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Label-free Isolation and Enrichment of Cells Through Contactless Dielectrophoresis

LEHRERVORBEREITUNG
KONZEPTE
SCHÜLERPROTOKOLL
JoVE Journal
Medizin
This content is Free Access.
JoVE Journal Medizin
Label-free Isolation and Enrichment of Cells Through Contactless Dielectrophoresis

1. Fabricating a Prototype cDEP Microfluidic Device: Overview

  1. Follow previously reported procedures22 using photoresist and Deep Reactive Ion Etching (DRIE) to etch the desired channel design (Figure 1) into a silicon wafer (Figure 2). Deposit a thin layer of Teflon to improve the release of the microdevice from the wafer.

Figure 1
Figure 1. Schematic of a low frequency continuous sorting device. The sample channel runs left to right and is 500 μm wide with sawtooth constrictions to 100 μm. The two pairs of fluidic electrode channels compose the source and sink electrodes, respectively, and are separated from the sample channel by a 20 μm thick PDMS barrier.

Figure 2
Figure 2. The fabrication process of a cDEP device. (a) For 60 sec, UV light selectively reacts with photoresist exposed through a mask pattern of the cDEP device geometry. (b) Photoresist is removed using developer. (c) Deep Reactive Ion Etching (DRIE) is used to etch 50 μm deep features, and 5 min of wet etching by tetramethylammonium hydroxide (TMAH) 25% at 70 °C is used to reduce roughness on the side walls. (d) A Teflon coating is added to improve device release from the wafer. (e) PDMS is poured onto the re-usable wafer stamp after degassing and cured for 45 min at 100 °F. (f) PDMS is removed from the wafer. PDMS and a clean glass slide are exposed to air plasma for 2 min and bonded together.

  1. Wrap the wafer with aluminum foil to prevent spill-over. Mix polydimethylsiloxane (PDMS) in 10:1 ratio of elastomer to curing agent, de-gas for approximately 20 min, and pour onto the wafer. Heat for 45 min at 100 °C to avoid damaging the Teflon coating of the stamp. Allow the device to cool down.
  2. After cooling, remove aluminum foil, trim PDMS using a surgical blade, and punch access holes at channel inlet/outlet using a blunt puncher suited to the size of tubing. Here, a 1.5 mm blunt puncher is used.
  3. Clean a glass microscope slide using a rinse of soap and water, ethanol, DI water, and drying with air, respectively. Clean the PDMS device using Scotch Magic tape. Examine under microscope to be sure channels are clean. Expose the slide and PDMS device to air plasma for 2 min. Firmly press channel side of device to glass slide, avoiding formation of air bubbles between the device and the slide (Figure 3).

Figure 3
Figure 3. (a) The mask used for photolithography during the silicon wafer stamp fabrication, and (b) the finished PDMS-glass device with the sample and fluid electrode channels filled with green and red food coloring, respectively. See Figure 1 for dimensions. Click here to view larger figure.

2. Preparing a Cell Suspension in DEP Buffer

  1. Prepare a low conductivity (100 μS/cm) buffer, which will be referred to as "DEP buffer" (8.5% sucrose [w/v], 0.3% glucose [w/v], 0.725% RPMI [v/v]).16
  2. Suspend cells in DEP buffer at 3 x 106 cells/ml. Here, cancerous late-stage mouse ovarian surface epithelial (MOSE-L) cells are used.

Note: Cell viability analysis by the trypan blue dye exclusion method showed a slight decrease in viability (from 95.1-91.6%) of early-stage MOSE (MOSE-E) cells suspended in DEP buffer at room temperature after 5 hr. It is predicted that a similar slight decrease in viability occurs for MOSE-L cells, indicating that cells should not be stored in DEP buffer long-term.

  1. Dye cells using a fluorescent membrane-permeable dye, such as the enzymatically-activated Calcein AM.
  2. Measure conductivity of the dyed cell suspension. The conductivity should be approximately 100 μS/cm. If the conductivity measurement is too high, spin the sample down, resuspend in DEP buffer at 3 x 106 cells/ml and repeat the conductivity measurement.

3. Loading the cDEP Microfluidic Chip

  1. Place the microfluidic chip under vacuum for 30 min.
  2. Meanwhile, cut a piece of flexible tubing to span the distance from the syringe pump to the microscope stage where the microfluidic chip will be located. Here, a 6 inch length of tubing is required. Fit tubing to needle tip on syringe.
  3. Estimate the required length for outlet tubing by dividing the target collected sample volume by the cross-sectional area of the tube. Cut the require length of tubing.
  4. Draw cell suspension into syringe. Check that no bubbles are located in the tubing or syringe.
  5. Upon removing chip from vacuum, insert the outlet tubing and prime the sample channel quickly to avoid trapped air bubbles in the channels. Gently tap the syringe when priming to avoid rupturing the thin (20 μm) insulating barrier, though it has been observed that the barrier can withstand a constant high throughput near 5 ml/hr without rupturing.
  6. To prime the electrode channels, quickly place empty pipette tips in one outlet of each fluidic electrode channel. Pipette 200 μl of PBS containing a small amount of rhodamine B and gently tap to introduce the fluid into the opposite end of the electrode channel. Maintain gentle pressure until PBS with rhodamine B visibly progresses up the tip of the empty pipette tip. Repeat for each electrode channel. Rhodamine B is used only to fluorescently visualize the fluidic electrode channels.
  7. After priming, fill each pipette tip reservoir with PBS with rhodamine B. Avoid bubble formation in the pipette tip reservoirs, and remove any visible bubble by pipetting gently up and down. Detach the outlet tubing and discard appropriately, then insert a fresh outlet tubing reservoir to collect the target volume.

4. Characterizing Crossover Frequency of Cells using cDEP Chip

  1. Position the chip on the stage of an inverted microscope equipped with digital camera (Figure 4).

Figure 4
Figure 4. (a) Overall experimental setup for cDEP experiments. The cDEP chip is located on the platform of the inverted microscope. A camera sends images to the computer for recording. The syringe pump maintains a constant inlet flow. The function generator generates a signal which is stepped up by the high voltage amplifier and connected to the cDEP chip by wire electrodes. The oscilloscope monitors the signal sent to the chip. (b) Detail view of the cDEP chip and fluidic and electronic connections. Click here to view larger figure.

  1. Mount syringe on syringe pump and insert wire electrodes into fluidic electrode channel reservoirs.
  2. Pump fluid through at 1 ml/hr to ensure good contact between the syringe pump and the syringe. Visually inspect the channel length to ensure unimpeded flow of cells and the absence of bubbles or leaks. Reduce flow rate to 0.005 ml/hr.
    Note: Throughput as high as 1 ml/hr31,35 has been achieved in devices of other geometries.
  3. For safety, test the electronics by powering on the function generator, high voltage amplifier, and oscilloscope, and adjusting to desired voltage and frequency. Here these parameters are 200 V and 20 kHz. Upon verification of acceptable performance, power off. Connect electrodes to high voltage amplifier.
    Note: Observe appropriate electrical safety procedures when operating the electronics at the high voltages used for these experiments.
  4. Upon achieving steady flow, apply the desired voltage at the desired frequency. In this experiment, voltage is 200 VRMS at frequencies between 5-60 kHz.
  5. Record video files of the cell response with image processing techniques (step 5) to quantify cell distribution in the channel and to characterize the crossover frequency. To do this, maintain a constant voltage and vary the frequency systematically. At the start and end of the experiment, as well as randomly between experimental runs, record the control cell distribution, the distribution of the cells without applying any electrical field. Estimate the amount of time required for cells to flow from the inlet to the monitored location (here, 5 min). After setting a new frequency, wait this amount of time, then begin recording (here, a 2 min video of cell distribution).

5. Image Processing for Characterizing Crossover Frequency

  1. Using a computational script, analyze each video frame by frame to determine the relative y-position (where the z-direction is the vertical depth of the channel, the y-direction is the channel width, and x-direction is the channel length) of each fluorescing cell or particle at a specified x-coordinate downstream from the region of high DEP force in the channel. Create a graph of the relative distribution.
  2. Compare the centerline of the distribution at each voltage and frequency with the centerline of the control distribution. For a given voltage and varying frequencies, determine the crossover frequency, where the centerline matches the y-position of the control.

6. Varying the Experiment to Perform Cell Sorting or Enrichment

  1. Suspend desired mixture in DEP buffer at a total concentration of 3 x 106 particles/ml. Here, this mixture is MOSE-L cells with 4 μm fluorescing beads in DEP buffer. Perform the previously described steps to prepare a cDEP device.
  2. To sort or enrich cells from a mixture, determine the crossover frequencies of the target cells and the background particles as previously described. Operate the experiment at a frequency between the two crossover frequencies of the target cells and the background particles so that the two populations of particles experience DEP forces in opposite directions. To sort MOSE-L cells and 4 μm beads, operate the microdevice above 11.90±0.63 kHz. the first crossover frequency of MOSE-L cells recently reported by Salmanzadeh et al.33
  3. To collect the contents of a sorted sample, remove the outlet tubing upon collecting the target volume, by placing a glove finger over the outlet opening and gently tugging on the tubing. Pour the collected target volume into a reservoir for further analysis. Note: Other sample recovery methods could include attaching a permanent reservoir to the chip and removing the sample by simple pipetting.

Label-free Isolation and Enrichment of Cells Through Contactless Dielectrophoresis

Learning Objectives

DEP should be observed qualitatively in the sample channel to confirm the device is operational when the electric field is present. One method to test for the presence of DEP is to adjust the frequency to values far from the crossover frequency where strong pDEP and nDEP are predicted (roughly >40 kHz to observe pDEP and <10 kHz to observe nDEP for most mammalian cancer cells in a buffer with conductivity of 100 μS/cm). It should be noted that inert microspheres exhibit pDEP below their crossover frequency and nDEP above their crossover frequency. For the sawtooth feature geometry presented here, pDEP should be seen for cells at the higher test frequency, indicated by the occurrence of pearl chaining and focusing of cells or particles at the sawtooth feature edge of the channel, while at the lower test frequency, nDEP should be apparent as cells are restricted to the region nearer the straight edge of the channel. At these low frequencies, cells may lyse due to electroporation, so the sample may appear to contain fewer cells, and those that are visible may appear enlarged or blurry if using an enzymatically-activated fluorescing dye. Verifying the frequencies at which pDEP and nDEP occur allows the determination of the crossover frequency as described in the protocol. For mammalian cancer cells, such as MOSE-L used here, we observed nDEP at 5 kHz (Figure 5a) and strong pDEP at 60 kHz (Figure 5b). MOSE-L cells had a diameter of 17.7±3.3 μm (n = 268 cells) and the beads have a 4 μm nominal diameter. A full analysis of the dielectric properties of MOSE-L cells compared to MOSE cells in earlier stages of progression can be found in the recent work by Salmanzadeh et al.33

If pDEP and nDEP are not observed at these extremes, various problems could be occurring. The sample conductivity may be too high due to contaminants or cell lysing. Insufficient electric field may be generated due to bubbles trapped in the fluid electrode channels, which prevent conduction of current to the portion of the channels bordering the sample channel. Unsteady flow may be caused by a bubble trapped in the syringe or inlet tubing, bubbles resulting from not keeping the device under vacuum for a sufficient time or not quickly filling the device upon removing from vacuum, leakage due to delamination of poorly bonded PDMS to the glass slide, tears in the barrier membrane due to excessive force exerted when filling the channels, or flow rates at the extremes of the pump operating range.

In addition to determining the crossover frequency of cells, this technique can be used to sort a mixture, illustrated here by a mixture of MOSE-L cells and beads. This example takes advantage of the negative dielectrophoresis (nDEP) exhibited by 4 μm beads at frequencies where MOSE-L cells experience positive dielectrophoresis (pDEP). We operated the device at 200 VRMS and 10 kHz (Figure 6a) and observed that both cells and beads were mixed as they experienced nDEP. At 50 kHz we observed movement of MOSE-L cells to the top of the channel, while beads were restricted to the lower portion of the channel, enabling separation of the mixture into two components (Figure 6b).

Figure 5
Figure 5. The position of MOSE-L cells is manipulated by changing the frequency of the applied electric field. The photos are taken at the final sawtooth feature in the sample channel and the fluidic electrodes are located at the corners on the right side. They are filled with PBS containing rhodamine B, which fluoresces to visualize the channels. (a) MOSE-L cells experience nDEP at 200 VRMS and 5 kHz. (b) MOSE-L cells experience pearl chaining and pDEP at 200 VRMS and 60 kHz. Click here to view larger figure.

Figure 6
Figure 6. A mixture of MOSE-L cells (green) and 4 μm beads (red) flow through the final sawtooth feature in the sample channel of a low frequency cDEP device. (a) At 200 V and 10 kHz cells and beads are mixed. Arrows point to faintly appearing cells that likely have died due to the low frequency conditions. (b) At 200 V and 50 kHz cells experience pDEP and move to the feature edge of the channel, while beads experience nDEP and remain confined to the region nearer the straight edge. Click here to view larger figure.

List of Materials

Name of Reagent/Material Company Catalog Number Comments
Polydimethylsiloxane (PDMS) Dow Corning, Midland, MI,USA Sylgard 184  
Glass slides The Microscope Depot 76079 2×3 inch-ground edges
Microbore PTFE Tubing Cole-Parmer Instrument Co, Vernon Hills, IL, USA EW-06417-31 Thin walled 20 gauge, 0.032″ID x 0.056″OD, 100 ft/roll
Luer-slip plastic syringes National Scientific company S7510-1  
Needle tip Howard Electronic instruments JG20-1.0 20 Gauge 1.0″, ID=0.025″ OD=0.036″
D(+)-Sucrose Fisher Scientific, Fair Lawn, NJ S3-500  
D(+)-glucose, reagent ACS, anhydrous Acros Organics N.V., Fair Lawn, NJ AC410955000  
RPMI-1640 Medium Quality Biological Inc. 112-025-101  
Calcein AM, Molecular Probes Invitrogen Corp. (life technologies), Carlsbad, CA, USA C3100MP excitation wavelength 488/emission wavelength 516
Rhodamine B, O Science Lab SLR1465-100G excitation wavelength 540/emission wavelength 625
Phosphate buffered saline (10X) Gbiosciences, St. Louis, MO RC-147  
Leica, inverted light microscope Leica Microsystems, Bannockburn, IL, USA Leica DMI 6000B  
Leica DFC420, color camera Leica Microsystems, Bannockburn, IL, USA Leica DFC420  
Function generator GW Instek, Taipei, Taiwan GFG-3015  
Wideband power amplifier Amp-Line Corp., Oakland Gardens, NY, USA AL-50HF-A  
HFHV Output Transformer   AL-T50-V25/300-F100K-600K  
High voltage amplifier Trek Model 2205  
USB Modular Oscilloscope, 100 MHz AgilentTechnologies U2701A  
Expanded Plasma Cleaner Harrick Plasma PDC-001/002 (115/230V) air plasma
Scotch Magic tape 3M   any available width is sufficient
1.5 mm puncher Harris Uni-Core Z708836-25EA  
.25% Trypsin-EDTA Invitrogen 25200-056  
FluoSpheres Sulfate Microspheres Invitrogen F8858 4.0 μm, red fluorescent (excitation wavelength 580/emission wavelength 605)
AZ 9260 photoresist AZ Electronic Materials    
AZ 400 K developer AZ Electronic Materials    
Tetramethylammonium hydroxide (TMAH) 25%     provided by Virginia Tech cleanroom
Teflon coating     applied using DRIE machine
Silicon wafer University Wafer 452 100 mm diameter, 500 μm thickness, one side polished (SSP)
Deep Reactive Ion Etching (DRIE) Alcatrel AMS SDE 100  

Lab Prep

Dielectrophoresis (DEP) is the phenomenon by which polarized particles in a non-uniform electric field undergo translational motion, and can be used to direct the motion of microparticles in a surface marker-independent manner. Traditionally, DEP devices include planar metallic electrodes patterned in the sample channel. This approach can be expensive and requires a specialized cleanroom environment. Recently, a contact-free approach called contactless dielectrophoresis (cDEP) has been developed. This method utilizes the classic principle of DEP while avoiding direct contact between electrodes and sample by patterning fluidic electrodes and a sample channel from a single polydimethylsiloxane (PDMS) substrate, and has application as a rapid microfluidic strategy designed to sort and enrich microparticles. Unique to this method is that the electric field is generated via fluidic electrode channels containing a highly conductive fluid, which are separated from the sample channel by a thin insulating barrier. Because metal electrodes do not directly contact the sample, electrolysis, electrode delamination, and sample contamination are avoided. Additionally, this enables an inexpensive and simple fabrication process.

cDEP is thus well-suited for manipulating sensitive biological particles. The dielectrophoretic force acting upon the particles depends not only upon spatial gradients of the electric field generated by customizable design of the device geometry, but the intrinsic biophysical properties of the cell. As such, cDEP is a label-free technique that avoids depending upon surface-expressed molecular biomarkers that may be variably expressed within a population, while still allowing characterization, enrichment, and sorting of bioparticles.

Here, we demonstrate the basics of fabrication and experimentation using cDEP. We explain the simple preparation of a cDEP chip using soft lithography techniques. We discuss the experimental procedure for characterizing crossover frequency of a particle or cell, the frequency at which the dielectrophoretic force is zero. Finally, we demonstrate the use of this technique for sorting a mixture of ovarian cancer cells and fluorescing microspheres (beads).

Dielectrophoresis (DEP) is the phenomenon by which polarized particles in a non-uniform electric field undergo translational motion, and can be used to direct the motion of microparticles in a surface marker-independent manner. Traditionally, DEP devices include planar metallic electrodes patterned in the sample channel. This approach can be expensive and requires a specialized cleanroom environment. Recently, a contact-free approach called contactless dielectrophoresis (cDEP) has been developed. This method utilizes the classic principle of DEP while avoiding direct contact between electrodes and sample by patterning fluidic electrodes and a sample channel from a single polydimethylsiloxane (PDMS) substrate, and has application as a rapid microfluidic strategy designed to sort and enrich microparticles. Unique to this method is that the electric field is generated via fluidic electrode channels containing a highly conductive fluid, which are separated from the sample channel by a thin insulating barrier. Because metal electrodes do not directly contact the sample, electrolysis, electrode delamination, and sample contamination are avoided. Additionally, this enables an inexpensive and simple fabrication process.

cDEP is thus well-suited for manipulating sensitive biological particles. The dielectrophoretic force acting upon the particles depends not only upon spatial gradients of the electric field generated by customizable design of the device geometry, but the intrinsic biophysical properties of the cell. As such, cDEP is a label-free technique that avoids depending upon surface-expressed molecular biomarkers that may be variably expressed within a population, while still allowing characterization, enrichment, and sorting of bioparticles.

Here, we demonstrate the basics of fabrication and experimentation using cDEP. We explain the simple preparation of a cDEP chip using soft lithography techniques. We discuss the experimental procedure for characterizing crossover frequency of a particle or cell, the frequency at which the dielectrophoretic force is zero. Finally, we demonstrate the use of this technique for sorting a mixture of ovarian cancer cells and fluorescing microspheres (beads).

Verfahren

Dielectrophoresis (DEP) is the phenomenon by which polarized particles in a non-uniform electric field undergo translational motion, and can be used to direct the motion of microparticles in a surface marker-independent manner. Traditionally, DEP devices include planar metallic electrodes patterned in the sample channel. This approach can be expensive and requires a specialized cleanroom environment. Recently, a contact-free approach called contactless dielectrophoresis (cDEP) has been developed. This method utilizes the classic principle of DEP while avoiding direct contact between electrodes and sample by patterning fluidic electrodes and a sample channel from a single polydimethylsiloxane (PDMS) substrate, and has application as a rapid microfluidic strategy designed to sort and enrich microparticles. Unique to this method is that the electric field is generated via fluidic electrode channels containing a highly conductive fluid, which are separated from the sample channel by a thin insulating barrier. Because metal electrodes do not directly contact the sample, electrolysis, electrode delamination, and sample contamination are avoided. Additionally, this enables an inexpensive and simple fabrication process.

cDEP is thus well-suited for manipulating sensitive biological particles. The dielectrophoretic force acting upon the particles depends not only upon spatial gradients of the electric field generated by customizable design of the device geometry, but the intrinsic biophysical properties of the cell. As such, cDEP is a label-free technique that avoids depending upon surface-expressed molecular biomarkers that may be variably expressed within a population, while still allowing characterization, enrichment, and sorting of bioparticles.

Here, we demonstrate the basics of fabrication and experimentation using cDEP. We explain the simple preparation of a cDEP chip using soft lithography techniques. We discuss the experimental procedure for characterizing crossover frequency of a particle or cell, the frequency at which the dielectrophoretic force is zero. Finally, we demonstrate the use of this technique for sorting a mixture of ovarian cancer cells and fluorescing microspheres (beads).

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