Lisandro Cunci*ab,
Marina Martinez Vargasac,
Roman Cuncid,
Ramon Gomez-Morenoac,
Ivan Perezab,
Abel Baerga-Ortizac,
Carlos I. Gonzalezace and
Carlos R. Cabrera*ab
aMolecular Sciences Research Building, University of Puerto Rico, 1390 Ponce de Leon Ave., STE. 2, San Juan, Puerto Rico 00926-2614, USA. E-mail: lisandro.cunci@upr.edu; carlos.cabrera2@upr.edu; Fax: +1-787-522-2150; Tel: +1-787-523-5319
bDepartment of Chemistry and Center for Advanced Nanoscale Materials, University of Puerto Rico, Río Piedras Campus, P.O Box 23346, San Juan, Puerto Rico 00931-3346, USA
cDepartment of Biochemistry, University of Puerto Rico, Medical Sciences Campus, P.O. Box 365067, San Juan, Puerto Rico 00936-5067, USA
dDepartment of Computer Engineering, Buenos Aires Institute of Technology, Av. Eduardo Madero 399, C1106ACD, Buenos Aires, Argentina
eDepartment of Biology, University of Puerto Rico, Río Piedras Campus, P.O. Box 23360, San Juan, Puerto Rico 00931-3360, USA
First published on 15th October 2014
The enzyme telomerase is present in about 85% of human cancers which makes it not only a good target for cancer treatment but also an excellent marker for cancer detection. Using a single stranded DNA probe specific for telomerase binding and reverse transcription tethered to an interdigital gold electrode array surface, the chromosome protection provided by the telomerase was replicated and followed by electrochemical impedance spectroscopy as an unlabeled biosensor. Using this system designed in-house, easy and affordable, impedance measurements were taken while incubating at 37 °C and promoting the probe elongation. This resulted in up to 14-fold increase in the charge transfer resistance when testing a telomerase-positive nuclear extract from Jurkat cells compared to the heat-inactivated telomerase-negative nuclear extract. The electron transfer process at the Au electrodes was studied before the elongation, at different times after the elongation, and after desorption of non-specific binding.
Cancer cell biosensors have been one of the main topics in the scientific literature during the last few years.4–8 Their potential use at the point of care can translate into an early onset of treatment that may change the prognosis of the patients. Several biosensors for the detection of telomerase as a cancer marker have been reported within the last few years,6,7,9–12 and two recent reviews.13,14 The most promising biosensor platforms that specifically detect telomerase rely on the principle of the elongation of single stranded DNA probes with specific sequences,15 such as 5′-TTAGGG-3′ for vertebrates. Using this principle, many electrochemical telomerase biosensors have been reported using differential pulse voltammetry,16–19 electroluminescence,20,21 and chronocoulometry,22,23 with only one that uses electrochemical impedance spectroscopy (EIS) for a dual purpose: for surface characterization and as the biosensor signal transducer.24
There are numerous advantages of using EIS in biosensor design, such as high sensitivity25,26 accuracy, rapid detection, compatibility with microfabrication technology27 and real-time measurements.28 In the detection of telomerase, EIS has been used in one instance24 where a ssDNA oligomer probe was tethered to the surface of a gold disk electrode, followed by incubation of the electrode in a HeLa cell extract for several hours. Then, the electron transfer reaction of the ferricyanide/ferrocyanide redox couple was measured in a different buffer by EIS, and the electron transfer resistance was correlated to the elongation of the probe. However, these reported biosensor configurations only considered the ferricyanide/ferrocyanide redox reaction and none have taken advantage of the vast diversity of molecules already in total/nuclear cell extracts and buffer solutions.
In this work, we designed easy software and constructed hardware for an in situ incubation while detecting the presence of the telomerase enzyme as a cancer marker by taking advantage of its reverse transcriptase activity measured in real time. For these experiments, we used Jurkat T cells which have been useful in studies of Telomerase activity regulation and in understanding the mechanisms of differential susceptibility of several cancers to radiation and other treatments.29–31 A nuclear extract from Jurkat cells in the absence of an additional redox couple was used as the telomerase-positive sample, and a solution heat-treated at 95 °C to inactivate the telomerase enzyme as the control. This work focused on the development of a proof-of-concept, straightforward detection of telomeric activity in under 20 minutes with a robust, powerful and scalable method, using an interdigital biosensor microchip and avoiding the need of a reference electrode. We propose this system as a step towards inexpensive and faster cancer detection at the point of care.
The hardware was designed to be easy to implement and inexpensive. Our temperature controller was built with commercially available components in a way that would allow any user to make their own with off-the-shelf components. A scheme of the circuit is presented in Fig. SI2,† and most elements may be obtained as samples for testing from each manufacturer. The circuit was soldered by hand and an explanation of how it functions is provided in the ESI.† We avoided the use of Labview and costly equipments for something as simple as temperature control for in situ incubation. On the other hand, we used a potentiostat for accurate EIS measurements but simple impedance measurement circuits can be modified to work with this system while reporting to the same software.
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| Fig. 1 (a) Procedure for the tethering of the TS probes and (b) the mechanism responsible for the expected change in the impedance during incubation at 37 °C. | ||
000× GelRed (Biotium) to visualize DNA under UV light at a wavelength of 302 nm. The agarose gel was placed in the electrophoresis chamber (BioRad) followed by adding 1× TAE buffer until the gel was completely submerged. DNA samples were prepared by mixing 15 μL of DNA with 1.5 μL of 5× nucleic acid sample loading buffer (BioRad). Each DNA sample was placed in its appropriate well, and run at 100 V (constant) for 40 minutes.
The accuracy in temperature measurement during detection in real time is very critical. Thermocouples, thermistors and other commercially available temperature sensors are covered with a packaging that delays precise temperature measurements resulting in inaccurate values, and have different thermal properties, which may result in unknown steady-state temperatures. Moreover, the delay due to the volumetric heat capacity can prevent rapid changes in temperature required for accurate control.
Each of the two electrodes of the interdigital microarray connected to the external pins are used for impedance measurement. The impedance was measured in a two electrode configuration, with the working electrode connected on the left electrode and the counter and reference electrodes together connected on the right electrode.
A support system was built for the microchip shown in Fig. 2 (Panels b, c, and d). Fig. 2 (Panels b and c) show the two aluminum sheets placed firmly together with screws and nuts, with a 1′′ dia. silicone flexible heater used for rapid changes in temperature (All Flex, Inc.) in contact with the biosensor microchip, which provides a fast temperature response. The reaction chamber was built using a rubber O-ring that enclosed the microelectrode sensor array with a glass slide on top. The volumetric capacity depends on the size of the O-ring, commonly being close to 20 μL. Even though 37 °C does not promote fast evaporation, since we used a few microliters, we found out that the reaction chamber was required in order to prevent solution evaporation during the experiments and further change in concentration. A clear scheme of the setup is shown in Fig. 2d.
The design of the IDA microchip electrode maximizes the interaction between the electrodes.35,36 An IDA was designed with a finger width of 10 μm and a separation of 5 μm between the fingers. After construction, the finger width was ca. 10.5 μm and the separation between the fingers ca. 4.5 μm. A scanning electron microscope (SEM) image of the IDA is shown in Fig. 2e and a close-up image in Fig. 2f. The theoretical area of each electrode was designed to be ca. 4.5 mm2, and the perimeter of closest contact at 52 cm.
First, the IDA was treated with piranha solution to clean all organic materials left from the photolithography process. Then, we used CV at 100 mV s−1, from 0.3 V to 1.5 V vs. Ag|AgCl in 0.5 M H2SO4 to verify that the gold surface was cleaned and both electrodes were homogenous in surface area. The TS probe was tethered to the gold surface as explained above, and the electrodes were used the same day that were modified. The sensors were maintained at 37 °C with our temperature controller and a measurement was taken every 5 minutes with the potentiostat. The open circuit potentials between the two electrodes before starting the experiments were less than or equal to 0.02 V. The impedance measurements were conducted from 1 MHz to 0.1 Hz, with a voltage amplitude of 10 mV at a fixed voltage of 0.00 V between the two electrodes. Between measurements, the electrodes were left at open circuit to avoid any electron transfer.
Nyquist plots were used to compare the EIS measurements of the biosensor IDA microchip with the telomerase-positive and telomerase-negative nuclear extracts as shown in Fig. 3a and b, respectively. Both electrodes showed Voigt circuits with at least three reactions obtained from three peaks seen in the phase curve in the Bode plots (data not shown). This may be due to at least three different reactions, or more than one reaction occurring at both electrodes with different chemical kinetics. These reactions are provided by the vast compounds between the buffer C used for the nuclear extraction, and the nuclear extract itself, without the need of an external labeling agent. These results are consistent with a two electrode system where both electrodes are similar (although never equal) and differ, even slightly, from each other in their surface properties. In these Nyquist plots, only the reaction at the lowest frequencies is appreciated, which is the most affected by telomerase binding and elongation, and has the slowest kinetics. Analyzing this reaction, it is clear from these plots that both electrodes experience significant changes in impedance in less than 20 minutes. Fig. 3a and b showed half circles expanding with time, and means that the charge transfer resistance (Rct) is increased. Rct is correlated to the diameter of the half circle, and it is easily seen in these graphs that the increment in the diameter is larger for the telomerase-positive solution compared to the telomerase-negative solution. This increase can be analyzed quantitatively by modeling the data and plotting the change in percentage with regard to the initial measurement.
Fig. 3c shows Rct calculated with the FRA Software (Autolab) versus time. Modeled with an asymptotic exponential equation (black line), the change in Rct is significant in only 20 minutes. The telomerase-positive as well as the telomerase-positive samples showed changes in Rct with time, however, these changes are significantly different when analyzed as a change in percentage compared to the initial measurement. The change in Rct in the telomerase-negative sample may be attributed to different reasons such as chemical changes in the solution and surface that occurred at 37 °C as well as temperature stabilization, that are also occurring at the telomerase-positive electrodes. For example, even though the O-ring provides a very good seal we may not prevent complete evaporation, which in turn changes the electrolyte concentration with time. Not only evaporation, but also, non-specific adsorptions can impact greatly the change in impedance. Since both electrodes experienced similar changes, we can attribute the difference in Rct vs. time to the elongation of the TS primer tethered to the IDA electrode surface.
These two electrodes differ in their absolute values due to variability in the construction and modification process. To verify these results, we repeated these experiments using a similar electrode but performing an additive experiment. We tested 10 μL of the heated control solution in our biosensor IDA microchip, and after 20 minutes, we added 10 μL of Jurkat nuclear extract solution with a total protein concentration of 763 μg mL−1. Fig. 3d and e show the Nyquist plot and the percent change in Rct with time, respectively. Again, the results follow a Voigt circuit with phase peaks similar to the electrodes discussed previously, and the diameter of the half circle increases with time, due to the elongation of the surface tethered primer TS. The percent change in Rct stays below 10% until 20 minutes where the telomerase-positive solution was added, and it raises up to ca. 45% in 15 minutes.
The tethering and elongation of the TS probe due to telomerase binding and reverse transcription with the reversibility of the electron transfer process at the Au surface was studied by cyclic voltammetry (CV). The CV was conducted in a 3 electrode system with both electrodes of the biosensor microchip used as the working electrode, a Pt wire as counter and Ag|AgCl as reference electrodes. A solution of 0.1 M PBS with 0.1 M KCl at pH 7.0, 1 mM of K3Fe(CN)6 and 1 mM K4Fe(CN)6 was used for the CV studies. Fig. 4 (Panels a, b and c) show the CV for Au, Au–TS, and Au–TS-elongated for 20 minutes at 37 °C with the telomerase-positive solution, respectively, from 10 to 300 mV s−1 in scan rates. Fig. 4d shows the CV for Au–TS-elongated after 4 months at room temperature in contact with telomerase-positive solution in a humidity saturated enclosure to avoid evaporation. Fig. 4e shows the CV for Au–TS-elongated (long time) for 4 months and stripped using 20 μL of 0.1 M PBS solution and chronoamperometry for 2 min at 1.3 V.37 This voltage was applied using one of the two IDA electrodes as working electrode, and connecting the second IDA electrode to the reference and counter electrode cables together. Prior to the experiments, these electrodes were washed thoroughly with nanopure water and 0.1 M PBS solution. These CV differentiate clearly in the shape of the oxidation and reduction peaks while after 4 months at room temperature the peaks are not detected for several scan rates. From these CV, the separation of the oxidation and reduction peaks (ΔEp–p), and the oxidation and reduction peak currents, iox and ired, respectively, were plotted versus the square root of the scan rates (v1/2) in Fig. 4 (Panels from f, g and h).
First, ΔEp–p decreases after the formation of the SAM compared to the clean gold electrode that is attributed to a more reversible electron transfer process due to faster kinetics. It is known that ssDNA has isoelectric point of 4.0–4.5 (ref. 38) with a negative charge when exposed to a pH 7.0 solution, and ferricyanide and ferrocyanide have negative charge which may suggest a slower electron transfer. However, we observed faster kinetics and enhanced reversibility as seen by L. Qingwen et al.39 when using a SAM of L-cysteine at Au and I. Feliciano-Ramos et al.40 when having a SAM of L-cysteine at Pd electrodes. Both groups worked at pH 7.0 and, although the carboxyl group has a negative charge, they attribute the enhanced reversibility to the local positive charge density of the amine. Therefore, even though TS has a net negative charge density, the localized positive charge densities of the amine groups may help the electron transfer process when the ssDNA is short enough, improving the reversibility as observed in our data. However, the reversibility of the electron transfer process in TS post-elongation, Fig. 4f, was affected by the increase of the ΔEp–p after 20 minutes in contact with the telomerase-positive solution. Compared to TS pre-elongation, the increment from 59 mV at 10 mV s−1, and 85 mV at 300 mV s−1, to 70 mV and 94 mV, respectively, is due to two mechanisms responsible for biosensing: (1) the telomerase binding to the TS probe and (2) the elongation of the TS probe at the electrode surface. In addition, the iox and ired peak currents were affected not only decreasing but also deviating from the linearity versus v1/2 as observed in the TS pre-elongation biosensor. This deviation from linearity at higher scan rates can be associated to a slower electron transfer process due to the blocking effect provided by the telomerase binding to the TS probe and its elongation.
After 4 months at room temperature, ΔEp–p increased dramatically not only due to the elongation but also probably due to non-specific surface interactions produced by the degradation products of the nuclear extract components. We applied a voltage of 1.3 V between the two electrodes during 2 min to desorb these species, and then, the connectors were swapped and the electrode used as working electrode was used as reference/counter electrode and vice versa, and 1.3 V was applied again for 2 min.37 The 20 μL PBS solution from the first and the second chronoamperometry, and a solution of the TS probe were used in an agarose gel electrophoresis (AGE) separation study. The results are shown in Fig. 5 next to the 10 kb DNA ladder. In the first column, we observed degradation fragments which were adsorbed to the electrode surface before the stripping procedures. In the second column, the absence of a line confirms that at least the majority of the adsorbed species were stripped from the electrode. In the third column, we observed one line at the bottom corresponding to the TS probe. The biosensor microchip after the stripping process should have a surface covered mostly by the elongated TS probe, as nothing else was observed in the second column of the AGE. After the chronoamperometry, the electron transfer process was faster with better reversibility as depicted in Fig. 4f (pink), shown by a decrease on the ΔEp–p, an increase in iox and ired, and a iox/ired peak current ratio closer to 1, as shown in Fig. 4 (Panels g and h, blue).
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| Fig. 5 Agarose gel electrophoresis of the non-binding species that were removed after the 1st and 2nd potentiostatic desorption at an applied voltage of 1.3 V between interdigital electrodes for two minutes, together with TS probe control and a 10 kbp DNA standard ladder reference, stained using GelRed. This was done adapting a procedure presented by J. Wang et al.37 | ||
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c4ra09689d |
| This journal is © The Royal Society of Chemistry 2014 |