The present invention refers to a method for the quantification of analytes concentration present in a sample by making use of a self-powered, disposable, single use device. The method relies on the combination of an electrochemical cell and an electronic load connected in parallel to it. The electronic load can be composed of a combination of at least one capacitive load and/or one resistive load. One fundamental aspect of the method is that the resistive load connected to the electrochemical cell has a value that puts the cell to work under diffusion-limited conditions. The level of the built-up voltage developed across the capacitive element can be correlated to the analyte concentration in the electrochemical cell. The built-up voltage in the capacitive element can be measured using an integrated readout unit that can be powered by the electrochemical cell itself. Alternatively, the readout unit can also be an external measuring device.
An analyte is a chemical species, whose presence or content in a sample is detected, identified and quantified through a chemical measuring process. The use of electrochemical systems including potentiometric or amperometric sensors and biosensors to quantity the analyte present in a sample has been widely reported.
These sensors generally consist of electrochemical cells containing a working electrode (sensing electrode), where the analyte reacts through a redox reaction, and a counter electrode, where the complementary redox reaction takes place. The sensing and counter electrodes may or may not be enzymatic. The sensing electrode is preferably selective towards the redox analyte reaction to ensure the reliability of the sensor.
These electrochemical sensors may be potentiometric, such as that presented in U.S. 2004/0245101 A1, where the open circuit voltage of the fuel cell is monitored and correlated to the concentration of analyte. This method has been designed for continuous flow conditions, where the fuel cell voltage is steady for as long as the fuel is provided with a constant flow and concentration of analyte. Although these biofuel cells operate at low efficiency, and have limited applicability as energy suppliers, the extractable electrical power is sufficient to probe the sensing elements. The sensor operates with no external power sources. However, an external readout system is needed to measure the open circuit voltage.
Alternatively, the determination of the analyte present in the sample can be performed using amperometric sensors, in which the fuel cell may be polarized by setting a constant operating voltage, applying a load or sweeping a voltage range, to generate electrical current. The fuel cell voltage or the generated current can be measured and correlated with the concentration of analyte. These systems commonly require complex electronics and an external power supply for the polarisation and recoding of electric current or voltage. Moreover, they require a dedicated external readout unit.
The use of external equipment such as a potentiostat or a power supply can be avoided by connecting the fuel cell to a load (i.e. a resistor), as reported in WO2005093400 A1, U.S. Pat. No. 9,220,451 B2 and US 2010/0213057 A1.
These type of sensors are generally regarded as self-powered, since no power supply is needed to operate them at a specific voltage or to perform a voltage sweep. However, they still need to be connected or integrated to a suitable transducer, which enables the conversion of specific analyte concentrations to electronic signals, and finally to human recognizable information.
In most cases, a voltage or current readout system is also needed. As described in US 2010/0213057 A1, the readout can be taken directly with an external unit (handheld display) or by coupling the sensor to a radio-frequency (RF) powered measurement circuit. The RF powered measurement circuit is remotely queried at regular intervals by an RF-power equipped hand-held display in order to provide continuous analyte level measurements.
The self-powered devices for analyte detection from a fuel cell are based on the correlation between the electrical current generated from the fuel cell and the concentration of analyte. However, this type of self-powered devices generally need an external receiver to receive the signal generated from the transmitting device or alternative methods to transduce the electrical current or voltage measured in the fuel cell to a user readable signal. To ensure reproducible results, it is necessary the use of a potentiostat to sweep voltage and obtain current values. This reduces the applicability of these type of devices as they hinder the possibility to power the device as a whole from the integrated sensor, since an external power supply and other auxiliary elements are needed to power the potentiostat. Moreover, these types of devices are aimed for long-term measurements or continuous monitoring applications and the sample in generally is continuously flowed into the electrochemical cell. As a consequence, the fuel cell voltage is steady for as long as the fuel is flowing through the cell and for a wide range of resistive loads. This facilitates the measurement of the fuel cell voltage.
In certain cases, the voltage or current generated from the fuel cell is not constant over time, for example, when the volume is restricted to few microliters due to the nature of the sample such as in case of extracted blood samples from a finger prick. In this case, when the fuel cell is connected to a load and the electrochemical reaction starts, depleting the fuel and generating a concentration gradient, which is proportional to the diffusion coefficient of the analyte. Consequently, the fuel cell voltage is continuously varying and decreasing along with the concentration of sample being depleted during the measurement. This makes it extremely difficult to measure the initial concentration of analyte in the sample.
Other type of devices like reported in US 2010/0200429 A1 make use of an enzymatic fuel cell to charge a capacitor, which discharges through a signal, such as LED lighting. In this case, a charge pump was required to boost the fuel cell voltage to be fed to a capacitor. After the capacitor reached a fixed value, it discharged through a load to again get recharged and the process continued. The charging/discharging frequency of the capacitor, which depends on the concentration of analyte, is transmitted by radio frequency and a receiver identifies the signal and converts it to an analyte concentration value.
In this case, it is necessary to use external equipment to measure voltage or current, or a radio frequency receptor. Additionally, the induced electromotive force in the fuel cell, that is fed to charge pump is dependent on the concentration of the sample. Hence, as previously mentioned, the observed concentration gradients while employing low volume samples is likely to alter the charging frequency dependency.
Similarly to the device described in the previous paragraph, where the load connected to an electrochemical cell is a resistor, the volume of sample supplied to the fuel cell is crucial. In batch systems where the sample volume is such that the concentration gradient generated does not reach the end of the sample volume or for continuous flow systems, where the analyte concentration and the bulk concentration are constant and the charging/discharging cycles remain constant. In this case, the charging/discharging frequency of the capacitor can be monitored and a signal can be sent to an external reader.
On the contrary, for a small volume of sample (i.e. a drop), the charging/discharging cycles are not constant. If a threshold voltage is set, the induced voltage decreases and the charging time of capacitor will become longer in time, as the analyte in the sample is depleted. With non-constant as well as inconsistent charging/discharging cycles, the frequency measurements become irrelevant and thus fail to provide a reliable measurement. If a specific time is set for charging cycle and the discharging cycle of the capacitor, the charging/discharging voltages will decrease in time, as the fuel is being depleted. This makes the reading using a threshold voltage difficult, since voltage reached is decreasing in each cycle. This could provide an inaccurate frequency result and therefore an inaccurate analyte concentration value.
Moreover, this type of devices require complex electronics, which often need to include a charge pump and an oscillator. This reduces the applicability of the device, and limits its usage in locations with no external power source, readout unit or receivers.
The object of this invention is to provide a simple method to measure the concentration of analyte in a sample fed into an electrochemical cell, which can contain a volume of sample, which might be any volume, and with the possibility to use, but with no need for an external power source or an external receiver. This method could use a single use, disposable and autonomous device, with simple, disposable and self-powered electronics, and avoiding the use of external batteries.
In particular, the method in this invention makes use of a device, which comprises an electrochemical cell, an electronic load connected in parallel to it, and a readout unit connected in parallel to the electronic load.
Specifically, the device and the method for quantifying the concentration of analyte in a sample comprises an electrochemical cell and an electronic load connected in parallel to it. The electronic load can be composed of a combination of at least one capacitive load and one resistive load.
One fundamental aspect of the device and method is that the equivalent resistance of the load connected to the electrochemical cell has a value that puts the cell to work under diffusion-limited conditions. Diffusion-limited is defined here as a condition in which the analyte reacting at the cell electrodes is consumed at an equal or faster rate than the rate of its transport through the reaction medium.
When the electrochemical cell operates in this diffusion-limited regime, it enters in a non-steady state in which the output voltage decreases with time. The current generated by the electrochemical cell in this condition is transferred totally or partially to the capacitive load. The built-up voltage developed across the capacitive element can be correlated to the analyte concentration in the electrochemical cell.
Therefore, this method allows for a simple and straightforward transduction of concentration of analyte to voltage. This device and method differ from other reported methods in a way that the method proposed here does not analyse the analyte concentration based on an output signal obtained from the frequency response obtained from multiple charging/discharging cycles. This device and method operate the electrochemical cell in a direct current (DC) mode during a single discharge cycle of the cell. This strategy allows simplifying significantly the instrumentation required to drive the electrochemical cell and readout unit.
Moreover, this device and method allow to quantify the analyte concentration of low volume or/and non-flowing samples, in which a diffusion-limited regime is established whenever any resistive load is connected to the electrochemical cell. This phenomenon, that would render other reported methods inaccurate, is taken in the present invention as an advantage and constitutes the cornerstone of the measurement principle.
The built-up voltage in the capacitive element can be measured using an integrated readout unit that is powered by the electrochemical cell itself. Alternatively, the readout unit can also be an external measuring device.
The electrochemical cell consists of at least one electrode, where the oxidation reaction takes place (anode) and one electrode, where the reduction reaction takes place (cathode). These electrodes are in contact with an electrolyte, where the ion transfer takes place.
In the electrochemical cell, at least one of the two electrodes (named sensing electrode) reacts with the analyte, through an oxidation or reduction reaction, while at the other electrode (named complementary electrode) a complementary reaction takes place (reduction or oxidation) in order to form an electrochemical cell which allows the generation of voltage and electrical current.
The sensing electrode may transfer the electrical current directly or through a mediator.
The sensing electrode may be constructed from any material, which is catalytic for the redox reaction of the analyte, including metals, alloys, redox polymers, enzymes or bacteria, such as glucose dehydrogenase enzyme, glucose oxidase, FDH, MDH, AOD, XOD, Hyderase, Gluconobacter oxidants, magnesium, palladium, bismuth, nickel, platinum, ruthenium, gold, carbon, graphite, iron, lithium, cadmium, copper, silver, zinc, aluminium, among others.
The sensing electrode may be enzymatic and similar to an electrode of a first generation enzymatic sensor. In this case, the electrode is selective towards a specific analyte, which is oxidized, while in a simultaneous reduction reaction a cofactor is reduced. Then, the reduced cofactor is oxidised, using oxygen to produce hydrogen peroxide at the electrode surface, and generating an electric signal proportional to the concentration of analyte. The sensing electrode may also be similar to an electrode of a second-generation amperometric sensor, composed by a mediator (in solution) for the electronic transfer to the electrode. The sensing electrode may also be similar to a third-generation amperometric sensor, with direct electron transfer, with the enzyme physically connected to the electrode.
At the complementary electrode, either a reduction or an oxidation reaction takes place; this reaction will be complementary to that taking place at the sensing electrode. The redox voltage of this reaction must be more electropositive than that of the reaction at the sensing electrode, if the complementary electrode acts as the cathode; or more electronegative than that at the sensing electrode, if the complementary electrode acts as the anode. This is necessary to generate a positive voltage difference between the cathodic and the anodic electrodes. The reaction taking place at the complementary electrode must not be the limiting reaction to the generation of electric current. The limiting reaction must be directly dependent on the concentration of analyte.
The complementary electrode may be formed by any redox species, complementary to the electrochemical reaction taking place at the sensing electrode. That could be metals, alloys, polymer materials reducing or oxidant, batteries or enzymes, such as iron, cobalt, nickel, benzoquinone, silver, silver oxide, silver peroxide, copper, magnesium, platinum, gold, carbon compounds, including electrodes based on activated carbon, graphite, carbon nanotubes and carbon paste, magnesium, zinc, aluminium, among others.
The sensing and complementary electrodes might be planar and distributed next to each other or in front of each other. More than one combination of sensing and complementary electrodes might be used to increase the voltage by connecting them in series or to increase the generated electric current by connecting them in parallel. Both electrodes might or might not be separated by an ion-exchange membrane, which can be selective or non-selective, by a porous material or by a salt bridge.
Besides the electrochemical cell, the device object of this invention also comprises a load, connected in parallel to the sensor, that can be resistive, capacitive, inductive, or a combination of them. By connecting the electrochemical cell to the load, it starts working under diffusion-controlled conditions. Then, the response from the electrochemical cell is dependent on the concentration of analyte in the sample. Using a reader connected in parallel to the load, the concentration of analyte can be identified from the readout of the voltage across the load.
In particular, in a first embodiment of the device, the load connected to the electrochemical cell is predominantly capacitive, being preferably a capacitor. The resistive load is set by the internal resistivity of the electrochemical cell and the ohmic resistance of the electrodes, circuit tracks and electrical connections of the assembly.
When the circuit is closed, the electrical charge generated from the electrochemical cell is transferred to the capacitor. The voltage reached across the capacitor (VC) depends on the electrical charge that has been transferred from the electrochemical cell (VS). This accumulated charge also depends on the concentration of analyte which has been oxidised or reduced in the electrochemical cell. As a result, the developed voltage across the capacitor (VC) provides information about the concentration of analyte in the sample.
Charge accumulation makes the capacitor voltage to rise according to eq (1) where VC(t) is the voltage across the capacitor, q (t) is the charge generated by the electrochemical cell working under diffusion-limited regime that is being stored in the capacitor with time and C is the capacitance of capacitor, A is the area of the cell sensing electrode, D the diffusion coefficient of the analyte, t the time and Co as the concentration of analyte. Similarly, charge accumulation can be expressed in terms of
As it can be seen, the capacitor built-up voltage is proportional to the analyte concentration and this allows a direct quantification of analyte content.
Under this configuration, the evolution of the built-up capacitor voltage causes the electrochemical cell voltage to rise simultaneously until the analyte is totally depleted from the sample. We can label this time as tsat, as the capacitor voltage reaches a saturation of transferred charge, as the electrochemical cell ceases generating current.
Alternatively, the charge transfer between electrochemical cell and capacitor can be interrupted by disconnecting the two elements at a particular time with an additional such as a diode, switch, transistor among others. The final fixed value of the capacitor voltage can be taken as Vout, which is directly proportional to the quantity of analyte in the sample.
In a second embodiment, the load connected to the electrochemical cell is predominantly resistive, being preferably a resistor. In particular, a resistive load R1 is connected in parallel to the electrochemical cell as the major load. A second branch containing resistor R2, capacitor C1 and diode D1 is also connected in parallel to the electrochemical cell.
In this embodiment, once the circuit is connected to the electrochemical cell, the resistive load R1 sets the cell in a diffusion-limited regime that causes a drop in the electrochemical cell voltage from its open-circuit potential. The current generated by the electrochemical cell flows through the branches containing R1 and R2. During this process, the capacitor C1 featuring in the branch alongside resistor R2 and D1 gets charged.
Eventually, the diode D1 goes into reverse bias when the built-up voltage in the capacitor increase and electrochemical cell voltage decreases under a threshold value. When the voltage across the diode puts it in reverse bias, the current through the branch containing it almost ceases (acting like a switch to cut off the connection between electrochemical cell and capacitor), and the capacitor is held at the final charged voltage acquired just before the diode significantly obstructed the current flow.
Importantly, even after, though the electrochemical cell is constantly dropping in voltage due to the influence of R1, the capacitor C1 maintains at the final charged voltage value, as the diode restricts the current flow in reverse direction. The final built-up output voltage across the capacitor is proportional to the analyte concentration. The level of output voltages reached in the capacitive element can be modulated or shifted by the choice of the combination of resistors R1 and R2 and capacitor C1 values without affecting the response pattern.
The differences in voltage levels acquired between analyte concentrations measured in the capacitive element can be modulated by the choice of the combination of the resistors R1 and R2 and capacitance value C1.
In a third embodiment of the invention, the load connected to the electrochemical cell is predominantly resistive, being preferably a resistor. In this embodiment, once the circuit is connected to the electrochemical cell, the resistive load R1 sets the cell in a diffusion-limited regime that causes a drop in the electrochemical cell voltage from its open-circuit potential.
The rate at which the electrochemical cell voltage decays is related to the concentration of oxidized or reduced analyte in the electrochemical cell. The rate of voltage drop in an electrochemical cell voltage when subjected to resistive load R1 is slower at higher concentrations of analyte. In this embodiment, information about the analyte concentration can be obtained by measuring the elapsed time between a previously defined initial voltage and a final threshold voltage, using the readout unit.
The readout unit allows the transduction of the response generated by the electrochemical cell to a signal that allows the user to derive information on the analyte concentration. This signal might consist of a digital screen or lighting, acoustic or mechanical signals. These signals may indicate the concentration of analyte or whether it has exceeded certain predefined threshold values.
The readout unit may be integrated in the device with the electrochemical cell and the load, making this device portable and disposable. Alternatively, the readout unit may be an external component.
Alternatively, the readout unit may be powered only by the energy generated by the electrochemical cell, or alternatively, it may be powered by an external power supply or a combination of both.
More specifically, in the methodologies involving the readout of a capacitive element the readout unit may consist of any unit capable of measuring the capacitor voltage. This allows to obtain information on the analyte concentration with direct current (DC) voltage readout systems and from a single charging cycle. The readout unit may consist of one or a set of transistors, integrated circuits, application-specific integrated circuits (ASICs), a multimeter, a USB communication system with a computer, an RFID, NFC wireless communication system, or Bluetooth system among others.
In another embodiment of the device, when the load connected to the electrochemical cell is resistive, the readout unit may consist of two units that measure voltage and time simultaneously, or one unit that integrates these two functions. The readout unit may consist of, for instance, any of the options to measure the voltage mentioned in the previous paragraph, combined with a method to measure time, such as complex electronics, that might include a clock, a quartz crystal, an RC circuit or any type of external clock among others.
In another embodiment of the device, it may be possible that the load comprises a matrix of capacitors in a way that the tension reached between each of the capacitor terminals provides discrete information of the concentration of analyte in the electrochemical cell.
A specific example of the embodiment of this device for quantification of the concentration of analytes in an electrochemical cell is a glucometer, in which the concentration of glucose is quantified. Glucose is the analyte present in blood and this device may be used for the diagnostic of diabetes.
In order to complete the description of the invention and improve the understanding of the invention characteristics, according to the preferred embodiment example, a set of drawing is presented as an integral unit of the invention description. This set of drawings, being illustrative and non-restrictive, represent the following:
In the following, and supported by
In a first embodiment, as depicted in
The readout element (3), as shown in
The readout unit (3) shown in
In another embodiment, as depicted in
The built-up voltage of the capacitor in the RC circuit in block (10) depends on the elapsed time in which the voltage of the electrochemical cell (1) evolves from an initial value to a final value. This interval is determined by block (9).
The magnitude of the interval depends on the analyte concentration in the electrochemical cell (1). Therefore, by measuring the built-up voltage in the capacitor of block (10) once the voltage in the electrochemical cell (1) has reached a threshold value, the analyte concentration can be quantified. Higher analyte concentrations originate higher built-up voltages in the capacitor, as it will have been charged for a larger period of time.
In another embodiment as shown in
As it also can be seen from
In another embodiment, the electrochemical cell (1) has been connected to the circuit shown in
As shown in
In additional embodiments, the electrochemical cell (1) has been connected to the circuit shown in
Number | Date | Country | Kind |
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P201930320 | Apr 2019 | ES | national |
Filing Document | Filing Date | Country | Kind |
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PCT/ES2020/070237 | 4/13/2020 | WO | 00 |