Wei
Cheng
a,
Norbert
Klauke
a,
Helen
Sedgwick
a,
Godfrey L.
Smith
b and
Jonathan M.
Cooper
*a
aBioelectronics Research Centre, Department of Electronics and Electrical Engineering, University of Glasgow, Glasgow, UK G12 8QQ. E-mail: jmcooper@elec.gla.ac.uk
bInstitute of Biomedical and Life Sciences, University of Glasgow, Glasgow, UK G12 8QQ
First published on 14th September 2006
A device based on five individually addressable microelectrodes, fully integrated within a microfluidic system, has been fabricated to enable the real-time measurement of ionic and metabolic fluxes from electrically active, beating single heart cells. The electrode array comprised one pair of pacing microelectrodes, used for field-stimulation of the cell, and three other microelectrodes, configured as an electrochemical lactate microbiosensor, that were used to measure the amounts of lactate produced by the heart cell. The device also allowed simultaneous in-situ microscopy, enabling optical measurements of cell contractility and fluorescence measurements of extracellular pH and cellular Ca2+. Initial experiments aimed to create a metabolic profile of the beating heart cell, and results show well defined excitation-contraction (EC) coupling at different rates. Ca2+ transients and extracellular pH measurements were obtained from continually paced single myocytes, both as a function of the rate of cell contraction. Finally, the relative amounts of intra- and extra-cellular lactate produced during field stimulation were determined, using cell electroporation where necssary.
Recent advances in lab-on-a-chip and other microtechnologies have attracted significant interest in the development of new microdevices for cell analysis, where precise control over the geometry of the sensor improves signal collection. The comparable size of single cells and microfluidic structures has provided an opportunity for more sensitive analysis, because the cell comprises a substantial fraction (often as much as 10%) of the volume being analysed.7–9
As a consequence, there has been a considerable interest in developing microsensors integrated within lab-on-a-chip structures for the analysis of single cells. For example, attempts to estimate the metabolic flux of cells using electrochemically-linked assays have been made10–13 and, most recently, a system to record membrane potential using microfluidics to trap single cells in a sub-nanolitre chamber has been described.14 There has, however, been substantially less work developing on-chip assays, where the cell’s metabolic and physiological function is manipulated in situ (including, for example, single-cell manipulation and intracellular monitoring,15–17 and single-cell perfusion or lysis followed by analysis of intracellular contents using chip-based electrophoresis18–20).
In this paper, studies of the physiology of single cardiomyocytes in a microfluidic system are presented. We describe an electrochemical biosensor, designed to measure extracellular lactate, which is combined with stimulating microelectrodes and integrated within a picolitre (pL)-scale microfluidic chamber. The device is used to stimulate the cell at pre-determined rates and explore the effect of making the cell “work” under different metabolic conditions. The microsystem also allows changes in cell length, pH and Ca2+ to be measured at the same time, providing details of the electrical and metabolic state of the heart cell. The measurements that we report of the metabolites released from the single heart cell will improve our understanding of cell metabolism during anoxia or ischemia.10–12
We chose to measure the single-cell production of lactate because it is an important cellular metabolite and of significant clinical interest in heart cell physiology. For example, lactate levels can be monitored to indicate the health of a cell, because damaged cells, or those in which oxygen supply is restricted, tend to produce larger amounts of lactate. Previously, the detection of lactate has been achieved using enzyme-linked electrochemical assays based on lactate oxidase. Although there have been attempts to immobilise the enzyme at both macroelectrodes21 and microelectrodes,22 less progress has been made on developing enzyme-modified integrated microbiosensors for monitoring lactate released from single cells within microfluidic devices.12
We have developed an immobilised microfabricated enzyme-modified sensor, used to determine the amounts of lactate produced from single cells in pL volumes with a detection limit of 4.8 fmol (equivalent to 7.4 µM). Within the microsystem, single cardiomycotes were forced to contract continuously using field stimulation (ca. 75 V cm−1) at rates between 0.5 and 2.0 Hz, as might be expected of the rabbit heart. Intracellular Ca2+ transients were monitored from continually paced single cardiomyocytes using Fluo-3 (a fluorescent Ca2+ indicator). Finally, the effect of continual pacing on the cell’s contractility and the extracellular pH in the restricted volume of the microchamber was investigated, and the results were interpreted in the context of lactate release.
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Fig. 1 Schematic illustration of the major steps involved in the device fabrication: (1) the photoresist-coated substrate was exposed to UV radiation through a mask; (2) the photoresist was developed; (3) metals were deposited by evaporation; (4) the electrode pattern was generated by lift-off; (5) silver was deposited by evaporation; (6) spin-coating was used to generate an S1818 photoresist sacrificial layer; (7) the device was again exposed to UV radiation; (8) the SU-8 and S1818 layers were developed; (9) finally, AgCl was electrochemically deposited. |
The microstructure fabrication involved the deposition of the microelectrodes onto a glass slide, which had been sonicated and cleaned in Opticlear™, acetone and methanol. The clean slide was spin-coated with S1818 photoresist at 4000 rpm for 30 sec, baked for 30 minutes at 90 °C and then soaked for 15 minutes in chlorobenzene. The electrode pattern was transferred onto the photoresist layer by UV exposure through a mask, followed by resist development. Metals were then deposited by electron beam evaporation producing a multilayer electrode structure of Ti/Pd/Pt (10/10/100 nm). The 10 nm Ti metallic underlayer allowed for good adhesion of the Pt over-layer to the glass slide, whilst the 10 nm Pd layer acted as a diffusion barrier layer to ensure good electrochemistry by preventing Ti from diffusing into the Pt. Finally, the platinum over-layer was evaporated to produce a coherent 100 nm thick electrode layer. After metal deposition, the microelectrode pattern was realised by lift-off in acetone. Associated with the microelectrode array were alignment marks to enable subsequent microstructures including both microfluidic structures and the Ag|AgCl reference to be deposited.
One of the Pt electrodes (Fig. 2, B) was modified with an Ag|AgCl layer to provide a reference electrode. Silver was coated using the same basic microfabrication process described above, in which a second mask was used to define a 20 µm × 20 µm area, over the reference electrode, using an appropriate registration and alignment series. The AgCl layer was deposited galvanostically at +0.15 V in a solution of 0.1 M HCl (until the oxidation current decreased to background). During the deposition of AgCl, a coil of platinum wire was used as a common counter and the pseudo-reference electrode.
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Fig. 2 Micrograph of the microelectrodes and 20 µm deep microchamber. The different functional microelectrodes are indicated as A, B, C, D and E (see text). A quiescent cardiomyocyte is also shown in the microchamber. |
Immediately prior to any further processing, a layer of S1818 photoresist was patterned over the microelectrode array as a sacrificial layer, protecting the electrodes from fouling by residues from subsequent processes. The microchamber and microfluidic structures were defined by photolithographically patterning an SU-8 negative resist. A 20 µm deep layer of SU-8 resist was patterned using the processing steps of spin-coating, pre-exposure baking, UV exposure through a mask, post-exposure baking and development. Five bonding pads, each associated with one of the five individual microelectrodes, were also exposed through the SU-8 layer.
A series of other microstructures were produced and used during this study, including the creation of micro-reservoirs for cell micro-culture. These comprised a poly(dimethylsiloxane) (PDMS) chamber of volume ca. 200 µl created by replica molding against an SU-8 master. Such structures were used as “holding tanks” for the selection and storage of cells immediately prior to measurements.
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H2O2 → 2H+ + O2 + 2e− +640 mV vs. Ag/AgCl | (2) |
Immediately prior to enzyme immobilization at the Pt working electrode (Fig. 2, A) the microfabricated electrochemical electrode was cleaned by scanning the applied potential between −1 V and +1 V in 100 mM H2SO4 at 1 V s−1, followed by washing in ultrapure water. The enzyme (20 µl solution containing 200 units per ml in PBS, pH 7.4) was pre-adsorbed onto the electrode surface by incubation overnight at 4 °C. A poly(o-phenylenediamine) film was deposited using cyclic voltammetry by scanning the applied potential at a rate of 50 mV s−1 for 6 min between 0.0 and +0.80 V vs. Ag|AgCl microreference in a supporting electrolyte solution of 50 mM PBS containing 50 mM KCl and 30 mM o-phenylenediamine. The growth of non-conducting polymer is self-limiting, and typically the resultant current fell to a steady state value within a minute, producing a film of defined thickness and composition. The polymer entrapped the enzyme locally at the working electrode, allowing the ready diffusion of electro-active species to the electrochemical interface. Inevitably some enzyme will be non-specifically adsorbed on other electrodes and within the microstructure, and much of this was removed by exhaustive washing prior to cell measurements. As a consequence, the majority of the measured current can be attributed to the locally immobilised enzyme. The device was stored under PBS buffer at 4 °C.
The pipette could be readily manoeuvred into the microchamber for low-volume dispensation using a three-axis micromanipulator (Leica, Germany). The whole operation was monitored using an inverted microscope (Zeiss, Axiovert). The microchamber was first filled with 0.2 µl of PBS, which was immediately covered with mineral oil to prevent the evaporation of bulk solution. An empty micropipette with an end bore of 40 µm was then inserted through the mineral oil layer into the droplet, so the buffer within the microchamber back filled the micropipette by capillary action. By carefully repeating the insertion and removal of the pipette, the total volume of the buffer could be readily controlled. To dispense pL-scale volumes, a second filament pipette with tip of ca. 1 µm diameter was filled with an appropriate stock solution (such as a calibration aliquot containing lactate). The injection pressure was 20 psi, and injection times of 20–1000 ms were used. There was a linear relationship between estimated injection volume and dispensation time over this range.
The micropipette was positioned above and close to the selected cell within the holding chamber and, by gentle expulsion and suction of the capillary, the cell was introduced into the capillary tip. The micropipette was then brought over the microchamber and a droplet containing the cell was deposited into the microchamber, such that the myocyte was aligned longitudinally to the axis of the chamber. The cell was observed to sediment to the bottom of chamber. As previously described, the volume of the medium was then reduced to the volume of the analytical microchamber by a second micropipette (tip diameter 40 µm).
Individual cells, Fig. 2, were stimulated within the device by applying a biphasic rectangular pulse of alternating polarity through the pair of stimulatory microelectrodes (Fig. 2, D and E) using a custom-built electric field stimulator coupled with a frequency generator. The amplitude, duration and frequency of applied potentials were controlled using instrumentation built in-house. The pH sensitive dye BCECF (10 µM, Molecular Probes, Eugene, OR, USA) was added to the microchamber to monitor the change in extracellular pH during field stimulation using the same filter set as for Fluo-3, described previously. The change in pH could arise either through the cell’s metabolic process or from electrolysis events owing to the stimulating microelectrodes (hydrolysis would be expected to occur at potentials >0.8 V vs. Ag|AgCl, and in all field stimulation experiments absolute applied potentials were maintained below this value).
A low-current potentiostat (CV-37, BAS) with data acquisition software was used to monitor the lactate produced from single cells. The lactate response was measured amperometrically at +640 mV vs. Ag|AgCl, recording the oxidation of enzymically produced H2O2, as previously detailed in eqn 1 and 2.
Previous reports23,24 suggest that a more efficient stimulation is provided when the electrical axis of stimulation is parallel to the long axis of the cardiac cell, as measured by the reduced potential required for effective cell excitation. The two stimulatory electrodes were therefore fabricated within the microchamber so that the cell could be easily aligned parallel to the electrical field. A sufficiently low voltage stimulatory pulse was applied, avoiding both electrolysis and polarisation of the electrodes and minimising the ionic flux caused by stimulation that could interfere with measurements.
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Fig. 3 Typical cyclic voltammograms showing the deposition of the polymer film (scan rate at 50 mVs−1) obtained using the microfabricated enzyme-modified sensor in PBS buffer (pH = 7.4) containing 30 mM o-phenylenediamine. The sensor surface area was 1800 µm2. |
After the adsorption of the enzyme and its subsequent entrapment in the polymer film, the sensors were characterised by the addition of standard aliquots of pL-amounts of L-lactate using the nanopipette system. The microchamber was first filled with 650 pL of PBS buffer (pH = 7.4) and, using pre-determined injection time intervals, 1.2 mM L-Lactate stock solution was injected to give final lactate concentrations of 7.4 µM, 18.5 µM , 36.9 µM, 55.4 µM, 101.5 µM, 221.5 µM and 443.1 µM. Each injection immediately resulted in a measurable electrochemical oxidation current with the signal returning to the background within 5–10 s, Fig. 4. The measured charge, Q, corresponded to total H2O2 oxidation, and showed a linear relationship to the quantity of injected lactate, x, up to a maximum of 101.5 µM (specifically, Q (nC) = 0.1835x (fmol), r = 0.993). The precision of measurement was investigated from four repetitive measurements with standard deviations <5.2%. To account for the non-Faradic current caused by the injection pulse perturbing the electrode double layer, two control experiments were performed involving the addition of identical volumes of buffer of the same ionic constitution, and the injection of lactate before the sensor was modified by enzyme. Although, in either case, there was a small background signal, the integral of total Q was always <2% of the equivalent titre of lactate, measured under identical experimental conditions.
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Fig. 4 Representative current–time response to successive additions of pL lactate, as described in the text. The total charge generated is the integral of the current–time curve. The relationship between Q with respect to the amount of lactate added was linear between 4.8 and 66.0 fmol, with a correlation coefficient r of 0.993. The sensor surface area was 1800 µm2. |
A minimum detection limit of 4.8 fmol was obtained (equivalent to the detection of ca. 7.4 µM considering the chamber volume of 650 pL), which compared favourably with other immobilised macro- and microelectrode biosensor systems.21,22 It is also interesting to note the fast response of the sensors, especially when compared to that using free-enzyme sensors.12 This high temporal resolution and sensitivity is important for real-time monitoring of metabolites.
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Fig. 5 Time course of local pH change within the 650 pL microchamber buffered in 20 mM HEPES at field strength above the threshold for electrical stimulation of single myocytes. The change in emission of BCECF was related to the initial emission and plotted as the relative intensity against time. The pH was monitored from a region of 4 µm × 4 µm which was located 2 µm away from the initial anode within the microchamber. After 25 s of continuous pulsing, the polarity of the pulses was reversed. |
In common with previous reports, it was found that stimulating the myocyte along the length of the cell, as opposed to across its width, reduced the potential at which stimulation could be initiated.23,24
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Fig. 6 (a) Intracellular [Ca2+] transients from Fluo-3 indicator-loaded single cardiomyocytes stimulated at field strength of 75 V cm−1 and frequencies of 0.5 Hz and 1.0 Hz. The vertical axis gives the relative fluorescence intensity, and the vertical bars along the horizontal axis indicate the start of each pulse. (b) The relative mean sarcomere length recorded from the same cardiomyocyte within the microchamber, where 100% indicates the maximum relative degree of contraction with respect to the resting cell. |
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Fig. 7 (a) The effect of applying short high voltage pulses (10 V, 0.04 ms) at 15 s, 30 s, and 45 s in the absence of the cell. (b) Typical responses to lactate released from an eletropermeabilised cell, (i) in the absence of pacing, no lactate is present in the extracellular space, (ii) electrochemical response as lactate is released from the single cardiomyocyte after eletropermeabilisation. The modified sensor was poised at 0.64 V vs. integrated Ag/AgCl microreference. |
Lactate was released from the cell immediately after the high pulse was applied. Fig. 7(b) shows a typical electrochemical response of lactate released from a single myocyte after electropermeablisation. Using the calibration curve, Fig. 4, we estimate that in total ca. 31 µM lactate was detected. Assuming that all the intracellular lactate was released and constrained within the microchamber, the average concentration of intracellular lactate was estimated to be 2.0 ± 0.1 mM (n = 3, assuming a myocyte volume of 10 pL), consistent with the normal values obtained from single healthy aerobic cells.26 In the future, this format will be used to monitor intracellular lactate released from the beating cell for different metabolic models, including those of hypoxia and ischemia, in order to provide a better understanding of the role of lactate in the control of both intracellular pH and cell metabolism.
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Fig. 8 (a) Myocyte contractility measured as the change of the sarcomere length within the chamber when stimulated at electrical field strengths of 75 V cm−1 at 1.0 Hz. Single representative transients from a continuous record are shown. The values on the right-hand side represent the period from the development of steady-state shortening. (b) Recordings of extracellular pH during continuous contraction with field strength of 75 V cm−1 and a frequency of 1.0 Hz (as indicated through vertical bars which mark the point of electrical stimulation), using semi-quantitative single wavelength fluorescence of BCECF. (c) Simultaneous recording of cell contraction with a field strength of 75 V cm−1 and a frequency of 1.0 Hz, using edge detection measurement. |
The extracellular pH was monitored during 20 min of continuous cell contraction using semi-quantitative single wavelength fluorescence of BCECF, Fig. 8(b) and (c). Considering that there was no electrolysis acidification within the microchamber at the field strengths used, Fig. 5, we expect the acidification of extracellular space to be caused by efflux of lactate into the extracellular space. When glycolysis proceeds anaerobically, lactate acid production increases dramatically and accumulates within the intracellular space. Raised lactate and a fall in intracellular pH stimulate the lactate transporter that co-transports lactate and a proton. This electroneutral transport leads to the efflux of lactic acid from the cell which dissociates and acidifies the extracellular space.27 Data with cells equilibrated with the mitochondrial inhibitor CN− (as a model for ischemia) indicated that lactate acid production was considerably increased. Not only was the extracellular pH lower than control conditions, but the lactate signal after electroporation was ∼10× larger than the control (mean concentration of lactate = 18 mM). Detailed experimental studies showing the efflux of lactate into the extracellular space, either using field stimulated cells or by using a model for ischemia, where the cell’s glycolytic pathways are uncoupled using CN−, will form the basis of a further publication.
Finally, it was noted that the acidification of intracellular or extracellular space could also lead to a fall in the cell’s contractility. Renewal of the buffer balances the falling pH of the extracellular space, and thus the contractility partially recovers (to 60% that at rest), Fig. 8(a). The quantitative measurement of intracellular and extracellular pH during continuous stimulation will also be investigated in future studies to advance our understanding of the acidification mechanism.
The experiments described above, although technically exacting, typically allowed single cell measurements to be made every 30–60 minutes. In order to improve the rate of data acquisition in future we are currently developing an array sensor based upon our previous experience in multi-chamber microfluidic measurements.24
This journal is © The Royal Society of Chemistry 2006 |