Tina
D'Aponte
a,
Maria
De Luca
a,
Nikola
Sakač
b,
Martina
Schibeci
c,
Angela
Arciello
c,
Emanuela
Roscetto
d,
Maria Rosaria
Catania
d,
Vincenzo
Iannotti
ae,
Raffaele
Velotta
a and
Bartolomeo
Della Ventura
*a
aDepartment of Physics “Ettore Pancini”, University of Naples “Federico II”, 80126 Naples, Italy. E-mail: bartolomeo.dellaventura@unina.it
bFaculty of Geotechnical Engineering, University of Zagreb, 42000 Varaždin, Croatia
cDepartment of Chemical Sciences, University of Naples “Federico II”, 80126 Naples, Italy
dDepartment of Molecular Medicine and Medical Biotechnology, University of Naples “Federico II”, 80131 Naples, Italy
eCNR – SPIN (Institute for Superconductors, Oxides and other Innovative Materials and Devices), Piazzale V. Tecchio 80, 80125 Naples, Italy
First published on 10th October 2023
Candida albicans is a fungal organism commonly found in the human body, including the genitourinary tract. Overgrowth of this yeast can lead to candiduria, the abnormal presence of C. albicans in urine. The detection of candiduria relies on various methods that offer sensitivity and specificity for accurate diagnosis, but none of them is rapid and cost-effective. Biosensors may offer an answer; in particular, impedance-based biosensors have shown promise in addressing the detection of C. albicans since they offer high sensitivity, simplicity of fabrication, excellent selectivity, real-time detection, and cost-effectiveness. However, variations in the working surface of commercial screen-printed electrodes as well as manual functionalization can impact robustness and reproducibility. In this paper, we describe significant advances that we introduced to perform electrochemical impedance spectroscopy for biosensing purposes. Specifically, we designed a microfluidic cell for standardizing the electrode functionalization and target detection, ensuring sensor reproducibility and robustness. By optimizing several parameters like the flow rate and the density of antibodies on the electrode surface, we could achieve a limit of detection of 10 CFU mL−1 in urine with a measurement that lasted for less than 90 minutes. The modularity of the device and the measurement procedure makes the described biosensor extendable for conducting high-throughput analyses.
The gold standard method for diagnosing candiduria is urine culture. It involves inoculating urine samples onto appropriate culture media, such as Sabouraud dextrose agar or chromogenic agar, which selectively promote the growth of Candida species.5,6 Colonies are then identified through morphological characteristics, biochemical tests, or automated systems.7 This method provides both qualitative and quantitative information, but it is time-consuming since approximately 48 hours are required to obtain a response.
Polymerase chain reaction (PCR)8,9 and other molecular techniques have emerged as valuable tools for detecting Candida DNA in urine samples. These methods target specific Candida genes or regions and offer high sensitivity and specificity. PCR can differentiate between various Candida species and even detect low fungal loads. However, it is worth evidencing that PCR assays for Candida detection in urine typically do not provide quantitative information regarding the fungal load. This limitation may hinder the ability to determine the severity of infection or monitor treatment responses accurately.10
Enzyme-linked immunosorbent assays (ELISAs) are already utilized for Candida detection and demonstrate a good limit of detection (LOD). However, they are still associated with relatively long waiting times for obtaining results.11
In the last year, Matrix-Assisted Laser Desorption/Ionization Time-of-Flight Mass Spectrometry MALDI-TOF MS has revolutionized microbial identification, including Candida species, since this technique analyses the protein profiles of microbial colonies and allows for rapid and accurate identification, even at the species level. Moreover, it can be applied to colonies obtained from urine culture. However, each of these methods has its own set of advantages and limitations, including factors like availability, cost, laboratory expertise, and the clinical context in which the test is being performed.12,13
Biosensors with enhanced sensitivity, selectivity, and ease-of-use would be crucial for improving the diagnosis and management of candiduria. In fact, a variety of biosensors have been proposed for the detection of Candida, offering different advantages and performance characteristics. Optical biosensing techniques,14 such as surface plasmon resonance and fluorescence-based assays,15,16 utilize the interaction of light with Candida-specific biomarkers for detection. Although they provide high sensitivity and real-time monitoring capabilities,17 these biosensors often require complex instrumentation, labelling processes, and expert personnel.
Electrochemical biosensors are emerging as a powerful tool for detecting pathogens in biological fluids such as blood, sweat, saliva, tears, and urine.18,19 This technology is also suitable for portable and wearable devices, allowing continuous monitoring and enabling early management in diagnostics.20,21 In particular, electrochemical biosensors offer an alternative approach for detecting Candida cells by leveraging their electrochemical properties.22 For instance, amperometric23 and potentiometric20 biosensors utilize the measurement of current or potential changes, respectively, upon Candida interaction. These biosensors demonstrate good sensitivity, simplicity, and cost-effectiveness, but they may suffer from limited selectivity due to non-specific interactions.
Impedance-based biosensors,24,25 which measure changes in electrical impedance resulting from Candida-cell interactions,26,27 have shown promise in addressing the limitations of previous biosensors. They provide high sensitivity, simplicity of fabrication, and excellent selectivity for Candida detection; in fact, sometimes they can even discriminate between different species of Candida with good sensitivity.28,29 Further, impedance-based biosensors offer real-time and label-free detection, enabling rapid analysis of samples without additional reagents. In this scenario, they have the potential to improve early diagnosis and accuracy in detecting candiduria due to all their advantages, while overcoming the disadvantages of the currently most widely used techniques (such as time and cost).
The use of screen-printed electrodes (SPEs) makes them cost-effective and reliable. The increasingly widespread use of SPEs in recent years could lead to acceleration in the development of SPE-based electrochemical sensors in various fields, including health monitoring.30 However, several limitations can arise, including robustness and reproducibility, due to variations in the working surface of each electrode, even if minimal, and the different conditions of manual drop-by-drop functionalization.31,32
In fact, electrochemical measurements are often conducted by incubating SPEs in various solutions. This serves two primary purposes: i) functionalizing the surface of the working electrode with antibodies, and ii) facilitating interaction with the analyte to be detected. The actual measurement is then performed in an electrolyte solution. However, this procedure leads to poor measurement reproducibility. The main issue arises because in addition to binding to the working electrode, both the antibodies and the analytes may also bind to the other two electrodes (auxiliary and counter electrodes). To address this challenge, we developed a microfluidic system that allows solutions to interact exclusively with the working electrode before SPEs are manually introduced into the electrochemical cell. It's worth noting that the use of microfluidics inherently reduces the operator dependence. With this approach, we have not only improved the performance of the biosensor but also minimized operator-related variability.
Gold screen printed electrodes (AuSPEs) were purchased from BVT Technologies (Stražek, Czech Republic). They consist of a gold disk-shaped working electrode (d = 1 mm), a silver/silver chloride reference electrode and a gold counter electrode. These three electrodes were printed onto a corundum ceramic base measuring 0.7 × 2.5 cm2. All potential values were referred to the silver/silver chloride reference electrode.
Bacterial strain E. coli ATCC 25922 was grown in Muller Hinton broth (MHB, Becton Dickinson Difco, Franklin Lakes, NJ, USA) and on tryptic soy agar (TSA; Oxoid Ltd., Hampshire, UK). In all the experiments, bacteria were inoculated and grown overnight in MHB at 37 °C. The next day, bacteria were centrifuged and solubilized in 1× PBS at the desired cell densities (101–106 CFU mL−1). By colony counting assays, it was verified that bacterial growth was negligible in 1× PBS with respect to MHB through a time interval of 3 hours at room temperature, whereas bacterial death was not observed.
EIS measurements were performed at frequencies that ranged from 0.5 Hz to 10000 Hz at a formal potential of 0.16 V and using an amplitude perturbation of 10 mV.
The interaction of the Candida cells with the working electrode of the SPE was realized using a customized fluidic cell featuring an inlet that exclusively targets the working surface while keeping the auxiliary and reference electrodes isolated from the solutions. This cell is shown in Fig. 1b, in which the microfluidic cell is depicted in X-ray view, providing a clear visualization of the specific geometry utilized to selectively wet the working electrode without affecting the adjacent two electrodes.
In fact, microfluidics plays a crucial role in enhancing the capabilities of EIS and its integration with EIS offers several advantages for impedance-based biosensors. Firstly, microfluidic devices enable precise control and manipulation of fluid flow, allowing for a uniform distribution of samples and reagents across the sensing area. This uniformity ensures consistent and reliable measurements, minimizing variations that may arise from manual handling. Secondly, microfluidic channels can be designed to optimize the interaction between Candida cells and the electrode surface.
In this regard, by controlling the flow rate, cell concentration, and flowing time, the detection sensitivity can be optimized. The confined microscale environment also facilitates efficient mass transport, ensuring enhanced sensitivity and faster response times.
Fig. S1a† shows the CV scans obtained before and after the cleaning procedure. The CV signal is that obtained after six scans in the range −0.6 V to +0.6 V, with a scan rate of 0.1 V. The CV scan after cleaning shows an increase in current, indicating a cleaner surface. Moreover, this procedure allowed us to measure the redox potential of the Fe(CN)63−/Fe(CN)64− solution, ultimately obtaining the formal potential of the redox couple for the subsequent EIS measurements. It is worth noticing that after cleaning, a reduction in impedance is also observed (as illustrated in Fig. S1b†); in particular, a lower RCT is revealing of a cleaner surface.
Frequently, the ideal capacitor CDL is replaced by a constant phase element CPE (Fig. S2c†) to account for inhomogeneity and defect areas of the biological layer. This element can fit the imperfect behaviour of the double-layer capacitance due to the porosity or the roughness of the electrode area.
A version of the Randles circuit reported in Fig. S2c† was used to find RCT from the Nyquist plots at the various target concentrations. To this aim, we relied on a tool from the PSTrace 5.5 software that used the Levenberg–Marquardt algorithm.
As is evident from Fig. 2, even the bare SPEs show different behavior (Nyquist plot and Rct) after the cleaning procedure – a feature that is unavoidable with typical commercial electrodes. To take into account the electrode variability, we normalized the change of the charge transfer resistance to its initial value Rct bare
![]() | (1) |
As a further check of the binding kinetics of Abs to the surface, we fixed the flow rate at 450 μL min−1 and measured rf after several functionalization stages. The results are reported in Fig. S4,† from which we deduced that n = 4 stages are sufficient to achieve saturation, i.e., an electrode surface fully covered by Abs.
Since the degree of surface coverage by antibodies plays a crucial role in the charge transfer impedance, we wondered whether n ≥ 4 (surface fully covered by Abs) led to an optimal response for EIS, or rather, a surface with a lower degree of coverage could give rise to a stronger variation of Rct. The reason behind this question is that when the surface is fully covered, it may restrict the current variations resulting from target recognition, ultimately hampering the resistance change. To determine the optimal degree of surface coverage, we measured the change in Rct induced by a relatively low concentration of C. albicans (102 CFU mL−1) using electrodes that underwent different stages of functionalization (n = 1, 2 and 4). The results are shown in Fig. 3 from which one can immediately see that the change of the charge transfer resistance – i.e., the difference of Rct measured after and before the target is conveyed to the cell – is larger for n = 1 [Fig. 3(a)]. In fact, Rct increases as n goes from 1 to 4 as a result of more Abs on the electrode, but this condition is not beneficial for the sensitivity.
With the same arguments used to define rf, we can define the ratio rs, which is due to the target recognition, as follows:
![]() | (2) |
The results are shown in Fig. S5† in which the errors arise from measurements carried out in duplicate or triplicate, whereas the experimental data were fitted by a logistic function. The shaded area represents the no-signal region when the 3SD criterion is adopted. In this case, the signal threshold is set above the control by 3 standard deviations. The relatively high uncertainty in the signal measured for the control can be attributed to fluctuations in the protein content of GYP, which is relatively high. It is evident that since the electrode surface was not fully covered, these proteins are capable of binding to the electrode in a non-specific manner. Nevertheless, even under these unfavorable conditions, a limit of detection of 102 CFU mL−1 can be safely deduced from Fig. S5.†
A comparison of the data obtained in urine with those measured in GYP (Fig. S5†) reveals a lower control value – as well as a lower uncertainty – in urine than in GYP. This significant difference has a notable influence on the limit of detection because, by applying the 3SD criterion (shaded area in Fig. 4), we can reach a value of 10 CFU mL−1. As previously observed, this can be attributed to the high protein content in GYP. In fact, despite being a real sample, urine typically has a much lower concentration of analytes that could potentially interfere with the impedance measurement.
The presence of proteins in GYP can also explain the larger dynamic range exhibited by the detection of cells in urine. The dose–response curve suggests an asymptotic value for rs of approximately 3, whereas in GYP, a saturation value of approximately 0.8 is observed. In fact, the presence of analytes (proteins) capable of binding to the partially covered electrode surface inherently reduces the effective area available for detection, thereby limiting the maximum detectable concentration.
An aliquot of urine of 1 mL was incubated with E. coli at a concentration of 106 CFU mL−1 and made to flow through the circuit for one hour at room temperature.
Subsequently, a washing step with PBS (0.01 M) was performed for 15 minutes to remove any non-specific bonds or contaminants. Fig. 5, which illustrates the changes in Rct, demonstrates that the charge transfer resistance is only slightly higher than that of the negative control (1 mL of urine), whereas it is significantly lower than the value measured in C. albicans at the same concentration. This outcome was somewhat expected since we intentionally employed a surface that was not fully saturated with antibodies to enhance the visibility of the target microorganism. However, due to their smaller size, the bacteria may exhibit some interference. Nevertheless, in view of its application, we can confidently conclude that the specificity of the biosensor described here is more than satisfactory.
![]() | ||
Fig. 5 Specificity test. At the same concentration of 106 CFU mL−1, the signal from C. albicans is approximately four times larger than that from E. coli. |
The measurement with the biosensor provided the value rs = 0.75 ± 0.10 that corresponds (see Fig. 4) to a cell concentration in the range 1–2 (×104) CFU mL−1, which is in satisfactory agreement with the value achieved from the cell culture.
The gold surface of the electrode was functionalized with antibodies using a UV-activation technique known as the Photochemical Immobilization Technique (PIT)34 – a procedure recently recognized for its remarkable effectiveness in tethering Abs to gold surfaces.39 The change in charge transfer resistance (Rct) served as the indicator of the presence of C. albicans.
Interestingly, we found that for targets as large as fungi, partial coverage of the surface resulted in a stronger signal that allowed us to achieve a limit of detection of 10 CFU mL−1 in urine. While this limit can generally be reached or exceeded (at least in simple matrices), it is noteworthy that our biosensor utilizes commercial screen-printed electrodes, which we incorporated into a fluidic design to optimize the interaction between the target and the surface. As a result, we were able to measure the concentration of C. albicans in urine in less than 90 minutes with a procedure that is virtually independent of the operator.
Given the simplicity of the equipment required to carry out the measurements, our biosensor lends itself as a point-of-care device. Moreover, both the cell and the fluidic components can be easily upgraded to create a multiplexing device. Overall, the combination of microfluidics and electrochemical impedance spectroscopy described here offers significant advantages only in terms of improved sensitivity, enhanced throughput, and precise control of fluidic parameters.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3sd00209h |
This journal is © The Royal Society of Chemistry 2023 |