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Self-Powered Potentiometric Sensors with Memory
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ACS Sensors

Cite this: ACS Sens. 2021, 6, 10, 3650–3656
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https://doi.org/10.1021/acssensors.1c01273
Published September 28, 2021

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Abstract

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Potentiometric sensors induce a spontaneous voltage that indicates ion activity in real time. We present here an advanced self-powered potentiometric sensor with memory. Specifically, the approach allows for one to record a deviation from the analyte’s original concentration or determine whether the analyte concentration has surpassed a threshold in a predefined time interval. The sensor achieves this by harvesting energy in a capacitor and preserving it with the help of a diode. While the analyte concentration is allowed to return to an original value following a perturbation over time, this may not influence the sensor readout. To achieve the diode function, the sensor utilizes an additional pair of driving electrodes to move the potentiometric signal to a sufficiently high base voltage that is required for operating the diode placed in series with the capacitor and between the sensing probes. A single voltage measurement across the capacitor at the end of a chosen time interval is sufficient to reveal any altered ion activity occurring during that period. We demonstrate the applicability of the sensor to identify incurred pH changes in a river water sample during an interval of 2 h. This approach is promising for achieving deployable sensors to monitor ion activity relative to a defined threshold during a time interval with minimal electronic components in a self-powered design.

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Copyright © 2021 The Authors. Published by American Chemical Society
Potentiometric measurement tools occupy a significant portion of the sensor market due to their simple underlying operation principle. (1,2) Ion-selective electrodes (ISE) are a dominant class of these sensors and are used for detecting pH and various analytes of interest, especially in healthcare and environmental sectors. (3,4) pH probes and other ISEs routinely show lifetimes on the order of months, (1,5) even when measured in highly complex samples. In the simplest configuration, so-called direct potentiometry, the potential induced by the ISE is a direct indicator of the analyte activity. As this spontaneous response requires no power source, they become potential candidates for developing energetically autonomous, or self-powered sensors.
Self-powered sensors omit external power sources and achieve detection by solely utilizing the harvested energy from their operation. (6−8) As a result, they integrate a two-fold approach by dealing with aspects related to both detection and energy. Usually, such an integration is possible by exploiting the sample under investigation to provide the required energy for sensing. A large proportion of self-powered electrochemical sensors have resulted from this approach, primarily in the field of biosensors (using biofuel cells and battery systems), where the analyzed sample induces a redox reaction across electrodes to produce a galvanic cell. (9) Often, the use of enzymes, organelle substrates, and microorganisms have helped to achieve amperometric operation of self-powered sensors for detection of analytes such as glucose, lactate, cholesterol, ethanol, toxins, and biological oxygen demand. (10−15) The electrical signal generated from these redox reactions serves either directly as the indicator of the sensor response or is further processed to other output forms. (16)
Because potentiometric sensors are usually read out at nearly zero-current conditions, self-powered approaches can only be conceived by subjecting the sensor to a transient state where it supplies a transient current. To achieve such a transition, the sensor may take advantage of a capacitive element. For instance, in the presence of an external power source, coulometric sensors accumulate charge across a capacitive element owing to a transient current generated in the process of the system attaining a new equilibrium state. Chemical substrates such as polymer films and electronic capacitors proved to be useful in realizing electric and optical readout of ions using this transduction principle. (17−20) Based on these developments, we recently demonstrated a self-powered version of a potentiometric sensor by placing a capacitor directly between the indicator and reference probes. (21) The induced potential difference across the probes generated a transient current flow and charged the capacitor to nearly the open-circuit voltage. As a result, no high-end instruments were necessary because the capacitor voltage could be read out later with a simple hand-held multimeter to reveal ion activity. This is different from the constant potential coulometric method of ion-sensing where the measured current transient observed over a time period allows for one to achieve a better resolution in ion activity measurements. (22,23) Instead, this approach aims to obtain only a single value of capacitor voltage, as in a traditional potentiometric principle. Here, the capacitor serves as a memory element and the existence of a transient current in the circuit is due to the nature of the element and is not the parameter of interest.
In the approach discussed above, the induced voltage in the potentiometric sensor corresponds to the state of analyte at the actual time of measurement or disconnection from the cell. For monitoring analyte concentration during a certain interval, these sensors would require sophisticated supplementary electronics. This would demand a substantial voltage and power that are often not available with potentiometric sensing probes to make the complete sensor self-sufficient in operation. Recent developments in galvanic bipolar electrochemical methods involving cascading strategies can prove to be useful to push the response voltage higher. Typically, a bipolar electrode is an electrically conducting element that undergoes faradaic reactions to develop a potential difference between its ends on applying a suitable voltage across it. A pair of driving electrodes that are connected to an external power source usually provides this voltage without actually establishing a physical contact with the bipolar element in an ionic medium. (24) Alternatively, an electrochemical system can achieve a similar potential difference through oxidation–reduction reactions (or with any electron-exchange process) at separate electrodes that are electrically short-circuited. In this case, the process becomes spontaneous and thereby involves no driving electrodes. However, by incorporating an additional pair of driving electrodes (connected to an external power source) in these systems, the induced potential difference can be further modulated in magnitude. In fact, a cascade of two bipolar electrode systems can eliminate the dependency on an external power source, with one of them driving the other through the generated induced voltage. (25) Note, however, that many of these systems continuously draw a substantial steady current due to the short-circuited sensing electrodes and may quickly affect the sensor stability during prolonged operation.
We present here a self-powered potentiometric ion sensor capable of tracking perturbations in ion activity over time to reveal the deviation of analyte concentration from its original value (Scheme 1). The sensor uses a four-electrode configuration where a pair of driving electrodes exhibit a sufficiently large potential to shift the potentiometric signal to a sufficient voltage for operating a basic diode. In the absence of the diode, the capacitor voltage at a specific measurement point in time misses the information about any prior concentration fluctuations. However, by introducing the diode, the capacitor charges based on the transient current that is allowed by it. Importantly, when the analyte concentration returns to its original value, the diode prevents the discharge of the capacitor. In this manner, the measurement of the capacitor voltage at a single time point may reveal important fluctuations in the ion concentration without requiring to perform a continuous measurement. We demonstrate a sensor application for tracking pH variation for a duration of 2 h in a river water sample. The current sensing approach integrates the memory effect in a potentiometric sensor with minimal electronic components that operate in a self-sufficient manner.

Scheme 1

Scheme 1. Schematic Illustration of the Approach Adopted to Track a Deviation in the Activity of an Analyte During a Time Interval by Reading Out the Response Stored in a Capacitor at a Specific Measurement Point in Time

Experimental Section

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Materials

Potassium chloride (KCl), hydrogen ionophore I, poly(vinyl chloride) (PVC) (high molecular weight), 2-nitrophenyloctylether (o-NPOE), sodium tetrakis[3,5-bis(trifluoromethyl)phenyl]borate (NaTFPB), tetrakis(4-chlorophenyl)borate tetradodecylammonium salt (ETH 500), tetrahydrofuran (THF), sodium chloride (NaCl), boric acid, zinc chloride (ZnCl2), phosphoric acid, and acetic acid were purchased from Sigma-Aldrich.
Hydrochloric acid (HCl, Thermo Fisher Scientific) and sodium hydroxide (NaOH, Alfa Aesar) were used as purchased. All experiments were performed with deionized water (resistivity > 18 MΩ cm) at room temperature. 10 μF metallized polyester capacitors (WIMA) and ESD Suppressors/TVS Diodes (PESD5Z3.3,115) were purchased from Distrelec, Switzerland, and Mouser Electronics.

Sample Preparation

Universal buffer solution was prepared by a mixture of phosphoric acid, acetic acid, and boric acid. NaCl and KCl solutions were prepared with the respective salts using deionized water. River water samples were collected from Arve river in Geneva, Switzerland.

Electrodes

Double junction Ag/AgCl (3 M KCl/1 M LiOAc), single junction Ag/AgCl (3 M KCl), and Pt electrodes were purchased from Metrohm, Switzerland. Zn electrodes (of diameter 1 mm, 99.995% trace metals basis) were obtained from Sigma-Aldrich.
Ag/AgCl electrodes were made by electrochemical oxidation of an Ag electrode (of diameter 3 mm, order no. 6.1204.330, Metrohm, Switzerland) using a similar procedure described in our previous work. (21)
A H+-selective membrane was prepared by dissolving a mixture made up of 58.36 mg of PVC, 116.73 mg of o-NPOE, 0.90 mg of NaTFPB, 20.67 mg of ETH 500, and 3.33 mg of hydrogen ionophore I in 2 mL of THF. The dissolved solution was cast into a glass ring (of inner diameter 22 mm) attached to a glass slide and was left overnight to form a membrane. A circular piece of the membrane (diameter 8 mm) was then loaded into the ISE body (Oesch Sensor Technology, Sargans, Switzerland) with an inner filling solution comprising 10 mM universal buffer (at pH 7) and 10 mM NaCl to obtain H+-ISE. The H+-ISEs were conditioned overnight in a solution, similar to the composition of inner filling solution.

Sensor Configuration

The sensor contains two separate compartments (of diameter 5.5 cm) to place the reference and sample solutions. The reference compartment contained 50 mL of 100 mM ZnCl2 solution (pH 2.6). On the other hand, the sample compartment featured 50 mL of solution containing 10 mM universal buffer and 10 mM NaCl. Zn and Ag/AgCl electrodes were immersed in the reference solution. The H+-ISE and Ag/AgCl (3 M KCl) electrodes were placed in a sample compartment. The separation between electrodes in each compartment is 2.5 cm (center to center). The connection between the compartments is established by making an electrical contact between the electrodes. While the Zn and Ag/AgCl (3 M KCl) electrodes were directly connected to each other, the Ag/AgCl and H+-ISE were connected through a DIP (dual in-line package) switch, diode, and capacitor.
For certain experiments, the solutions and the electrodes were modified. These were mentioned in the text wherever appropriate.

Sensing Measurements

The circuit connection, or activation of the sensor is made using a DIP switch. During sensing measurements, the concentration of the reference solution is kept constant. Small and defined changes in pH of the sample solution were made using 1 M HCl and 1 M NaOH solutions. The voltage measurements of the sensor components (capacitor and electrodes) were carried out with EMF16 data acquisition system (input impedance of ∼1013 Ω; Lawson Labs, Inc., Malvern, PA).
In certain experiments, a source meter (Keithley 2450) was used to supply voltage across the electrodes. We mentioned this at appropriate places in the text.

Results and Discussion

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The approach adopted to detect a deviation occurring in activity of an analyte during a predefined time interval without requiring continuous monitoring is illustrated in Scheme 1. The sensor system uses two compartments containing two electrodes, each electrically connected in a closed bipolar electrode configuration. The sample compartment contains the ISE, E1, selectively responsive to the analyte, along with the reference electrode E2, as in a traditional measuring cell. The second compartment contains a driving electrode E3 and a second reference element E4 in a solution whose composition is known and constant. Typically, the potential between the indicator and reference electrodes produces a potentiometric response for the analyte ion activity in the sample in analogy to classical measurements. However, the response relevant to this sensing approach is the induced voltage between electrodes E1 and E4. Therefore, in the absence of electrodes E2 and E3 that form the driving circuit, the ISE response can be obtained against the electrode E4 by establishing a salt bridge connection. Further, this response can be transferred to a capacitor by connecting it across these electrodes in a self-powered manner. (21) However, the incorporated two additional electrodes (E2 and E3) in the present work act to increase this response signal by a voltage increment, given by the asymmetry of the driving and reference electrode pair. Because these additional electrodes work by utilizing the resources already available in the original system, the system may be considered self-powered. (25) In this configuration, the open circuit potential difference (Ecell = −Ve) for the entire cell can be expressed as
(1)
where E1, E2, E3, and E4 are the potentials at the respective electrodes mentioned above. Hereafter, to explain the circuit behavior, a positive voltage Ve is referred to denote an open circuit voltage as it represents Ecell with an opposite polarity.
A capacitor can be charged to this induced potential difference, Ve, when connected as the only circuit element between E1 and E4 according to the relation
(2)
where Vc is the voltage across the capacitor with a capacitance C and i is the current flowing through the closed circuit over time t during the charging process. This strategy allows one to capture the charge redistributed upon the transient electrochemical imbalance in the capacitor, which acts as an energy storage element that can be read at any time. The voltage built up across the capacitor thereby remains a direct function of the cell potential with time. Because of this, the capacitor cannot retain information about past events but reflects the potential at the time of readout or disconnection from the cell.
To overcome this, the circuit may be endowed with a concentration memory by introducing a diode in series with the capacitor. In that case, the voltage Vc does not rapidly assume the value of the steady-state open-circuit voltage, Ve, because the diode now dictates the charging behavior of the capacitor. To illustrate this, the typical current–voltage characteristics for a unidirectional diode is shown in Figure S1. The curve can be explained with the help of a Shockley ideal diode equation (eq 3) that exponentially relates the voltage across the diode, Vd, with the current, i, flowing through it.
(3)
where is is the reverse bias saturation current (typically less than 1 nA) observed at Vd < 0. η is the ideality factor (or emission coefficient) that accounts for recombination of charge carriers. Its value for an ideal diode is 1, but it usually varies between 1 and 2 depending on the operating conditions, physical construction, and the involved fabrication process. VT = kT/q = 25.69 mV (at 25 °C) is the thermal voltage, with k being the Boltzmann constant, T being the absolute temperature, and q being the elementary charge.
As indicated by the significant exponential term in eq 3, the diode conducts with a very low resistance at higher voltages to allow for a substantial current (Figure S1a,b). However, at low voltages, the exponential term becomes negligibly small, and the current is approximately equal to is. The diode therefore becomes more resistive and almost ceases the current flow at lower voltages. For instance, for an input voltage appearing across the circuit containing a diode and capacitor connected in series, a transient current prevails. This is an advantage, as significant current is not drawn from the system continuously, which otherwise would happen if the sensing electrodes were short-circuited or connected through a low-value resistor. Because the capacitor voltage is low initially, the diode experiences almost the input voltage and offers a very low resistance. As a result, the response time is quicker at this moment due to a very low time constant to charge the capacitor. However, as time progresses, the gradual increase in capacitor voltage causes a decrease in voltage across the diode. This eventually leads to a longer response time due to a larger time constant by virtue of the diode becoming highly resistive (Figure S1c). This behavior makes the diode to allow for current flow only in one direction, that is, when the voltage across it is sufficiently high. As a result, upon activating the sensor in Scheme 1 by closing the switch S1, the capacitor initially charges quickly owing to a less resistive diode. With time, however, the gradual buildup of Vc results in a decreasing voltage across the diode (Vd = VeVc). The diode starts to provide a high resistance for charging the capacitor further. Importantly, the diode allows for the capacitor to maintain its charge even when Ve is found to decrease again. This is driven by its ability to restrict current in the reverse direction.
Before establishing the pH sensing system as described in Scheme 1, the effect of driving circuit was evaluated using an initial model system with symmetrical reference elements that was driven by an external applied voltage. It comprised four identical Ag/AgCl electrodes placed in two separate solutions containing 100 mM KCl each (Figure 1a). On applying a bi-directional staircase signal from 0 to 1 V in steps of 100 mV with a step time of 10 s to the driving electrodes (E2, E3), the observed potential difference between the other two electrodes in the sensing circuit is found to have the same value (Figure 1b). This result shows that the electrodes forming the detection circuit experience an additional voltage whose value corresponds to that between the two driving electrodes. Importantly, this behavior was not altered by the insertion of a capacitor between the electrodes in the sensing circuit. Instead, the circuit charged the capacitor to a voltage equivalent to the value between the electrodes. Here, the RC time constant for the capacitive element was on the order of 50 ms, sufficiently small in the time scale of the experiment to not appreciably alter the time response of the potential readings. The use of ion-selective membranes of high resistance may result in larger values.

Figure 1

Figure 1. (a) Model system to study the influence on the capacitor connected between indicator and reference electrodes due to a voltage applied across the driving electrodes. (b) Measured voltages for an applied bi-directional staircase signal.

The capability to influence the voltage across the electrodes in the sensing circuit with the help of two independent driving electrodes may be used to shift the level of the potentiometric signal obtained conventionally in the measurement compartment. This was demonstrated with an electrochemical sensing cell for the measurement of pH for its wide practical applicability and because sample acidity can be reliably changed in a very wide range. For sensing pH, electrode E1 was replaced with an H+-ISE while keeping the other electrodes as Ag/AgCl elements, using 10 mM universal buffer and 10 mM NaCl solution for the sample and 100 mM KCl for the reference solution (Figure 2b). The pH probe gave a Nernstian response against a double junction Ag/AgCl (3 M KCl/1 M LiOAc) electrode as confirmed in separate experiments (Figures 2a and S2). For an applied external voltage of 0.9 V between the driving electrodes, the acquired voltage response for pH was shifted by this value relative to measurements against a double junction Ag/AgCl electrode, but still showed a Nernstian behavior (Figure 2c). The opposite slope for pH shown in Figure 2c (when compared to Figure 2a) comes from presenting the voltage with reference to ISE as denoted in the circuit (Figure 2b). On reversing the polarity of the applied voltage, a difference of −0.9 V in measured voltages was equally observed from conventional potentiometric measurements.

Figure 2

Figure 2. (a) Response of H+-ISE against a double junction Ag/AgCl (3 M KCl/1 M LiOAc) electrode. (b) Model system involving an external power source to shift the level of a conventional potentiometric signal and to a charge a capacitor to the translated voltage. (c,d) Voltage across capacitor at different pH values for an applied voltage of 0.9 and −0.9 V, respectively, between the driving electrodes.

So far, a source meter provided the required voltage across the driving electrodes for imposing the voltage levels in the response curves. To eliminate the dependence on external power sources while shifting the level of response voltage, a potential difference between driving electrodes was induced electrochemically. The modified system contained a Zn electrode as E3 is immersed in a 0.1 M ZnCl2 reference solution at pH 2.6 (Figure 3a). In this configuration, a Nernstian response for pH with a potential shift of ∼1.065 V relative to the potentiometric measurement with a double junction Ag/AgCl (3 M KCl/1 M LiOAc) electrode was observed (Figure 3b). This shift is due to the asymmetry induced by the Zn electrode E3, which acts in some analogy to the voltage applied with an external source meter. As shown in Figure 3b, the voltage response again remained identical when a capacitive element was introduced between electrodes E1 and E4. Importantly, the Zn electrode remained stable during the pH measurement for at least 17 h within a variation of ±1 mV when monitored against a double junction Ag/AgCl electrode (Figure 3c).

Figure 3

Figure 3. (a) pH sensing configuration without an external power source to shift a potentiometric signal and to store the response by charging the capacitor. (b) Response of the sensor at different pH values in open circuit and with a capacitor. (c) Stability of Zn electrode over time.

The capacitor in the circuit (Scheme 1) is initially in a discharged state. On activating the sensor by closing switch S1, Ve aims to approach the open-circuit voltage. Because the initial capacitor voltage is zero, the diode offers a very low resistance because the potential across this circuit element is close to Ve. As the capacitor is charging in the process of approaching Ecell, the voltage across the diode is continuously decreasing, making the diode more resistive and increasing the charging time of the capacitor. The evolution of Vc at different pH sample values is shown in Figure 4a. Within a measurement period of 600 s, there is a clear distinction in the time evolution of Vc for different pH values.

Figure 4

Figure 4. (a) Voltage evolution across the capacitor at different pH of the sample. The solid lines represent the capacitor voltage, and the dashed lines indicate the induced voltage, Ve. (b) Response across the capacitor for voltage applied using source meter. The sample is maintained at pH 7. The dashed lines represent the applied voltage, and the solid lines represent the capacitor response. (c) Voltage response of capacitor for pH changes incorporated in a sample (originally at pH 7) to deviate from its initial state. The solid lines represent the capacitor voltage, and the dashed lines indicate the induced voltage, Ve. (e) Voltage across capacitor measured at the end of 2 h using a hand-held multimeter. Here, the river samples are spiked to a higher pH for an abrupt interval of 5 min, before returning it to original value. The second y-axis (Q) in the figure corresponds to the capacitor curves.

Achieving a self-powered memory function is possible if the diode obstructs current flow in reverse direction to preserve the accumulated charge across the capacitive element when Ve returns to baseline potential. To illustrate this, we initially applied a voltage of 148 mV with the source meter in the driving circuit to mimic a pH change of 2.5 in the sample (Figure 4b), while leaving the solutions undisturbed with a sample pH of 7. During a measurement time of 10 min, the capacitor voltage deviated from its normal course observed at pH 7 because of the applied voltage at the indicated intervals. Notably, irrelevant of the time instance at which the voltage change was induced, the capacitor maintained the charge across it until the end of the time period. The longer the duration of the superimposed change, the greater the capacitor voltage owing to the longer charge buildup time. A similar behavior could be observed with smaller voltage changes of 29.6 and 59.2 mV (Figure S3). A single measurement of the capacitor voltage at a specific time point could reveal a prior potential excursion by comparing the value with that obtained for the sample in its original state. In the absence of the approach described here, this information could only be achieved by performing a continuous potentiometric measurement. Based on the data obtained with applied voltages, the sensor behavior was further explored without a source meter, but by imposing intermittent pH changes of either 1 or 1.5 units in the sample (10 mM universal buffer and 10 mM NaCl solution) using the configuration shown in Scheme 1. As shown in Figure 4c, the capacitor voltage deviated from its normal course (observed with sample at pH 7) in a similar manner as with voltages applied using the source meter.
We further applied the sensor to probe for adverse pH changes in water from the river Arve in Geneva. The pH of the river water sample was found to vary between 8.18 and 8.43 when left in laboratory air for a duration of 2 h. The sensor delivered a capacitor voltage of 0.69735 ± 0.00265 V at the end of 2 h with these samples (Figure 4d). Due to the time variation of pH of river water, the capacitor voltage was found to be less stable in comparison to the value obtained with universal buffer solution (0.685 V at pH 8.18) (Figure S4). Initial experiments superimposed a voltage of 88.8 mV between the driving electrodes using a source meter to mimic an intermittent pH change of 1.5 units. The required shortest duration of this superimposed change is about 3 min to reliably detect the pH change. The difference in measured capacitor voltage was found to exceed ∼9 mV when the duration of applied voltage was at least 5 min (Figure S5). To evaluate the memory function of the circuit during an actual measurement, the river water pH was perturbed with NaOH to introduce a pH variation of about 2.5 for a period of 5 min before returning to baseline. As expected, the capacitor voltage was found to remain distinctively different throughout the duration of the measurement period relative to baseline (Figure 4d). The potential across the Zn electrode when measured against a double junction Ag/AgCl electrode was within ±1 mV (Figure S6). Upon acquiring a single capacitor voltage measurement at the end of 2 h with the help of a simple hand-held multimeter, the sensor revealed the introduced pH perturbations in river water despite returning the sample to the original pH (Figure 4e). In this manner, the capacitor voltage in combination with the diode served as a memory element to recognize that the pH had been altered within the measurement period. The sensor configuration shown in Scheme 1 allows one to track deviations corresponding to pH increments in one direction only. An expansion of the cell components would be required to develop sensors capable of detecting both upper and lower threshold limits.

Conclusions

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The work demonstrates a self-powered potentiometric sensor capable of reporting an output voltage that can reveal deviations in an analyte concentration during a desired time interval. By incorporating a diode alongside an electronic capacitor, it is possible to preserve the harvested energy in the capacitor due to the diode’s ability to restrict the discharge of the capacitor. A measurement at the end time using a simple hand-held multimeter would allow one to identify that the ion activity had increased in the time period of interest. By incorporating a pair of asymmetric driving electrodes, the potentiometric signal can be shifted to a higher voltage, which allows one to operate the diode. Owing to the diode–capacitor combination, no substantial net current is flowing over prolonged time in the sensing circuit, which allows for a high potential stability of all electrodes. Without sophisticated electronics and dependence on external powers sources, the sensor allowed for the detection of a short-lived pH perturbation in a river water sample within a time interval of 2 h. The sensing approach in this work may form the technological basis to achieve a completely self-sufficient potentiometric sensor that could either assess ion activity above a given threshold, for instance in pollution events. It may also be useful for retaining the sensing signal in point of care analytical devices after the underlying measurement step is complete.

Supporting Information

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The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acssensors.1c01273.

  • Details related to diode characteristics, response of H+-ISE, capacitor voltage curves under different conditions, and stability of the Zn electrode (PDF)

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Author Information

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  • Corresponding Authors
  • Author
    • Sunil Kumar Sailapu - Department of Inorganic and Analytical Chemistry, University of Geneva, Quai Ernest-Ansermet 30, CH-1211 Geneva, SwitzerlandInstituto de Microelectrónica de Barcelona, IMB-CNM (CSIC), C/del Til·lers, Campus UAB, Bellaterra, 08193 Barcelona, SpainOrcidhttps://orcid.org/0000-0002-0923-0879
  • Author Contributions

    S.K.S., N.S., and E.B. conceived the idea. S.K.S. and E.B. designed the experiments. S.K.S. performed the experiments. S.K.S. and E.B. analyzed the data. S.K.S., N.S., and E.B. wrote the paper.

  • Notes
    The authors declare no competing financial interest.

Acknowledgments

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The authors acknowledge funding received from the European Union’s Horizon 2020 research and innovation programme under the Marie Skłodowska-Curie grant agreement no. 712949 (TECNIOspring PLUS) and from the Agency for Business Competitiveness of the Government of Catalonia. E.B. acknowledges financial support from the Swiss National Science Foundation. The authors thank Stéphane Jeanneret for his contribution to the work.

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    Sode, K.; Yamazaki, T.; Lee, I.; Hanashi, T.; Tsugawa, W. BioCapacitor: A novel principle for biosensors. Biosens. Bioelectron. 2016, 76, 2028,  DOI: 10.1016/j.bios.2015.07.065
  17. 17
    Jansod, S.; Bakker, E. Self-Powered Electrochromic Readout of Potentiometric pH Electrodes. Anal. Chem. 2021, 93, 42634269,  DOI: 10.1021/acs.analchem.0c05117
  18. 18
    Kraikaew, P.; Sailapu, S. K.; Bakker, E. Rapid Constant Potential Capacitive Measurements with Solid-Contact Ion-Selective Electrodes Coupled to Electronic Capacitor. Anal. Chem. 2020, 92, 1417414180,  DOI: 10.1021/acs.analchem.0c03254
  19. 19
    Han, T.; Mattinen, U.; Mousavi, Z.; Bobacka, J. Coulometric response of solid-contact anion-sensitive electrodes. Electrochim. Acta 2021, 367, 137566,  DOI: 10.1016/j.electacta.2020.137566
  20. 20
    Wang, H.; Yuan, B.; Yin, T.; Qin, W. Alternative coulometric signal readout based on a solid-contact ion-selective electrode for detection of nitrate. Anal. Chim. Acta 2020, 1129, 136142,  DOI: 10.1016/j.aca.2020.07.019
  21. 21
    Sailapu, S. K.; Kraikaew, P.; Sabaté, N.; Bakker, E. Self-Powered Potentiometric Sensor Transduction to a Capacitive Electronic Component for Later Readout. ACS Sens. 2020, 5, 29092914,  DOI: 10.1021/acssensors.0c01284
  22. 22
    Hupa, E.; Vanamo, U.; Bobacka, J. Novel Ion-to-Electron Transduction Principle for Solid-Contact ISEs. Electroanalysis 2015, 27, 591594,  DOI: 10.1002/elan.201400596
  23. 23
    Vanamo, U.; Hupa, E.; Yrjänä, V.; Bobacka, J. New Signal Readout Principle for Solid-Contact Ion-Selective Electrodes. Anal. Chem. 2016, 88, 43694374,  DOI: 10.1021/acs.analchem.5b04800
  24. 24
    Rahn, K. L.; Anand, R. K. Recent Advancements in Bipolar Electrochemical Methods of Analysis. Anal. Chem. 2021, 93, 103123,  DOI: 10.1021/acs.analchem.0c04524
  25. 25
    Jaworska, E.; Michalska, A.; Maksymiuk, K. Self-Powered Cascade Bipolar Electrodes with Fluorimetric Readout. Anal. Chem. 2019, 91, 1552515531,  DOI: 10.1021/acs.analchem.9b03405

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  • Abstract

    Scheme 1

    Scheme 1. Schematic Illustration of the Approach Adopted to Track a Deviation in the Activity of an Analyte During a Time Interval by Reading Out the Response Stored in a Capacitor at a Specific Measurement Point in Time

    Figure 1

    Figure 1. (a) Model system to study the influence on the capacitor connected between indicator and reference electrodes due to a voltage applied across the driving electrodes. (b) Measured voltages for an applied bi-directional staircase signal.

    Figure 2

    Figure 2. (a) Response of H+-ISE against a double junction Ag/AgCl (3 M KCl/1 M LiOAc) electrode. (b) Model system involving an external power source to shift the level of a conventional potentiometric signal and to a charge a capacitor to the translated voltage. (c,d) Voltage across capacitor at different pH values for an applied voltage of 0.9 and −0.9 V, respectively, between the driving electrodes.

    Figure 3

    Figure 3. (a) pH sensing configuration without an external power source to shift a potentiometric signal and to store the response by charging the capacitor. (b) Response of the sensor at different pH values in open circuit and with a capacitor. (c) Stability of Zn electrode over time.

    Figure 4

    Figure 4. (a) Voltage evolution across the capacitor at different pH of the sample. The solid lines represent the capacitor voltage, and the dashed lines indicate the induced voltage, Ve. (b) Response across the capacitor for voltage applied using source meter. The sample is maintained at pH 7. The dashed lines represent the applied voltage, and the solid lines represent the capacitor response. (c) Voltage response of capacitor for pH changes incorporated in a sample (originally at pH 7) to deviate from its initial state. The solid lines represent the capacitor voltage, and the dashed lines indicate the induced voltage, Ve. (e) Voltage across capacitor measured at the end of 2 h using a hand-held multimeter. Here, the river samples are spiked to a higher pH for an abrupt interval of 5 min, before returning it to original value. The second y-axis (Q) in the figure corresponds to the capacitor curves.

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      Jansod, S.; Bakker, E. Self-Powered Electrochromic Readout of Potentiometric pH Electrodes. Anal. Chem. 2021, 93, 42634269,  DOI: 10.1021/acs.analchem.0c05117
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      Kraikaew, P.; Sailapu, S. K.; Bakker, E. Rapid Constant Potential Capacitive Measurements with Solid-Contact Ion-Selective Electrodes Coupled to Electronic Capacitor. Anal. Chem. 2020, 92, 1417414180,  DOI: 10.1021/acs.analchem.0c03254
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      Han, T.; Mattinen, U.; Mousavi, Z.; Bobacka, J. Coulometric response of solid-contact anion-sensitive electrodes. Electrochim. Acta 2021, 367, 137566,  DOI: 10.1016/j.electacta.2020.137566
    20. 20
      Wang, H.; Yuan, B.; Yin, T.; Qin, W. Alternative coulometric signal readout based on a solid-contact ion-selective electrode for detection of nitrate. Anal. Chim. Acta 2020, 1129, 136142,  DOI: 10.1016/j.aca.2020.07.019
    21. 21
      Sailapu, S. K.; Kraikaew, P.; Sabaté, N.; Bakker, E. Self-Powered Potentiometric Sensor Transduction to a Capacitive Electronic Component for Later Readout. ACS Sens. 2020, 5, 29092914,  DOI: 10.1021/acssensors.0c01284
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      Hupa, E.; Vanamo, U.; Bobacka, J. Novel Ion-to-Electron Transduction Principle for Solid-Contact ISEs. Electroanalysis 2015, 27, 591594,  DOI: 10.1002/elan.201400596
    23. 23
      Vanamo, U.; Hupa, E.; Yrjänä, V.; Bobacka, J. New Signal Readout Principle for Solid-Contact Ion-Selective Electrodes. Anal. Chem. 2016, 88, 43694374,  DOI: 10.1021/acs.analchem.5b04800
    24. 24
      Rahn, K. L.; Anand, R. K. Recent Advancements in Bipolar Electrochemical Methods of Analysis. Anal. Chem. 2021, 93, 103123,  DOI: 10.1021/acs.analchem.0c04524
    25. 25
      Jaworska, E.; Michalska, A.; Maksymiuk, K. Self-Powered Cascade Bipolar Electrodes with Fluorimetric Readout. Anal. Chem. 2019, 91, 1552515531,  DOI: 10.1021/acs.analchem.9b03405
  • Supporting Information

    Supporting Information


    The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acssensors.1c01273.

    • Details related to diode characteristics, response of H+-ISE, capacitor voltage curves under different conditions, and stability of the Zn electrode (PDF)


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