H. Yoshikawa*,
M. Yoshinaga and
E. Tamiya
Department of Applied Physics, Osaka University, Suita, Osaka 565-0871, Japan. E-mail: yosikawa@ap.eng.osaka-u.ac.jp
First published on 18th April 2018
We evaluated optical pickup ELISA with an original microfluidic disk that contains eight radially arranged channels, which enable semi-automatic sample loading and washing. This disk-shaped chip composed of acrylic plates was fabricated by CO2 laser machining and capture antibodies were immobilized in the channels. After the immunoreaction with antigens and enzyme-linked secondary antibodies, an enzyme-catalyzed nanoaggregation of o-phenylenediamine was detected by measuring the reflectivity change of a laser beam focused in the channel. The assay of C-reactive protein (CRP) was successfully performed in a short amount of time (approximately 20 min from CRP loading). The limit of detection was determined to be 2 ng mL−1, which is more sensitive as compared with conventional ELISA using microplates.
Let us consider signal detection methods used in conventional ELISA.9 Colorimetric assays, including ELISA, are widely utilized in the field of bioanalysis due to their simplicity and high reproducibility. Enzymes such as horseradish peroxidase and alkaline phosphatase, which catalyse the colorimetric change of specific chemical reagents, are usually utilized. Colour changes due to enzymatic reactions are quantitatively evaluated based on optical absorbance measurements. For such colorimetric assays, microtiter plates and plate readers are widely recognized as standard systems, where optical absorbance of the test solution in each well is sequentially and semi-automatically measured. Normally, the degree of colour change (i.e. absorbance) of 100–200 μL of the solution is measured to evaluate the concentration of the target protein at the final stage of the ELISA (Fig. 1a). Since absorbance is proportional to the path length of light passing through the solution, reduced solution volume, i.e. a decrease in the light path length, results in reduced sensitivity for microELISA. In addition, an error in the solution volume results in error in the result of the measurement.
To overcome this obstacle, several signal detection techniques have been used in previous microELISA studies. Representative methods include detection of luminescence, such as fluorescence and chemiluminescence.6,10–12 Luminescence detection is quite sensitive; however, a sensitive photodetector, an excitation light source (for fluorescence), expensive reagents, and a set of optical filters are necessary. Thermal lens detection is also a sensitive method that Kitamori et al. applied to their microELISA systems.13 However, the thermal lens method requires two laser sources and elaborate optical systems to focus two laser beams at different depths. These detection methods may satisfy the sensitivity requirement, but the detection system used are complicated, bulky, and expensive.
As an innovative way to solve the problems inherent in colorimetric-based ELISAs, we propose the application of optical pickup detection of horseradish peroxidase (HRP), which was recently developed by our group.14,15 In principle, this is a method to induce and detect oxidative polymerization (dimerization) of o-phenylenediamine (oPD) using a single laser beam. oPD is a well-known colorimetric reagent used in conventional ELISAs; oxidative polymerization (mainly dimerization) of oPD is catalysed by horseradish peroxidase (HRP), and the reaction product (diaminophenazine: DAP) has an intense colour.9,16 In conventional colorimetric ELISA, this colour change is evaluated by light absorbance. On the other hand, the optical pickup method detects aggregate deposition due to further oxidative polymerization induced by a focused laser beam (Fig. 1b), which is similar to commercial read-and-wright system of optical discs (CD, DVD, and BD). The detection mechanism was explained in detail in previous reports.14,15 The oPD reaction occurs with a laser focus of approximately 1 μm in diameter. As a result, the sample volume necessary in this method is on the scale of several nL–pL, which is much smaller as compared with that of conventional ELISA. In addition, signal intensity is not dependent on the optical path length. Furthermore, a low-power visible laser beam and a general photodetector can be used, which allows for simple, compact, and low-cost optical setup. Therefore, optical pickup detection is expected be highly compatible with microELISA applications.
Assessments using commercial pickup devices for CD/DVD/BD suggested that our optical pickup detection has good compatibility with disk-shaped biosensors, which applies fluidic controlled-pumpless microfluidics based on the centrifugal force.6,17,18 Although sophisticated disk-shaped chips have been designed and developed to minimize manual labour in ELISA, here we propose a disk-shaped chip for optical pickup ELISA with a simple design to semi-automate the washing process. Inadequate or excess washing harms data quality, and individual difference in the washing process results in error. In this paper, we demonstrated for the first time that ELISA with optical pickup detection can be carried out with an original microfluidic disk, which enables semi-automatic sample loading and washing.
o-Phenylenediamine (oPD: Sigma) was dissolved in citrate buffer (pH 4.5) to prepare a 4 mM oPD stock solution. This stock solution was mixed with H2O2 aqueous solution (BioCheck, MB-10024; 0.015% (v/v) H2O2 in 0.1 M citrate buffer, pH = 5.0) at 1:1 ratio just before its use for the HRP specific reaction. Human CRP (BioCheck, BC-1119) was diluted in PBS buffer, and five test solutions (50, 10, 2, 0.4, and 0.08 ng mL−1) were prepared. Each solution was mixed with HRP (horseradish peroxidase)-modified anti-CRP (BioCheck, BC-1119) at 1:5 just before being introduced into each channel of the chip (Fig. 3d). After a 10 min incubation period, the solution was rinsed with washing buffer. Finally, the oPD/H2O2 solution was poured into each channel (Fig. 3e), and optical pickup detection was performed after 10 min (Fig. 3f).
Optical setup was performed as previously described.14 Briefly, the 532 nm line of a DPSS green laser (PHOTOP, DPGL-2100F) was focused onto the interface between the top plate and the oPD/H2O2 solution in a chip channel via a 60× objective lens (Olympus, UPlanFLN), as shown in Fig. 3e. The laser power was approximately 2 mW at the focus. A part of the focused laser beam was reflected at the interface, and the intensity of the reflected beam was measured by a photomultiplier (Hamamatsu Photonics, R1166) at a sampling rate of 50 Hz. Temporal change of the reflected laser intensity was recorded in a PC via a data acquisition board (National Instruments, USB-6341).
As shown in Fig. 2, our microELISA chip has eight channels to load sample solutions into, and the laser beam is focused for pickup detection. In addition, wash solutions flow through the channels by centrifugal force to rinse out excess proteins. Therefore, channel structure is important for sensitivity and data quality. We evaluated optical pickup signals using test microplates, which has channels with different width, length, and height. Fig. 4 shows the temporal change in the reflection intensity of the focused laser beam, i.e. optical pickup signal. The CRP concentration was 100 ng mL−1. In all cases, the intensity of the reflected laser beam was first increased, and was then decreased to form a peak in the intensity variation curve. This intensity change is attributed to the formation of a submicron sized aggregate due to the photo-oxidative polymerization of oPD induced by the laser absorption in the colored solution, as shown in Fig. 1b. The laser irradiation time at the peak (peak time: Tp) represents the reaction time necessary to generate an aggregate with a certain size, and is dependent on the coloring degree of the solution, that is, the concentration of DAP included in the solution prior to irradiation. In the case of optical pickup ELISA, the degree of the enzyme reaction, i.e. the concentration of target biomarkers, is determined from this Tp. Among the three channel widths (Fig. 4a), the 0.5 mm channel yielded the longest detection time (Tp of approximately 25 s) for the optical pickup signal, whereas the difference between the 1 and 2 mm channels is small. The peak times of the 1 and 2 mm width chip were close to each other as compared with that of the 0.5 mm width chip. Channel width wider than 1 mm would also be appropriate; however, increase in channel width requires greater sample volume. Fig. 4b indicated that channel length has minimal effect on detection result in the length scale of 2–6 mm. However, channel height demonstrated a clear relationship with detection time, as shown in Fig. 4c; an earlier peak time onset was associated with reduced channel height. This indicated that the reaction was enhanced by increased surface-to-volume ratio of the solution-filled channel, since antigen–antibody binding and HRP enzyme reaction occurs at the channel surface of the bottom plate to which antibodies are bound.22,23 On the other hand, the surface to volume ratio does not change with the reduction of the channel width. The cause of the width dependence of the sensitivity is under investigation. Hydraulic pressure and/or shear stress on the bottom surface, which depend on the channel shape, may sweep a part of binding antigens/antibodies. Insufficient flow may cause an excess residual of the blocking solution. Thus we believe that the optimal flow rate and the channel shape to maximize the sensitivity exist. Theoretical and simulation analyses are also necessary to discuss deeply such microfluidic properties, but Fig. 4 indicates a channel fabrication guideline for not reducing the sensitivity. Although a channel height shorter than 85 μm is expected to produce faster reactions, the height is determined by the thickness of the commercial PET film, which is used as a spacer to make the channel height. Therefore, we fabricated microELISA chips with a channel width of approximately 3.5 mm and a channel height of 85 μm for the following CRP detections.
Finally, we performed optical pickup microELISA using the optimally designed chip. Fig. 5a shows the temporal change of the reflected laser intensity measured for each CRP concentration. The intensity of the reflected laser beam gradually increased, and reached its maximum at Tp, which is dependent on CRP concentration. Results indicated that higher CRP concentration is associated with shorter Tp. Tp was plotted as a function of CRP concentration with a standard deviation of measurements carried out thrice (Fig. 5b). Fig. 5 indicates that pickup signals at 0.4, 2, 10, and 50 ng mL−1 are distinguishable and the logarithm of the concentration is roughly proportional to the peak time in this range. The limit of detection (Ld) was estimated to be ∼2 ng mL−1 based on the commonly used simplistic way, where Ld was calculated as a standard deviation of the blank multiplied by 3.24 It should be noted that the assay, including the incubation and semi-automatic washing processes, was successfully performed in a short amount of time (approximately 20 min from CRP loading). For comparison, a conventional ELISA of CRP was performed with a microtiter plate (see ESI†). Fig. S2† shows that absorbance at 2 ng mL−1 CRP couldn't be distinguished from that of the blank sample and 10–100 ng mL−1 CRP was quantitatively detected with a microplate based ELISA using the same reagents and incubation times. This demonstrated that optical pickup ELISA is more sensitive as compared with conventional ELISA. This could be attributed to the high surface-to-volume ratio of the microELISA chamber, which enhances chemical reactions, leading to short antigen–antibody incubation (10 min) and oPD reaction (10 min) times.
Fig. 5 (a) CRP concentration dependence of the optical pickup signal. (b) Peak time vs. CRP concentration. |
Footnote |
† Electronic supplementary information (ESI) available: Optical pickup signals obtained with a PMMA and glass substrates, FDTD simulation, and conventional microplate ELISA can be found. See DOI: 10.1039/c8ra01149d |
This journal is © The Royal Society of Chemistry 2018 |