Tara
Forrest
,
Thomas
Cherubini
,
Stéphane
Jeanneret
,
Elena
Zdrachek
,
Polyxeni
Damala
and
Eric
Bakker
*
Department of Inorganic and Analytical Chemistry, University of Geneva, Quai Ernest-Ansermet 30, CH-1211 Geneva, Switzerland. E-mail: eric.bakker@unige.ch
First published on 22nd December 2022
Current methods to monitor nitrate levels in freshwater systems are outdated because they require expensive equipment and manpower. Punctual sampling on the field or at a fixed measuring station is still the accepted monitoring procedure and fails to provide real-time estimation of nitrate levels. Continuous information is of crucial importance to evaluate the health of natural aquatic systems, which can strongly suffer from a nitrogen imbalance. We present here a nitrate-selective potentiometric probe to measure the analyte continuously without requiring maintenance or high-power consumption. Owing to a simple design where the sensors are located directly in contact with the sample, the need for constant pump usage is eliminated, requiring just 0.7 mW power per day instead of 184 mW per day and per pump. It is estimated that with this power consumption, the setup can easily run for more than 97 h on four simple Li-ion batteries. A simple in-line one-point calibration step was implemented to allow for drift correction. At the same time, a symmetrical design was used involving a second nitrate probe as a reference electrode placed in the calibrant compartment. This, combined with an in situ calibration step, allows one to quantify nitrate ion concentrations directly, instead of yielding activities. The dependence on ion activity was removed by using the analysed sample spiked with nitrate as the calibrant. This results in essentially the same activity coefficients and additionally reduces junction potentials to a fraction of a millivolt. In addition, a symmetrical reference element served to compensate for fluctuations caused by environmental factors (temperature, convection, etc.) to achieve improved stability and signal reproducibility compared to a traditional Ag/AgCl based reference electrode. The final prototype was deployed in the Arve River in Geneva for 75 h without requiring any intervention. The nitrate levels measured using the symmetrical reference element over this period were estimated at 44.0 ± 3.5 M and agreed well with the values obtained with ion chromatography (38.2 ± 2.1 μM) used as the reference method. Thanks to a modular sensing head the potentiometric sensors can be easily exchanged, making it possible to quantify other types of analytes and leading the way to a new monitoring strategy.
Environmental significanceThe effects of excessive amounts of different forms of N (e.g. NH4 and NO3) in water range from human health impacts to eutrophication (which affects dissolved O2, T and pH). The European Union adopted a motion which sets out the obligation to monitor eutrophication risks and report the results every 4 years. Currently constant monitoring points are lacking due to low spatial density and frequency of monitoring. The observations point out that the monitoring network should be strengthened and a different strategy must be envisioned. We propose here a nitrate-selective potentiometric probe that directly measures concentration continuously, has low maintenance and does not require a large power source. This proposed system could pave the way to replacing manual sampling for better nitrate level estimations. |
In 1991, the European Commission (EC) established a decree aiming to reduce nitrate pollution and prohibit further pollution.1 Since this directive, the use of nitrate-based fertilisers has been more adequately regulated and systematic water quality monitoring has been implemented. This trend can also be seen here locally in Lake Geneva, where the nitrate levels have been either constant or decreasing since 1991.2 Although it seems that the general tendency leans towards a decrease in nitrate levels and an increase in the general water quality, the monitoring process is not uniform and still rather tedious. The current strategy relies on fixed sampling stations and punctual sampling at strategic sites, which both require manpower and expensive measurement techniques, making it impossible to ensure a constant monitoring of nitrate levels. Monitoring nitrate runoff continuously is especially important due to the rapid multiplication of algae that generally are the cause for eutrophication. This fragile ecological equilibrium can be quickly impacted if no actions are taken swiftly.
Several methods are generally used to monitor nitrate in freshwater systems, such as ion chromatography,3,4 colorimetric assays,5–7 spectrophotometry8–10 and use of ion-selective electrodes.11–14 Ion chromatography is highly selective and sensitive and a well-established laboratory technique that allows nitrate quantification to the ppb level. Unfortunately, the equipment is pricy and bulky and therefore not applicable for in situ measurements, although some studies have been performed to make it portable.4 Colorimetric assays to determine nitrate date back to the 19th century6 and are mostly based on Griess test after subsequent reduction of nitrates into nitrites. Currently Griess reagent test kits are commercially available and this methodology is still at the core of modern research.7 Although these tests have proven to be reliable, they require reagent mixing by the user, which is incompatible with direct in situ measurements. Also using the reduction to nitrite, this time with a cadmium column, followed by azo-dye spectrophotometric detection, continuous analysers have been developed.15,16 The constant usage of pumps to deliver reagents makes these systems unfit for field measurements where no power source is available. Spectrophotometric water analysis of nitrate is possible because of its absorbance in the UV range but limited to freshwater owing to chloride interference. Continuous and on-site measurements are possible with this technique when coupled with a flow system.10 Long-term measurements in this case are not practical due to high power consumption because of the necessary and constant use of a peristaltic pump and UV spectrophotometer.
The use of ion-selective electrodes to quantify the nitrate levels in water dates back to the 1970s11 and was then based on classical liquid-contact electrodes where a Ag/AgCl reference element is placed on the backside of a polymeric PVC-based membrane in a solution of fixed nitrate and chloride concentrations. Over the years, attempts to miniaturise these sensors and apply them to field measurements have been made,12 but although the stability of these sensors proves to be good at high analyte concentrations (>10−2 M), the lifetime and E0 value reproducibility were poor at lower concentrations13 (∼10−4 M) which are in the environmentally relevant range. Developing ion-selective electrodes that have a long lifetime has always been and remains a fundamental challenge. The focus is often only set on maintaining14 a Nernstian slope and sufficiently low detection limit during the analysis period to ensure an adequate response. Unfortunately, less attention is drawn to maintaining a stable E0 value during the development of new sensors because correcting a long-term potential drift can be compensated by regular calibration. This maintenance step is recommended daily with commercially available ready-made nitrate sensors.22 Having to perform a calibration daily adds a complication, which is incompatible with independent long-term monitoring.
In the last few decades, special attention has been drawn to replacing liquid-contact electrodes with solid-contact electrodes23 where no inner filling solution, which must be punctually replaced, is required. The implementation of a transducing layer between the conducting element and the polymeric membrane increases the stability of the signal and gives more control over potential stability. Such sensors have already been applied to the determination of nitrate levels in environmental samples, but in most cases, measurements are performed on collected samples and not made in situ.24,25 An important characteristic of potentiometric sensors is that they are designed to measure activity rather than concentration, which may be a drawback in environmental analysis because the reporting of concentrations is prevalent. Converting activity to concentration requires one to know the total ionic strength of the sample which is not easily available in situ. Recently, however, direct access to concentration measurements with potentiometric sensors has been achieved for cations.26 It used a symmetrical design, with two different indicator electrodes measured against each other, in which the activity coefficients for the analyte ion and the ion measured at the reference electrode changed similarly with ionic strength. Another approach for direct concentration measurements for anions has been developed based on a pulstrode protocol.27
Submersible potentiometric probes28,29 are by nature designed to perform measurements directly in the field and have been used previously in environmental studies,17,18,30–32 but they require a pump to drive the sample towards the measuring site. To enable constant monitoring, the pump must run continually, which would lead to unreasonable power consumption and difficulties in deployment because of power source availability. We present here a simple nitrate-selective submersible potentiometric probe to perform constant monitoring in an independent manner. For this purpose, solid-contact nitrate-selective PVC based electrodes have been selected. The chosen transducing layer polymer, PEDOT-C14, was based on previous work on nitrate sensors performed by our group.33 This choice was also supported by the observation that electrodes prepared with PEDOT-C14 exhibited more mechanical stability than those prepared with carbon nanotubes as seen in previous work.30 This was attributed to the layer-by-layer deposition procedure of carbon nanotubes23 that promoted membrane fall-off. In this new design, the probes are located in a small recess and are in direct contact with the sample allowing constant monitoring without the requirement of any additional power. A small peristaltic pump has been programmed to run briefly at predetermined time intervals to perform a one-step calibration that is used to correct underlying drifts, that would otherwise bias the signal, and allow direct estimation of the concentration of the analyte of interest. The implementation of this automated process cancels the need for external calibration and reduces the necessity for maintenance.
Following a recent research finding by our group,34–36 a new reference element based on the principle of electrochemical symmetry was also tested and implemented to reduce the temperature influence on the sensor signal. In this case, both reference and measuring electrodes are of the same nature (PVC nitrate-selective membrane) as opposed to an asymmetrical system where a plasticised membrane is measured against an all-solid-state reference, Ag/AgCl in most cases. Although lacking stability over time, the Ag/AgCl reference electrode was chosen for comparison purposes as it is currently the gold standard in the field. It also offers miniaturisation possibilities that are often desired in submersible probes. Traditional reference electrodes, such as classical double junction electrodes, exhibit a higher stability and do not require a Cl− background but are known to be bulky, which is incompatible with the reduced available space in submersible probes. In an asymmetrical setup, outside influences such as temperature can affect the E0 value of the reference and measuring electrode differently, resulting in unwanted drifts and deviations. With an automated one-point calibration occurring 2–3 times a day and a sensing principle based on open circuit potential, the power consumption of the probe remains low and allows independent measurements to be carried out continuously on simple batteries. Longer deployment periods could be envisioned thanks to solar panels in order to have fewer power limitations. After initial testing in a laboratory with both artificial and natural freshwater samples, the prototype was deployed in the Arve River in Geneva for testing under real conditions. The obtained results from the field campaigns were cross correlated with traditional reference measurement methods for nitrate. Comparisons between the proposed system and other types of submersible probes for freshwater sensing can be found in Table 1.
Principle | Application | LOD | Characteristics | Reference |
---|---|---|---|---|
Pump driven fluidic system with an ISE | on site | 20 μM | High energy consumption due to pumps | 17 |
Pump driven fluidic system with an ISE | in line | 1.6 μM | High energy consumption and manual weekly calibration | 18 |
Gravity-fed fluidic system with an ISE | in situ | 7 μM | Non-submersible probe | 19 |
Commercial multiparameter probe (YSI) with an ISE | in situ | 0.2 μM | Matrix effects, limited to 15 m depth | 20 |
ISE with a solar powered antenna | in situ | 7.5 μM | Non-submersible probe | 21 |
Low power consumption submersible probe with an ISE | in situ | 6 μM | Submersible, no matrix effects low power consumption, and automated recalibration | This work |
Before any experiments, the functionality of the electrodes was tested by calibrating them with NaNO3 solutions from 10−7 M to 10−2 M in deionised water. The response slope as well as the lower detection limit were recorded as they are needed for further calculations. All activity coefficients were calculated according to ref. 38. To test the reliability of the electrodes under different conditions, the light and pH influence on the potentiometric signal was evaluated. It can be seen in Fig. S2A† that the signal remains constant no matter the light intensity and in Fig. S2B† that the signal remains stable when changing the pH of the solution from 6 to 11, especially in the range that is environmentally relevant (from pH 6.5 to 9.0). To confirm the applicability of these nitrate ion-selective electrodes for measurements over several days, a water layer test was conducted (see Fig. S3†) and showed no water formation between the transducer layer and the ion-selective membrane. The selectivity of these membranes was also tested to ensure the reliability of the measurements on real samples. This experiment was performed according to the MSSM.39 It can be seen in Fig. S4 and Table S1† that the proposed ion-selective electrodes are discriminating against sulfate and chloride, which are the main anions that might interfere in freshwater samples.
A schematic representation of the sensing head can be seen in Fig. 2. The sensing head is divided into two parts: a modified T-junction that contains the reference elements and sensing dome, located in contact with the sample. The top channel, called the calibrant inlet, is used to deliver the calibrant to the ion-selective electrodes during the calibration step. This is achieved using a small peristaltic pump that is activated punctually. Both references, located in the top part of the modified T-junction, will only ever be in contact with the calibrant solution thanks to the smaller diameter connection, separating both parts of the T-junction. The use of a channel exhibiting a smaller diameter prevents mixing between the calibrant and sample during the measuring periods. A small drain channel is located after the recess and can be used to aspirate solution from the sensing dome, for example in case an air bubble gets stuck inside (which will generate potential drifts). The small diameter connection between both parts of the modified T-junction is designed to ensure that when the drain channel is used, solution is pumped selectively from the sensing dome and not from the top part where the reference electrodes are located. The ion-selective electrodes are located at the bottom of the sensing head in a small dome-shaped recess. The dome has a diameter of 12.64 mm for a maximal depth of 3 mm. A schematic side-cut of the dome with its housing can be seen in Fig. S5.† It is possible to fit six measuring electrodes in the sensing dome. This can be useful to obtain intra-electrode reproducibility or measure more than one type of analyte. This geometry was chosen amongst others to have no sharp edges that would impair equal diffusion of the sample in the recess. The sensing dome is closed using metallic mesh (30 μm mesh size-stainless-steel) that shields the electrodes from outer foreign objects but still allows solution to flow freely in and out.
This difference in temperature influence is of great importance for a probe that is meant for measurements outside the laboratory, where temperature gradients during experiments can be relatively large, especially in surface waters during day and night cycles. In a follow up study,35 it has also been demonstrated that other types of drifts, occurring for example at a transducer–membrane interface or because of water uptake, are also comparable between ion-selective electrodes of the same batch. With these considerations in mind, by measuring one electrode against another of the same type (located in a solution of a fixed concentration), these drifts should cancel themselves out and lead to higher stability and reproducibility.
During the sample measurement, the whole system is passive and renewal of solution in the sensing dome is achieved by natural water motion or buoyancy. During the calibration phase (Fig. 3B), a small pump is activated and the calibration solution is pushed towards the sensing dome. In this configuration, all electrodes are now measuring the same solution. Due to the small volume of the sensing dome, less than a minute is needed to fully replace the sensing dome solution. It has also been seen that the metallic mesh placed in front of the electrodes for protection helps slow down the diffusion of the calibration solution into the bulk, therefore rendering the system more efficient and allowing for a shorter calibration period. This is a significant advantage in terms of power consumption.
During the reequilibration period, the pump is stopped and the sample gradually fills the dome again to go back to its initial state. In field campaigns, the probe is always anchored to a boat or a buoy, hence it is never static. This natural movement will help the reequilibration process and speed it up. The whole calibration procedure can be preprogramed into the probe and run at fixed time intervals (Fig. S6†). The duration of a cycle can be adjusted to space out the number of calibrations to fit the experimental needs. Since the concentration of the calibrant solution remains constant, the potential value corresponding to the calibrant should remain stable throughout cycles and is therefore a good control parameter towards undesired drifts. In addition to this, the calibration step is also used to estimate the concentration of the real sample with better accuracy.
When performing a calibration in a laboratory setup, one is able to obtain a calibration curve that will normally adhere to the theoretical Nernst equation. It is well known that this equation correlates the measured potential with the activity of the ion of interest. During field measurements, estimating the activity of the sample is of limited interest since the ionic strength (aI = γ·cI) has to be known to compute the concentration of the ion of interest. Determining the total ionic strength requires a concentration estimation of all major ionic species. Because this involves benchtop instrumentation it defeats the purpose of direct on-site measurements. In the case presented here, since the calibrant is based on the sample, it can be assumed that the ionic strength is the same in both cases. It is possible to use this information to obtain the concentration of the sample based on the Nikolsky–Eisenmann equations of both solutions:
![]() | (1) |
![]() | (2) |
![]() | (3) |
If eqn (2) is subtracted from eqn (1), the difference potential ΔEMF is obtained. This allows the removal of the parameter KI which is the same in both cases owing to the similar composition of the sample and calibrant. The activity coefficient is now present everywhere in the logarithmic part of eqn (4) and therefore also cancels out:
![]() | (4) |
It should be emphasised here that this assumption is only possible because both samples have very similar ionic strengths. As mentioned before, the calibrant is prepared on-site by spiking a nitrate aliquot in a known volume of sample. The concentration of nitrate in both solutions can now be correlated:
![]() | (5) |
Finally, the temperature correction on the slope can also be adjusted, by knowing at what temperature the laboratory calibration was performed initially:
![]() | (6) |
If eqn (1)–(6) are now combined, the unknown nitrate concentration in the sample can be calculated using the following equation:
![]() | (7) |
This makes it now possible to have direct access to the concentration (not activity) of the medium, without having to estimate the total ionic strength, which is impossible during on-site measurements.
Tests mimicking a real environment were conducted in a fish tank equipped with a water circulating system to reproduce the natural flow of a river. The tank was filled with a solution containing 0.5 mM NaCl/0.5 mM NaNO3 and the calibrant was set to 0.5 mM NaCl/2.0 mM NaNO3. As seen in Fig. 4, the sample was first measured and then periodically the pump was activated to push the calibrant (containing a higher concentration of nitrate ions) into the sensing dome as depicted in Fig. 3. Due to the different concentrations of nitrate anions in the two solutions the potential value drops according to the Nernst equation when the calibrant solution is pushed towards the dome. Once a stable potential value was obtained for the calibrant, the pump was stopped and the signal was found to gradually return to the initial potential value corresponding to the sample. The rate at which the initial potential is recovered can be adjusted by changing the mesh size. By comparing Fig. 4A and B it can be noticed that with the larger mesh size, the baseline is reached faster than with the smaller sized mesh. More cycles could be performed in 2000 s with the 74 μm mesh size due to a faster reequilibration time. Having different mesh sizes is also an advantage for field testing where it can be adapted depending on the turbulences present in the medium. A smaller mesh size may be more suited in the case of a very turbulent sample to achieve the calibration step, while a larger mesh size might be advantageous in more stagnant environments to not impair the reequilibration process after the calibration step.
The potential jump that was observed in both cases (∼−38.0 mV) was consistent with theoretical calculations based on the Nernst equation, taking into account the junction potential. In this case, since solutions of low ionic strength were used, the junction potential had to be considered. The classical Henderson equation was used to estimate the junction potential and all ion mobility values were taken from ref. 41. The liquid junction potential was calculated according to Henderson's eqn (8).
![]() | (8) |
With a calculated potential difference of −39.0 mV, it can be concluded that the solution exchange during the calibration process is optimal and that the proposed geometry of the sensing head works as expected for the one-point calibration.
To avoid high junction potentials (up to 5 mV) when working with solutions of low ionic strength, follow-up experiments using the same setup were conducted in real water samples sourced from the Rhône River in Geneva. To confirm the small junction potential between two solutions of higher ionic strength, the concentrations of all major cations (K+, Na+, Ca2+ and Mg2+) and anions (NO3−, Cl−, HCO3− and SO42−) were estimated using reference methods specified in the experimental section. The individual concentrations of each ion can be found in Table S2.† The calibrant used in this case was the same Rhône River water sample but spiked with NaNO3. The concentration of nitrate in the calibrant was 155.3 μM compared to 35.3 μM in the sample. The resulting junction potential calculated between the two solutions was lower than 0.3 mV and can be neglected considering that the expected potential shift between both solutions corresponds to −38.0 mV.
The results from the tank-based tests with a real sample are presented in Fig. 5. In this case, a piece of fine mesh (30 μm) was mounted to have the same conditions that would be further used in the field campaign. In addition to testing the one-point calibration protocol, the symmetrical reference element was also implemented. Since the experiment is performed in a controlled environment, the temperature fluctuations are minimal; therefore their influence on both references should not be seen. In both cases, the reversibility is satisfactory and the signal corresponding to the sample is recovered in minimal time. It can be noticed that the time trace corresponding to the response versus the Ag/AgCl reference exhibits more noise and perturbations, especially during the calibration step. This can be explained by the fact that when the pump is activated, the electrodes are subjected to a stronger flow than during the passive sample measurement, causing a small perturbation. Since this flow is similar in the modified T-junction, where the symmetrical reference is located, and the sensing dome, when measured against each other, this interference cancels out, leading to a smoother signal. The potential values recorded for the sample exhibit a smaller standard deviation when measured against the symmetrical reference (2.7 ± 0.2 mV) element than that exhibited when measured against the Ag/AgCl reference (34.2 ± 0.6 mV). The same conclusion can be drawn for the potential values corresponding to the calibrant (−0.6 ± 0.6 mV for the classical system versus −34.3 ± 0.3 mV for the symmetrical system). The observed potential shift between both solutions is closer to the theoretical value with the symmetrical system (−37.0 ± 0.3 mV) compared to the classical system (−34.8 ± 0.6 mV). Cycle by cycle data extracted from Fig. 5 can be found in Table S3† for the symmetrical reference and Table S4† for the Ag/agCl reference element. Both tests performed in the laboratory showed that the one-point calibration is successful and sufficiently accurate to enable one to estimate the nitrate concentration of an unknown sample with eqn (7), without having to use traditional measurement methods for nitrate that are not well suited for field work. This accuracy is reinforced by the use of the symmetrical reference element that helps cancel out small perturbations or drift, seen when using a traditional Ag/AgCl reference element.
Field measurements were performed in the Arve River in spring 2022. The probe was anchored with a rope to a platform close to the shore. During the testing period the smaller mesh size was always used (30 μm) due to a turbulent flow which is typical for this time of the year, due to snow melting in the French Alps where the Arve has its source. The probe was immersed during the day and preprogramed to perform a calibration every 8 h. The details of the calibration cycle can be found in Fig. S6 and Table S5† During each cycle, the pump was activated for a total time of a 120 s and the signal related to the calibrant was recorded at the end. No measurements were taken during the 5 min following the calibration routine to leave some time for the calibrant to dissipate from the dome and be exchanged with the sample again. Knowing the flow rate of the pump (2.6 mL min−1), 15.6 mL of calibrant was consumed every day assuming 3 calibrations are performed. With the 500 mL calibrant bag that was mounted, the solution would have to be renewed only every 30 days. The results generated by the probe were stored internally on an SD card as a text file. These files were then processed with Mathematica to generate time traces and convert potential readings into nitrate concentrations with eqn (7).
Performing 3 calibrations a day means that the pump is activated for a total of 360 s per day. Knowing that the pump requires 50 mA at 3.7 V, the daily power consumption is just 0.77 mW. If the pump was running continuously, as it is classically done in submersible probes, the daily required power would be 185 mW. The main board included in the instrument needs 100 mA at 5 V to run at full power. If needed, the main board can go into standby where it will only need 20 μA at 5 V. Assuming the board runs at full power continuously, the daily required power may be estimated at 0.5 W. With this information, it is assumed that the probe can run for at least 97 h on 4 Li-ion batteries. To remove the need for battery exchange, it is calculated that a 43 × 55 cm solar panel would be sufficient to power the device with only 2 h of direct sunlight a day.
Fig. 6A shows the potentiometric time trace of a nitrate-selective electrode versus the Ag/AgCl reference, showing a drifting signal over time. Over the 75 h of the testing period the overall potential change was estimated at around 30.0 mV (from ∼30.0 mV at t = 0 h to ∼0.0 mV at t = 75 h). Fig. 6B, which represents the potentiometric time trace of the nitrate-selective electrode used as the reference relative to the same Ag/AgCl electrode, shows that this drift is similar. Since both reference electrodes are in a solution of fixed concentration, one can be sure that the observed potential shift is a drift and not a response towards nitrate. The intense drift seen in the first few hours after immersion may originate from the low water temperature, below 10 °C during the testing period. To correct for the drift seen in both cases, the symmetrical reference was used to generate Fig. 6C. Both graphs presented in Fig. 6A and B are raw potentiometric data, where no temperature correction is applied. Applying a temperature correction here to generate Fig. 6C is not needed as it would be cancelled out mathematically. The temperature correction was applied when calculating the concentration of nitrate as seen in Fig. 7. The drift is now compensated for and the observed signal exhibits an increased stability. The spikes, corresponding to the calibration events, are now more reproducible and the overall signal change over the entire testing period is now approximately 6.0 mV.
![]() | ||
Fig. 6 (A) Potentiometric response of a nitrate-selective electrode versus the Ag/AgCl electrode. The 30 μm mesh size was used due to the strong flow of the river. (B) Potentiometric response of a symmetrical nitrate-selective reference electrode versus Ag/AgCl. (C) Potentiometric response of the nitrate-selective electrode versus the symmetrical reference. Graphs (A) and (C) represent the same measuring electrode. Graph (A) and (B) are raw potentiometric traces without temperature correction. In this case, the nitrate concentration of the calibrant was estimated at 161.8 μM by ion chromatography. The nitrate concentration calculated from graph (C) can be seen in Fig. 7. |
![]() | ||
Fig. 7 Converted potentiometric data using eqn (7) to get the concentration of an unknown sample. (A) Results of the nitrate-selective electrode versus the symmetrical reference. (B) Results of the nitrate-selective electrode versus the Ag/AgCl reference. On both graphs, blue dots represent the nitrate concentration obtained by ion chromatography from punctual sampling. Error bars represent the standard deviation (n = 3). |
To confirm the reliability of the system, the water from the Arve River was punctually sampled throughout the testing period and analysed by ion chromatography to allow cross-correlation. The potential readings obtained with the probe were converted to concentration values using eqn (7). It should be noted here that the parameter EMFcal was always updated after a calibration cycle to use the latest value. Throughout the cycles, the average value for EMFcal was more reproducible when using the symmetrical reference (EMFcal, symmetry = −22.0 ± 1.6 mV) compared to that obtained when using the Ag/AgCl reference (EMFcal, Ag/AgCl = −16.7 ± 2.2 mV). The same conclusion can be drawn when estimating the ΔEMF between EMFcal and the EMF reading before the calibration process. The average ΔEMF when measuring against the symmetrical reference was found to be equal to ΔEMFsymmetry = −27.5 ± 1.2 mV compared to ΔEMFAg/AgCl = −23.6 ± 2.0 mV, obtained using the traditional reference element. Both average ΔEMF values differ by 3.9 mV, which will have an impact on the observed nitrate concentration value.
Fig. 7 presents the converted raw data, extracted from the probe, into a molar nitrate concentration. The implementation of the in-line calibration step allowed one to have direct access to the concentration of nitrate ions instead of activity. The blue dots on the graph indicate the concentration of nitrate obtained by ion chromatography used as the reference method. From Fig. 7A and B it can be seen that the concentration levels obtained using the symmetrical reference correlate better with the measured levels by ion chromatography. The fluctuation of the signal is also minimised when using the symmetrical reference since interferences, such as temperature drift or convection, affect both plasticised membranes in a similar manner. A more stable signal correlates with the trend seen in the different ion chromatography (IC) measurements over time. The average nitrate concentration measured by ion chromatography is 38.2 ± 2.1 mM. Individual nitrate concentrations recorded by IC can be found in Table S6.† Sampling more often would have been an advantage for better cross-correlation between IC data and the probe, but it was unfortunately not possible due to the complicated access to the anchoring point of the probe. When performed, sampling was conducted manually, thus stressing the need for better measuring systems and sampling facilities. The average nitrate concentration observed using the probe for the same times at which these samples were taken was 44.0 ± 3.5 mM when measured against the symmetrical reference element. This value increases to 77.4 ± 6.4 mM when using Ag/AgCl as the reference, which is unacceptable. This overestimated concentration was measured with the Ag/AgCl electrode and is presented in Fig. 7B is due to a lower and biased measured ΔEMF than expected. A smaller ΔEMF suggests a smaller difference between the concentration of the sample and calibrant, thus the overestimation. Such high deviations can cause issues during a monitoring campaign, expressing the need for better reference elements.
The potentiometric response of the electrodes was tested before the immersion in the real sample and after the testing period, to confirm that they were still functional. It can be seen in Fig. S7† that after the experiment in the Arve River, the E0 value has indeed shifted and the lower detection limit shifted from −5.2 to −4.8 in nitrate logarithmic activity. This change is not significant for our experiments as the natural nitrate concentration found in the Arve River is in both cases still in the linear response range. It is assumed that this effect is due to biofouling at the surface of the electrode. For longer deployment periods, a new strategy to avoid biofouling will have to be implemented. Several options could be envisioned, such as replacing the stainless-steel mesh by copper mesh that is known to have antifouling properties42 or by in situ electrochemical generation of chlorine43 using the metallic mesh as the electrode. The latter strategy is mainly used in seawater, where the concentration of salt is high, but recently attempts with lower amounts of NaCl44 have been undertaken and could be applied to the case of freshwater. For improved results, both of these options could be combined with ion-selective membrane surface modification with silver nanoparticles45 for increased anti-biofouling properties. To prevent microbial growth and biofouling in the compartment where the reference electrodes are located, a piece of copper mesh could be implemented between the calibrant bag and tubing inlet. By avoiding biofouling of the electrodes and using solar panels to power the probe, maintenance should only be required to refill the calibrant bag and exchange the electrodes. In a previous study, it was shown that nitrate-selective electrodes were functional for at least 3 weeks.34 The main limiting factor in this case is the lifetime and lower detection limit of the ion-selective electrodes.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d2em00341d |
This journal is © The Royal Society of Chemistry 2023 |