Open Access Article
Kira L.
Rahn
,
Sommer Y.
Osman
,
Quinlan G.
Pollak
and
Robbyn K.
Anand
*
Department of Chemistry, Iowa State University, 1605 Gilman Hall, 2415 Osborn Drive, Ames, IA 50011-1021, USA. E-mail: rkanand@iastate.edu
First published on 23rd November 2023
The COVID-19 pandemic highlighted the importance of designing sensitive and selective point-of-care (POC) diagnostic sensors for early and rapid detection of infection. Paper-based lateral flow assays (LFAs) are easy to use, inexpensive, and rapid, but they lack sensitivity. Preconcentration techniques can improve the sensitivity of LFAs by increasing the local concentration of the analyte before detection. Here, ion concentration polarization (ICP) is used to focus the analyte, SARS-CoV-2 Spike protein (S-protein), directly over a test line composed of angiotensin converting enzyme 2 (ACE2) capture probes. ICP is the enrichment and depletion of electrolyte ions at opposing ends of an ion-selective membrane under a voltage bias. The ion depleted zone (IDZ) establishes a steep gradient in electric field strength along its boundary. Enrichment of charged species (such as a biomolecule analyte) occurs at an axial location along this electric field gradient in the presence of a fluid flow that counteracts migration of those species – a phenomenon called ICP focusing. In this paper, running buffer composition and pretreatment solutions for ICP focusing in a paper-based LFA are evaluated, and the method of voltage application for ICP-enrichment is optimized. With a power consumption of 1.8 mW, S-protein is concentrated by a factor of 21-fold, leading to a 2.9-fold increase in the signal from the LFA compared to a LFA without ICP-enrichment. The described ICP-enhanced LFA is significant because the preconcentration strategy is amenable to POC applications and can be applied to existing LFAs for improvement in sensitivity.
The need for increased sensitivity of selective point of care (POC) biosensors has been made emergent by the COVID-19 pandemic.1–4 The virus is contagious, by both symptomatic and asymptomatic individuals. Testing methods that facilitate early diagnosis are required to administer early treatment for at-risk individuals, decrease the spread of the virus, and track case rates for resource allocation. An ideal diagnostic test would be rapid, inexpensive, sensitive enough for early diagnosis, and not require trained personnel.4–6 Amplification strategies, like reverse transcription polymerase chain reaction (RT-PCR), are extremely sensitive and selective, however they require long times, expensive equipment, and trained technicians to perform.1,4
LFAs are ideal POC sensors for rapid and inexpensive diagnosis, however they lack sensitivity.1,5,6 In a LFA, the antigen-containing sample is flowed across a paper strip containing a test line composed of an immobilized capture probe that selectively binds to the antigen.6,7 A transduction element is present in the assay to indicate presence or absence of the analyte. For example, a detector antibody that binds to the antigen and is conjugated to a Au nanoparticle can be added to the assay for colorimetric detection. The typical sensitivity of a LFA is on the order of 10 μM.1 Increasing the sensitivity LFAs is important so that infectious diseases, like COVID-19, can be diagnosed earlier in the disease progression. There are three main strategies for increasing the sensitivity of a LFA: develop higher affinity biorecognition elements, improve transduction techniques, and preconcentrate or amplify the antigen.1,5,7,8 Preconcentration methods are attractive because these techniques can be applied to any LFA.
Existing strategies for improving the sensitivity of LFAs with preconcentration include the use of isotactophoresis,8 magnetic fields,9 two-phase micellar systems,10 and pressure.11 While these methods improve the sensitivity of LFAs, they require several user steps that may add to user-to-user reproducibility issues. ICP is an attractive method for further improving the sensitivity of LFAs because beyond sample addition, the only user-required step is to push a button to turn on a power source (such as a battery). Additionally, the enriched plug can be held directly over the test line for an extended period, allowing for improved binding of the antigen to the capture probe.
ICP is an electrokinetic technique where background electrolyte ions are simultaneously depleted and enriched at opposing ends of an ion-selective structure in the presence of an electric field to form an ion depleted zone (IDZ) and ion enriched zone (IEZ).12–14 A local electric field enhancement is formed within the IDZ, and charged analytes are focused along the electric field gradient at the boundary of the IDZ when electro-migratory and convective velocities are balanced. Several groups have already demonstrated the use of ICP focusing in a paper-based device.15–21 Han and coworkers patterned Nafion, an ion selective membrane, on tape and showed that 300-fold preconcentration of a protein could be achieved in a cellulose strip.15 Frequently, the voltage to induce ICP is applied between two electrodes, one in the sample inlet and one in contact with the cation selective membrane.15,16 Kwak and co-workers showed, in a microfluidic channel, that by applying the voltage directly to two Nafion membranes, improved preconcentration was achieved and the location of the focused plug remained more stationary.22 Kim and co-workers also used this double-gate design to preconcentrate β human chorionic gonadotropin (β-HCG), the protein detected in pregnancy LFAs, using a battery-operated device.17 Notably, preconcentration of the target was performed before the assay and off-strip, instead of directly over the test line. After preconcentration, Kim and co-workers introduced the enriched plug to the LFA strip and allowed the target to flow downstream for β-HCG detection. While they were able to preconcentrate the antigen by a factor of 25, the overall improvement to sensitivity remained 2.69-fold. We hypothesize that enriching the antigen off-strip and subsequently flowing the focused plug onto the LFA led to diffusional broadening and a decreased interaction time between the antigen and the antibody. Further work from this group improved upon this design by incorporation of rolled paper disks for the anode, cathode, and collection area.23 By application of 150 V, SARS-CoV-2 IgG from serum was preconcentrated and then added to a commercial LFA with a 32-fold improvement in the LOD. Recently, an ICP-integrated LFA has been demonstrated by enriching SARS-CoV-2 nucleocapsid protein directly over the commercial test line to achieve an enrichment factor greater than 10.24 Most interestingly, the addition of stacked paper layers between the cation exchange membrane and the paper strip inhibited pH changes that can occur when the acidic Nafion membrane is in direct contact with the LFA.
Here, we demonstrate the ICP-driven enrichment of an antigen directly over the capture probes in a LFA that results in binding of the antigen-probe pair. A Pluronic solution is identified as a low-conductivity solution compatible with ICP that also works as a pretreatment solution to attenuate non-specific adsorption of the antigen in the nitrocellulose membrane. Similarly, HEPES buffer is identified as an ICP and biocompatible buffer due to its low conductivity and buffering range. We optimize the device configuration to obtain a reproducible and stationary enrichment location that spans the width of the test line in the LFA. We quantify the impact of magnitude of voltage application and time of voltage application on the binding of the focused antigen to the capture probe. We demonstrate that the ICP-enhanced LFA improves the sensitivity by a factor of 2.9. Combined, these results demonstrate a new platform for improving the sensitivity of LFAs with ICP focusing.
.8,25,26 The Damköhler number (Da) is the ratio between maximum reaction and diffusion rates and is often used to determine if the reaction is in a mass transport limited or kinetically limited regime.8,25,26 If Da ≫ 1, then the rate is limited by mass transport (diffusion and convection), while if Da ≪ 1, the rate is limited by kinetics. For a LFA in nitrocellulose,
where
p0 is the surface concentration of capture probe, d is the nitrocellulose pore radius, and D is the diffusivity of the antigen in the nitrocellulose membrane.8 Typically d is the channel height, but since the channel is composed of porous paper (nitrocellulose membrane), the pore radius was chosen as the characteristic length for diffusion of the proteins.8 For our assay in the absence of ICP, we estimate Da to be on the order of 10−4 indicating that the assay is kinetically limited (see the ESI† for more details on this calculation).
If we assume perfect mixing and that convection and diffusion supply the antigen to the capture probe faster than the reaction kinetics (i.e., we are in a kinetically limited case), and the concentration of the antigen near the capture probes is approximately equal to the concentration of the antigen added, then the fraction (hlfa) of the surface concentrations of bound capture probes (
b) to
p0 can be estimated by eqn (1):8,25,26
![]() | (1) |
is the initial molar concentration of the antigen in the immediate vicinity of the capture probes normalized by KD. See the ESI† for a derivation of eqn (1).
For an interpretation of the relationship in eqn (1), it is useful to consider the assay at two concentrations of antigen added to the assay. When a 1.3 nM solution of S-protein is added to the assay, 99% of the capture probes that will bind to the antigen will be bound within 12 min. The fraction of capture probes that will bind is approximately 0.4% of the total probes. On the other hand, when a 10-fold more concentrated solution of antigen is added (13 nM solution of S-protein) to the assay, 4% of the total probes will bind, with 99% of those probes binding within 11.6 min. In other words, the 10-fold increase in concentration of antigen (1.3–13 nM) should yield an approximately 10-fold increase in percent of bound capture probes. In the 13 nM case, it takes 1.7 min for 2% of the probes to bind and 3.5 min for 3% of the probes to bind. These cases highlight the importance of (1) increasing the local concentration of the antigen over the capture probes and (2) allowing sufficient time for the complex formation to occur so that a higher proportion of capture probes will be bound to the antigen at equilibrium.
The mechanism for ICP in our LFA is depicted in Scheme 2. As shown in Scheme 2a, upon addition of the sample to the sample pad, the background electrolyte initially spreads evenly through the nitrocellulose membrane. When voltage is applied, the cations (blue circles) migrate towards the cathode, travel through the cation-selective membrane, and are consumed or balanced by electrochemical reactions. Meanwhile, anions (red circles) migrate towards the anode and accumulate around the cation-selective membrane. Cations are produced by electrochemical reactions at the anode and accumulate near the anions to satisfy charge neutrality. In time, an IEZ is formed near the anode, while an IDZ is formed near the cathode. A steep electric field gradient exists between the IDZ and IEZ, depicted in Scheme 2b, where the analyte (green circle) is enriched in the position where its electrophoretic (vel) and convective (vc) velocities are balanced. The test line of the LFA is aligned at the position where focusing occurs (Scheme 2c).
Current voltage curves (CVCs) are often obtained for ICP devices to characterize the system.19,20 In a CVC, the voltage applied to the device is increased as the current is measured. There are three regions in a CVC: the ohmic region, the limiting region, and the over-limiting region. At low voltages, the IDZ and IEZ have not yet formed. The Nafion-coated electrodes and sample-soaked nitrocellulose membrane act as a resistor. Therefore, by Ohm's law, the current is equal to the voltage applied divided by the resistance of the device. The slope of the CVC is linear and constant in the ohmic region. As the voltage increases further, the IDZ forms. This region of the CVC is called the limiting region because the resistance is increasing due to the depletion of ions, limiting the current through the device. Increasing the voltage even higher can lead to the formation of electroconvective vortices that allow the IDZ and IEZ to mix. This mixing allows ions to pass through the depletion zone, so the current can again increase. In cellulose-based devices, another region of limiting-current can be observed because the size of the electroconvective vortices is confined by the fibers in the cellulose.20
For LFAs with ICP-enrichment, the backing card and microfluidic diagnostic tape with Nafion-coated electrodes described above were used. First, the Nafion-coated electrodes were dried by blotting on a lint-free wipe. Cu tape was attached to the AgCl electrodes to connect the device to a power supply. Then, the nitrocellulose membrane was aligned so there were 5.0 mm between the membrane and the AgCl electrodes. The Nafion-coated electrodes on the diagnostic tape were aligned on top of the nitrocellulose membrane and backing card and sealed. Sample and waste pads were attached to the backing card, overlapping the nitrocellulose membrane.
The assembled devices were used immediately. A pipette was used to deliver 300 μL of the sample solution (composed of the analyte, the buffer, and 0.05% Tween-20) to the sample pad. If ICP-enrichment was performed, the voltage was turned on immediately after the solution had wicked across both anodic and cathodic Nafion membranes. The fluorescence intensity was monitored with a SMZ800N stereoscope (Nikon Industries, New York, NY) equipped with a Sola Lumencor Light engine (Lumencor, Beaverton, OR) and Photometrics Cool Snap Dyno camera (Tucson, Arizona).
Our first challenge in developing an ICP-enhanced LFA was determining the best way to establish contact between the Nafion-coated electrodes and the nitrocellulose membrane. We attempted to use magnets and Scotch double-sided tape to attach Nafion-coated AgCl electrodes that were painted on transparency film to the top on the LFA (see Fig. S1†). While enrichment occurred, we realized that the contact between the Nafion and the nitrocellulose membrane would be improved if the Nafion were painted on an adhesive that could stick directly to the nitrocellulose membrane, and not just the tape around it (see Fig. S2†). Therefore, we used the microfluidic diagnostic tape as the backing for the Nafion-coated electrodes and attached it and the sample pad, nitrocellulose membrane, waste pad to an adhesive backing card. Not only did the Nafion maintain good contact with the nitrocellulose membrane, but the added benefit in lamination was that evaporation of the sample was decreased so that the assays could be performed for longer times.
![]() | ||
| Scheme 3 Schematic of the three configurations of Nafion-coated electrodes – (a) double-gate, (b) sandwiched double-gate, and (c) flipped sandwich double-gate configurations. | ||
The device design was improved by sandwiching the nitrocellulose membrane with two sets of Nafion-coated electrodes, shown in Scheme 3b. The resistance of a substance is proportional to the length divided by the cross-sectional area. By sandwiching the nitrocellulose membrane with two Nafion membranes, the contact area was increased and therefore, the resistance of the system was decreased. The CVC for the sandwiched double-gate design is shown in Fig. 1a (blue line). The decreased electrical resistance of the Nafion-coated electrodes can be quantified by comparing the slopes of the of the ohmic region in the CVC for each configuration. The slope of the double-gate configuration is 9.0 μA V−1, while the slope of the sandwiched double-gate configuration is 18.3 μA V−1. Since the contact area was doubled, this increase in the slope by a factor of 2.03 is expected. In the ohmic region of the CVC, the slope is equal to the inverse of the resistance. Therefore, a steeper slope indicates a lower resistance, indicating that the sandwiched double-gate design is less resistive than the single-layer double gate design. The average fluorescence intensity of the enriched plug was higher in the sandwiched double-gate design than the single-layer design (Fig. 1b), with maximum EFs of 4 ± 1 and 2.1 ± 0.8, respectively. Additionally, the uniformity of the enriched plug in the x-direction (perpendicular to the nitrocellulose membrane), shown in Fig. 1c and d, is improved in the sandwiched double-gate design compared to the double-gate design.
Pretreatment of the LFA was required to decrease non-specific adsorption between the charged protein and the nitrocellulose membrane. The pretreatment solution from Lee and co-workers (composed of 10 mM 2-amino-2-methyl-1-propanol (pH 9.0), 0.5% BSA, 0.5% β-lactose, 0.05% Triton X-100, 0.05% sodium azide)32 as well as a commercially available LFA pretreatment solution, Stabilgaurd,33 were first used. Both pretreatment solutions resulted in poor flow of the S-protein in the nitrocellulose membrane and minimal enrichment (see Fig. S3†). Pluronic is a triblock copolymer composed of hydrophilic tails and a hydrophobic center often used in polydimethylsiloxane (PDMS)-glass microfluidic devices to increase the hydrophilicity and decrease nonspecific adsorption of biomolecules to the PDMS surface.34 Pretreatment of the nitrocellulose membrane and sample pads with 1.0 mM Pluronic F-127 solution yielded better flow of the protein in the nitrocellulose membrane and improved enrichment.
Unfortunately, the S-protein in the nitrocellulose membrane flowed slowly past the cathodic Nafion-coated electrode. We hypothesized that the low concentration and volume of Tris buffer (100 mM) did not have a sufficiently high buffering capacity to negate acidification of the adjacent segment of the nitrocellulose membrane by Nafion. Additionally, the location of the enriched plug was near the anodic Nafion-coated electrode, meaning that the test line would be slightly overlapping with the acidic Nafion. Binding of S-protein to ACE2 is pH dependent (see Fig. S4†), with the best binding occurring around pH 7 (see ESI† for evidence). For these reasons, we investigated alternative buffers for our ICP-enhanced LFA.
Two candidates were investigated: HEPES and Bis-Tris propane. Both buffers were chosen because they have two acidic protons and therefore larger buffering ranges. Additionally, both molecules are bulky and have lower conductivity than other biological buffers, which is important to minimize Joule heating and to prevent formation of gas bubbles by electrolysis at the electrodes. To obtain a biological pH for Bis-Tris propane, a high conductivity was obtained from the addition of acid. The enrichment was minimal and near the anodic Nafion-coated electrode because of the difficulty to deplete the high concentration of ions (see Fig. S5†). HEPES buffer was used in further experiments because its conductivity was low (2.0 mS cm−1), and the focused plug of S-protein was not overlapping with the Nafion-coated electrodes. It's important to note that enrichment is demonstrated in “neat” buffer and would need to be adapted to clinical samples. While ICP has been successfully demonstrated in biofluids, such as urine35 and blood,36 the high ionic conductivity of biological samples is challenging to ICP focusing. Moreover, interfering proteins present in the sample co-enrich and can drive lower mobility targets, such as nucleic acids, upstream.37 Reduction in non-specific binding can aid in preventing false positives that would be given by interfering proteins. We envision the ICP-enhanced LFA could be utilized for the analysis of patient nasal swabs, if a low salinity viral transport medium is prepared. Universal viral transport mediums are typically formulated with balanced salt solutions and can be buffered to an ideal pH with HEPES.38 Future studies will determine the highest ionic strength compatible with the ICP-enhanced LFA in order to avoid dilution of samples prior to enrichment.
The flipped sandwich configuration (depicted in Scheme 3c) was chosen over the sandwiched configuration because the focused plug was more uniform in the x-direction (perpendicular to the nitrocellulose membrane), as demonstrated in Fig. 2c and d. This asymmetric focused plug occurs because the electric field is not uniform across the width of the nitrocellulose membrane due to the highly resistive nature of both the Nafion membranes and the nitrocellulose membrane. By flipping the top layer of Nafion-coated electrodes, we are applying the voltage at both the top and bottom edges of the nitrocellulose membrane, resulting in a more uniform electric field and focusing pattern.
As shown in Fig. 3a, the enriched plug consists of two spots of enrichment in a line perpendicular to the nitrocellulose membrane. To increase the uniformity of the enriched plug in the y-direction (parallel to the nitrocellulose membrane), the width of the nitrocellulose membrane was decreased from 5.0 mm (Fig. 3a) to 1.0 mm (Fig. 3d). The gap between the two enriched plugs decreased as the width decreased, until ultimately the focused plug formed a single band across the entire width of the nitrocellulose membrane.
From a CVC of the new configuration with a 1.0 mm-wide nitrocellulose membrane (Fig. S6†), HEPES buffer and the flipped-sandwich Nafion configuration, the onset voltage for ICP is maintained at 13 V. However, the change in width increased the resistance of the device, further decreasing the total current throughout the device. The maximum current in the CVC was attenuated from 140 ± 40 μA to 22 ± 3 μA, which is favorable for the adaptation of this device to point of care applications, because low power requirements (1.8 mW) can be powered by a battery-operated device.
The signal enhancement (SE), defined as the average fluorescence intensity of the test line after the assay is complete divided by the average fluorescence intensity of the test line immediately after the test solution has wicked across the test line, of the LFA with ICP-enrichment at t = 40 min was 4.1, while the SE for the LFA without ICP-enrichment at t = 40 min was 1.3. Interestingly, the initial average fluorescence intensity of the nitrocellulose membrane just after the solution has wicked across the test line (i.e., the denominator in the SE calculation) is lower for the LFA with Nafion-coated electrodes than without (37.6 RFU and 91.4 RFU, respectively). We hypothesize that this decrease in fluorescence intensity occurs because the acidic Nafion membranes still disrupt the flow of the S-protein across the strip. When reading a paper-based LFA, a positive result is determined by the user identifying the presence of a line. In the context of our LFA where the antigen is conjugated with a green-fluorescent dye, a green test line will be easier to see against a lower background intensity of the surrounding part of the nitrocellulose membrane. Therefore, we will compare the SE instead of the average fluorescence intensity of the test line when comparing the performance of the LFA configurations.
Recent studies have demonstrated that the net charge of S-protein changes with different variants of SARS-CoV-2.39 A change in the charge of a molecule will result in a change in electrophoretic mobility, which may alter the axial position where the molecule is focused. This property may alter the location that the test line should be aligned because the analyte may focus in a different location. However, we believe that the change in focusing location will be minimal for the variants of S-protein because the percent change in the charge of the protein is small; according to Pawłowski, the formal charge of wild-type S-protein is −12 elementary charge units (e) and mutations have resulted in a net change to the formal charge of S-protein by −1, 0, 1, or 2e.39 Others report that the net charge of the surface of the folded S-protein is −32e.40
Fig. 5 shows the average fluorescence intensity of the test line over time for two cases; one where 80 V was directly applied to the Nafion-coated electrodes, and one where the voltage is ramped to 80 V at a rate of 1.0 V per 10 s (n = 3). The voltage is applied for 20 min in each case. The average maximum fluorescence intensity is slightly higher for the ramped case, as shown in Fig. 5a, but more importantly the standard deviation of the fluorescence intensity between each trial (indicated by error bars in Fig. 5a) was lower for the ramped case than the direct voltage application case. By comparing the fluorescence intensity of the enriched plug to a calibration curve of fluorescence intensities of distinct protein concentrations (0.1 to 100 μg mL−1) in the nitrocellulose membrane (Fig. S7†), the enriched concentration could be calculated. It was found that the enriched plug was 16.7-fold higher than the initial concentration added for the ramped voltage case, and 14.3-fold higher for the direct voltage case.
The SE of the region of the nitrocellulose membrane containing the test line 20 min after the voltage had been turned off in an ICP-enhance LFA is plotted in Fig. 5b for the two voltage application methods. To account for day-to-day variability of the test line, the SE is normalized (nSE) by the SE of an LFA without ICP-enhancement taken on the same day. Therefore, an nSE of 1.0 would indicate that the ICP-enhanced LFA yielded the same SE as an LFA without ICP-enhancement. The average nSE for the direct voltage case was 2.0 ± 0.4, while for the ramping case the enhancement was 1.7 ± 0.7, which are not significantly different (p = 0.33). The lack of reproducibility of the location of the enriched plug led us to the conclusion that ramping the voltage in an ICP-enhanced LFA is more favorable.
After determining the optimal voltage for ICP-enrichment, the optimal time for enrichment was investigated. Fig. 6c shows the average fluorescence intensity over the region containing the test line over time for this investigation. In each case, the voltage was ramped to 80 V at a rate of 1.0 V per 10 s and then held at the maximum voltage for a total time of 15 min, 20 min, or 30 min. Notably, the scale for the average fluorescence intensity in Fig. 6c is lower by a factor of 4 than the scale for Fig. 6a. This change is because the initial concentration of S-protein in our sample solution was decreased by a factor of 4. It was found that 20 min and 30 min yielded statistically similar improvements (p = 0.5) to average fluorescence intensity of the test line after voltage application, shown in Fig. 6d, likely because we had reached saturation conditions. Both enrichment times yielded significantly improved enrichment than the 15 min enrichment time (p = 0.03 for 20 min and p = 0.01 for 30 min). Therefore, 20 min was chosen as the optimal enrichment time because for a POC device, a faster test is more favorable.
The improvement to the sensitivity of the LFA with ICP-enrichment compared to the LFA without ICP-enrichment was calculated by dividing the slope of the linear portion of the calibration curve with enrichment by the slope of the linear portion of the calibration curve without enrichment, shown in Fig. 7. We found that the ICP-enriched LFA yielded a 2.9 ± 0.5-fold higher signal than the LFA without enrichment. On average, there was a 21 ± 4-fold increase in concentration of S-protein over the test line during enrichment. Using eqn (1), the expected improvement of the amount of S-protein that binds to the test line with an increased concentration of S-protein can be calculated by comparing the limit of the amount bound to the test line (hlfa), which is equal to
. For example, the maximum increase in concentration for the ICP-enhanced LFA with 0.4 μg mL−1 S-protein was 21-fold; this increase in concentration should have led to a 16-fold increase in the amount of S-protein bound to the test line. However, only a 1.6-fold increase was observed.
We hypothesize that the improvement to the amount of S-protein bound to the test line is not as high as expected for several reasons. First, the enriched plug does not cover the entire test line area, but we report the average fluorescence intensity of the entire test line area. For example, in one LFA with ICP-enrichment the average SE for the total area of the test line was 2.3, while the average SE for a smaller portion of the test line where S-protein was focused was 4.3. Second, we are using dissociation constant measurements from Lee and co-workers;32 the kinetics are likely different in our assay because both the S-protein and the ACE2 capture probes are conjugated to dyes. If the dissociation constant is in fact lower by a factor of 90, for example, then the expected improvement of the amount of S-protein that binds to the test line following 21-fold enrichment is only 1.6-fold (not 16-fold), indicating that the binding kinetics could be better than what is reported by Lee and co-workers. Third, after enrichment, the voltage is turned off and the test line is exposed to sample solution that does not have as high a concentration of S-protein as the enriched plug. In other words, before we measure the SE, we allow the enriched plug to wash off of the test line so that S-protein that is not bound is not counted in our measurement. Because the amount of the S-protein that is bound to the test line is in equilibrium with the unbound S-protein, we may be losing protein that was bound during enrichment during this wash period. Lastly, it is possible that the protein structures have been altered or denatured due to a change in temperature from Joule heating, and pH and salt concentration between the Nafion membranes, which can decrease the binding affinity. Incorporation of the previously reported paper stacks between the Nafion and LFA23 may help to address this issue, while preserving our disposable membrane-coated electrode design that is most suited to the POC. We hope to answer these questions with future studies in our lab.
Future improvements to this ICP-enhanced LFA include the addition of a detector antibody conjugated with a Au NP so that the LFA can be read by eye or a with a camera instead of requiring fluorescence detection. Additionally, the device design will be modified further to increase the electric field strength in the region containing the capture probes and therefore improve the enrichment of the antigen to improve binding to the capture probes. Ultimately, we aim to improve the sensitivity of the ICP-enhanced LFA and the amenability of the proposed platform for POC applications.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: https://doi.org/10.1039/d3ay00990d |
| This journal is © The Royal Society of Chemistry 2024 |