Hideyuki
Arata‡
,
Hiroshi
Komatsu
,
Aishan
Han
,
Kazuo
Hosokawa
* and
Mizuo
Maeda
Bioengineering Laboratory, RIKEN, 2-1 Hirosawa, Wako, Saitama 351-0198, Japan. E-mail: k-hoso@riken.go.jp; Tel: +81-48-467-9312
First published on 22nd May 2012
We present a new method for rapid microRNA detection with a small volume of sample using the power-free microfluidic device driven by degassed PDMS. Target microRNA was detected by sandwich hybridization taking advantage of the coaxial stacking effect. This method allows us to detect miR-21 in 20 min with a 0.5 μL sample volume at a limit of detection of 0.62 nM. Since microRNAs can act as cancer markers, this method might substantially contribute to future point-of-care cancer diagnosis.
Power-free poly(dimethylsiloxane) (PDMS) microfluidic device was fabricated as reported elsewhere17,18 with an additional process of selective immobilization of probe DNA on glass plates. This microfluidic device allows self-pumping by PDMS air absorption without connecting to an exterior power supply. Two PDMS microchannels were used: first for the selective patterning of probe DNA and second for miRNA detection. Symbols and sequences of oligonucleotides, probe DNAs and miRNAs, used in this study are listed in Table 1. The device fabrication process is as follows. First, glutaraldehyde (Wako) was incubated on aminated glass plates (SD00011, 25.4 mm × 76.2 mm, Matsunami Glass Ind., LTD) at 37 °C for two hours. Next, a PDMS microchannel of 100 μm in width and 25 μm in height was formed on the glass plate and degassed in a vacuum chamber for 40 minutes. Amino-labelled DNA (Pro21, Pro141) (Oligonucleotide, Europhins operon) was injected into the channel by power-free pumping and incubated at 37 °C for 30 min. Finally, the PDMS microchannel was detached from the glass plate in stopping buffer (25 mM Tris, 0.05% Tween 20). The glass plate was washed by ultrasonication, with both the stopping buffer and deionized water, to remove the remaining DNA on the surface. The second PDMS microchannel was fabricated and mounted onto the glass plate to form microfluidic devices with several microchannels of 100 μm in width and 25 μm in height (Fig. 1). MiR-21 was adopted as a model sequence since it is one of the most well-known miRNAs as cancer markers.19,20
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Fig. 1 (a) Schematics of the power-free microfluidic device. PDMS absorbs air in the outlet chamber thus being a self-stand pumping device. Probe DNA is immobilized onto the glass surface and microchannels convey the sample to the probe. (b) Schematics of sandwich hybridization. Half of the miRNA sequence is complementary to the fluorescent labeled probe DNA and the other half is complementary to the probe DNA immobilized on the glass surface. |
Symbol | Sequence (from 5′ to 3′) |
---|---|
Pro21 | NH2–TTT TTT TTT TTT TTT TCA ACA TCA GT |
Pro141 | NH2–TTT TTT TTT TTT TTT CCA TCT TTA CC |
ProFlu21 | CTG ATA AGC TA–Fluorescein |
ProFlu141 | AGA CAG TGT TA–Fluorescein |
Pro21full | NH2–TTT TTT TTT TTT TTT TCA ACA TCA GTC TGA TAA GCT A |
MiR-21 | UAG CUU AUC AGA CUG AUG UUG A |
MiR-141 | UAA CAC UGU CUG GUA AAG AUG G |
MiR-ran | UGG UGC GGA GAG GGC CCA CAG U |
MiR-21Flu | Fluorescein–UAG CUU AUC AGA CUG AUG UUG A |
MiR-21Gap | UAG CUU AUC AGU ACU GAU GUU GA |
Two protocols, “Protocol 1” and “Protocol 2”, were conducted to detect miRNA by sandwich hybridization. In protocol 1, fluorescent labelled probe DNA (ProFlu21) was pre-hybridized to miR-21 in an off-chip tube before injecting into the microchannel. In protocol 2, miR-21 was hybridized to Pro21 immobilized in the microchannel, and then ProFlu21 was injected to the microchannel to hybridize to the captured miR-21. All the hybridization processes were carried out at room temperature (∼25 °C) in a blocking solution (BS) (0.01% Roche Blocking Reagent, 0.02% (w/v) SDS, 5 × SSC, 0.05% Tween 20). Protocol 1 was carried out as follows. First, miR-21 was hybridized with ProFlu21 of 1 μM in a tube with the BS for 5 min. During this period, 0.5 μL of the fresh BS was injected into the microchannel and incubated for 3 min. Subsequently, 0.5 μL of the mixture of miR-21 and ProFlu21 sustained in the BS was injected into the channel and incubated for 5 min. Finally, non-hybridized RNA and ProFlu21 were washed out by 1–3 μL of the BS for 10 min. Protocol 2 was carried out as follows. First, 0.5 μL of BS was injected into the channel and incubated for 3 min. Next, 0.5 μL of miR-21 diluted in the BS was injected into the channel and incubated for 5 min. Subsequently, 0.5 μL of 1 μM ProFlu21 in the BS was injected into the channel and incubated for 5 min. Finally, the channel was washed out by 1–3 μL of BS for 10 min. Detection of multiple sequences from a single sample solution was also demonstrated by protocol 1. Specifically, the microfluidic devices with probe DNAs of two different sequences, Pro21 and Pro141, were prepared with the same protocol. The sample solutions with four combinations were prepared: miR-ran in the BS: miR-21 and miR-ran in the BS: miR-141 and miR-ran in the BS: miR-21, miR-141 and miR-ran in the BS. In this demonstration, the concentration of miR-21 and miR-141 was 100 nM and that of miR-ran was 1 μM. In all the experiments, channels were observed by the fluorescent microscopy and images were captured by CCD camera (Photometrix Cool SNAP HQ2). Fluorescence intensities were analysed by software (ImageJ). Three to seven data were used to plot each averages and standard deviations.
With both the protocols, results with the Pro21 patterned devices showed fluorescence intensities in the channel with miR-21 but not in the channel without miRNA (Fig. 2(a)). The fluorescence intensities decreased at lower miR-21 concentrations and showed almost no fluorescence intensity less than 0.1 nM (Fig. 2(b)). The data points were fitted with the four-parameter logistic function21 and LOD was evaluated by the 3σ criterion. As a result, we obtained an LOD of 0.62 nM by protocol 1. This is comparable with typical LOD of DNA by existing microchips for solid-phase hybridization assays.22–24 On the other hand, LOD of 5.3 nM was obtained by protocol 2. The lower LOD by protocol 1 can be explained by the effect of coaxial stacking-aided hybridization13–16 which is known to support oligonucleotides hybridization. It means, if we assume that this is effective also in miRNA–DNA hybridization, the affinity of ProFlu21–miR-21 hybrids to Pro21 should be higher than that of miR-21 alone to Pro21. The hybridization efficiency by protocol 1 was almost the same as that of non-sandwich hybridization between full-matched probe DNA (Pro21full) and fluorescent labelled miR-21 (MiR-21Flu) under the same condition (Fig. 2(c) Full match). This indicates that the effect of coaxial stacking allows sandwich hybridization efficiency approximately the same as non-sandwich hybridization even in short RNAs. Hybridization efficiency between half-matched probe DNA (Pro21) and MiR-21Flu showed hybridization efficiency as low as sandwich hybridization by protocol 2 (Fig. 2(c) Half match). This suggests that the efficiency of hybridization between Pro21 and MiR-21 is the limiting factor in protocol 2.
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Fig. 2 (a) Bright field microscopic view (top) and fluorescent microscopic view (bottom) of microchannels by protocol 1. Red dotted lines indicate the area where probe DNA is immobilized on the glass surface. Blue dotted lines indicate the microchannels. Target miRNA was injected into the left channel and random miRNA was injected into the right channel. (b) Fluorescence intensity vs. miRNA concentration by the two protocols, protocol 1 and protocol 2. (c) Fluorescence intensity vs. fluorescent labeled miRNA concentration by probe DNA with different length. |
The coaxial stacking effect can also be supported by the melting temperature (Tm) calculation. The Tm values were calculated using on-site software HyTher (see ESI†). The Tm values between miR-21 and individual probes, ProFlu21 and Pro21, were 37.6 °C and 42.0 °C, respectively. On the other hand, with both of the probes, the sandwich construct including a coaxial stacking site raised the Tm value to 73.4 °C which was as high as that of intact RNA–DNA duplex with 22 bps. Those theoretical results are consistent with the experimental results that the fluorescent signals of the sandwich structure without any gap (Fig. 2(b) Protocol 1) and RNA–DNA hybrids of 22 bps (Fig. 3(c) Full match) were almost at the same level.
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Fig. 3 Multiple sequence detection from a single sample solution. The blue lines indicate the microchannels and the red lines indicate the probe DNA patterned area. Fluorescence intensities appeared only on the corresponding probe DNAs in all four cases. |
To further confirm this effect, both protocol 1 and protocol 2 were carried out by an artificial variant of miR-21 with additional U base at the centre of the sequence (MiR-21Gap), which induces a single base gap between the two probe DNAs, while retaining the affinity to the individual probes (Fig. S1†). The results show, in both protocols, approximately the same affinity when non-labelled miR-21 was detected by protocol 2 (Fig. S2†). This can be attributed to the gap between the two probe DNAs, which eliminate the coaxial stacking effect. These results clearly indicate that the coaxial stacking effect was the major cause of the higher sensitivity with protocol 1 than that with protocol 2. Therefore, protocol 1 with probe DNA construction without any gap between two probe DNAs is the ideal design of miRNA detection by sandwich hybridization.
The experiments of multiple sequence detection from a single sample solution resulted in fluorescence intensities only on the probe DNA of corresponding sequences in all four cases (Fig. 3). This capability of multiple sequence detection strongly supports the fact that miRNA detection by this device is a promising technology in cancer diagnosis because each cancer has only a few corresponding marker miRNA which may exclude the need of screening hundreds of sequences by conventional array chip.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c2an16154k |
‡ Present address: JST-ERATO Higashiyama Live-Holonics Project and Graduate School of Science, Nagoya University, Japan. |
This journal is © The Royal Society of Chemistry 2012 |