrodes at frequencies ranging from 100kHz to 1.5MHz and amplitudes between 2V and 7V they are successfully trapped and levitated at the level of the central electrode in the middle of microwells with a diameter of 125mum. By changing signal phases, other configurations are also enabled to load particles in the well or eject them from the bottom. The extension to an array of microwells is presented and design rules are described for routing electrode connections and setting signal parameters. K562 cells cultured with Ara-C 1000nM were successfully trapped and controlled in physiological media. Polystyrene beads were also levitated in water and were used for experimental measurements on minimum amplitudes and phase differences in the signals required to levitate beads, confirming the results obtained by simulation.     

Dependence of dielectrophoretic force on the size of cylindrical particles by the example of a suspension of erythrocytes

For the modeling of erythrocyte rouleaux (linear cell aggregations), we propose an approximation procedure for the dipole moment in short cylinders, which contains the case of ellipsoidal bodies only as a first approximation. The method allows one to introduce corrections that are more representative for these particles. Depending on the number of erythrocytes forming an aggregation, i.e., on different but discrete measures of rouleaux lengths, the dielectrophoretic force is calculated and represented against the frequency of the applied a.c. field. As a result, frequency regions in the upper MHz range appear in which the strength and direction of DEP forces are different for different rouleaux sizes. This property is suitable for the detection and spatial separation of rouleaux populations of different length in blood samples by means of a microelectronic array.