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Applied and Environmental Microbiology, December 2008, p. 7297-7305, Vol. 74, No. 23
0099-2240/08/$08.00+0 doi:10.1128/AEM.01002-08
Copyright © 2008, American Society for Microbiology. All Rights Reserved.
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Department of Civil and Environmental Engineering, University of Michigan, Ann Arbor, Michigan 48109,1 Department of Civil and Environmental Engineering,2 Department of Animal Sciences, University of Illinois at Urbana-Champaign, Urbana, Illinois 618013
Received 4 May 2008/ Accepted 16 September 2008
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The peptide nucleic acid (PNA) oligomer probe was studied for its hybridization properties for the first time about 15 years ago (15). PNA differs from DNA in that it contains an electro-neutral polypeptide backbone while DNA includes a negatively charged sugar-phosphate backbone (31). The neutral backbone results in hybridization characteristics unique to PNA probes. For example, compared with traditional DNA probes, PNA probes bind more strongly to target nucleic acids (15) and are less dependent on the salt concentration used when hybridized to target DNA oligonucleotides (24). Furthermore, their hybridization kinetics are less affected by the secondary structure of target nucleic acids (3). These characteristics have allowed successful applications of PNA probes in various fields of microbiology (7, 11, 32, 54).
Apart from PNA-conferred improvements in probe composition, novel probe chemistries have also been devised for both DNA-and PNA-based probes. These include molecular beacons (MBs) (50, 55), adjacent fluorescence resonance energy transfer probes (9, 49), light-up probes (38, 46), and quenched autoligation probes (40, 41). The first DNA MB probes were developed by Tyagi and Kramer (50). A DNA MB contains a probe sequence complementary to the target region of nucleic acids and a stem structure consisting of a few nucleotides complementary to each other, allowing the DNA MB to form a stem-loop structure. A fluorophore is attached to one end of the DNA MB, while a quencher is bound to the other end. When no target nucleic acid is present, DNA MBs remain in their stem-loop configuration and the proximity of the quencher to the fluorophore results in limited or no fluorescence. When DNA MB probes bind to target nucleic acids, the stem-loop structure opens, resulting in an increase in the distance between the fluorophore and the quencher, and fluorescence can be detected. Thus, DNA MB probes fluoresce only upon hybridization to target nucleic acids, allowing for a solution-based hybridization format (50). Hybridizations with DNA MBs exhibit several other advantages, such as a low background signal (28), high specificity (5), and high sensitivity (51). Because of these characteristics, DNA MB probes have been shown to be advantageous in applications in real-time PCR (35, 51), visualization of mRNA in living cells (6), and detection of nucleic acids in array techniques (4, 57) but have been less successful in quantifying rRNA in solution-based hybridizations (55).
PNA MB probes were developed to make use of the advantages of both PNA probes and the structure of MBs (33, 42). Different from DNA MBs, which contain a stem-loop structure, PNA MBs consist of only a loop structure. The stemless loop structure of PNA MBs simplifies probe design. PNA MBs are hydrophobic and therefore tend to fold to minimize the surface area in aqueous solution (42). In addition, the electrostatic interaction between two oppositely charged amino acids at each end may help bring the fluorophore and quencher into close proximity. So far, most of the studies of PNA MBs have focused on the hybridization of PNA MBs to DNA oligonucleotides (24, 26) or PCR products (35), except for a few studies in which 16S rRNA was used as targets in PNA MB hybridization (13, 55, 56). Even though PNA MBs are considerably more expensive than DNA MBs and are available from only one authorized vendor (Panagene, Daejeon, Korea), the use of PNA MBs in solution-based rRNA-targeted hybridizations showed much promise in a previous study (55). However, more work to evaluate reaction kinetics and hybridization specificity is needed before this technique can be used as a quantitative tool for environmental samples.
The present study addresses how probe sequence and hybridization conditions affect the kinetics of hybridization of PNA MBs to 16S rRNA and how well PNA MBs can differentiate target and nontarget rRNA, which affirms the potential of PNA MB hybridization as a quantitative assay in environmental studies.
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TABLE 1. Specificity, coverage, and sequences of PNA MBs Dmonas0121 and Dsoma0848a
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TABLE 2. Target sites in 16S rRNA of target and nontarget species included in this study for PNA MBs Dmonas0121 and Dsoma0848
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Total RNA was extracted from centrifuged cell pellets using a phenol-chloroform-isoamyl alcohol extraction procedure (44), and the RNA was resuspended in distilled deionized water and stored at –80°C. The concentrations of nucleic acids in the RNA extracts were measured spectrophotometrically using a NanoDrop ND1000 (NanoDrop Technologies, Wilmington, DE) at a wavelength of 260 nm. Furthermore, the quality of the RNA extracts was evaluated using polyacrylamide gel electrophoresis (Jule Biotechnologies Inc., Milford, CT), and images of the gels were analyzed using Kodak (Rochester, NY) molecular imaging software (version 4.0.3K1). The concentration of 16S rRNA in each extract was calculated as the product of the total nucleic acid concentration estimated spectrophotometrically and the mass ratio of 16S rRNA to total nucleic acid obtained from the gel image analysis.
Hybridizations.
The hybridization buffer composition and hybridization condition for PNA MB Bact0338 were adopted from the study by Xi et al. (55). The hybridization buffer used for PNA MBs Dmonas0121 and Dsoma0848 was modified from the same study and contained 25 mM Tris-HCl and 10 mM NaCl, except for specific experiments as described below. In the experiments testing various salt concentrations, hybridization buffers contained NaCl with final concentrations ranging from 0 to 500 mM. In the experiments using formamide for stringency control, hybridization buffers contained formamide ranging from 0 to 90% (vol/vol). In the experiments for which environmental samples were used, hybridization conditions were adopted from characterization experiments in this study or the study by Xi et al. (55). Detailed hybridization conditions for all experiments are summarized in Table 3.
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TABLE 3. Hybridization conditions for various experimentsa
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Data analysis.
Net RFUs for hybridization of PNA to 16S rRNA were calculated as the differences between RFUs obtained with samples containing only PNA MB and RFUs from samples also containing 16S rRNA.
A pseudo-first-order model was used to fit the kinetic curves (36) for the formation of hybrids between PNA MB probes (P) and target 16S rRNA (R):
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are the hybrid concentrations at time t and at time infinity, respectively. The value of [PR]t was measured in RFU. The values of [PR]
and ku were simulated using the curve-fitting function in the software program KaleidaGraph (Synergy Software, Reading, PA). The two parameters, [PR]
and ku, provided information on the final hybridization signal and the apparent rate constant, respectively. The values of the apparent rate constants were subject to statistical analyses in Microsoft Excel using two-way analyses of variance with the sequence as one independent variable and the NaCl concentration as the other independent variable. In this study, the units for the pseudo-first-order apparent rate constant are RFU·min–1·M–1. If RFU are converted to molarity, the units simplify to min–1.
Detection limit.
The detection limit of the PNA MB hybridization assay was determined using a standard procedure (17) with seven replicates for each 16S rRNA concentration included in the experiment (Table 3). In brief, measurement results from seven replicates were calculated for standard deviation (s), a critical t value was obtained using a degree of freedom of 6 and a confidence level of 99% (t6, 0.99), and a method detection limit (MDL) was calculated as
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FIG. 1. Nonspecific opening of PNA MB Dsoma0848 due to the increases in the hybridization temperature and formamide concentration in hybridization buffers. No rRNA was present in this experiment.
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Hybridization kinetics. (i) Kinetics of hybridization to target and nontarget 16S rRNA.
Prior to the determination of optimal hybridization conditions, the kinetic properties of hybridizations of PNA MB were studied with various 16S rRNA sequences and in hybridization buffers of various NaCl concentrations. Five hundred fmol (1 fmol equals 10–15 mol) of one target 16S rRNA (D. suillum) and two nontarget 16S rRNAs (M. minutulum and M. methylotrophus) were used in each hybridization reaction with 10,000 fmol of PNA MB Dsoma0848 (Table 3). This 20-fold excess of PNA MB to target and nontarget 16S rRNA resulted in hybridization reactions that exhibited pseudo-first-order kinetics, as indicated in Fig. 2 with good agreement between the simulation curves and the experimental data points. Hybridization of PNA MB Dsoma0848 to its target 16S rRNA (D. suillum) resulted in the highest final net fluorescence signals among the three hybridizations. Unexpectedly, the final signal of the hybridization to the 16S rRNA with four mismatches (M. methylotrophus) was higher than that from the hybridization to the 16S rRNA with one mismatch (M. minutulum). This phenomenon was also observed for some hybridization conditions in other kinetic experiments (Fig. 3a). In addition, the hybridization of PNA MB Dsoma0848 to nontarget 16S rRNAs exhibited faster kinetics and reached equilibrium faster than the hybridization to target 16S rRNA (Fig. 2).
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FIG. 2. A sample plot showing the kinetics of the hybridizations of PNA MB Dsoma0848 to target and nontarget 16S rRNA in the presence of 10 mM NaCl. The points are experimental data points, and the lines are curve fit based on a pseudo-first-order reaction model simulated in KaleidaGraph. The numbers in parentheses indicate the numbers of mismatches between 16S rRNA and PNA MB. The r2 values of the three curves in this figure ranged from 0.986 to 0.993.
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FIG. 3. The effects of NaCl concentrations in hybridization buffers on final net fluorescence signals (a) and apparent rate constants (b) from hybridizations of PNA MB Dsoma0848 to target and nontarget 16S rRNA. Mean values of duplicates are reported, and the error bars represent the range of the duplicates. The numbers in parentheses indicate the numbers of mismatches between 16S rRNA and PNA MB.
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The apparent rate constants also decreased as the NaCl concentration increased (Fig. 3b). In addition, the apparent rate constants for the target were lower than those of the nontargets at all the NaCl concentrations tested, although this difference was not statistically significant. In the two-way analysis-of-variance tests, the NaCl concentration—an independent variable—appeared to have a significant effect on the apparent rate constants (P < 0.05). In contrast, sequence—the other independent variable—did not have a significant effect on the apparent rate constant (P = 0.24). The interaction between the two independent variables was not significant, either (P = 0.99). The slower overall kinetics of the hybridization with target rRNA did not allow elimination of signal from nontargets using a kinetic approach.
Optimization of hybridization conditions. (i) Stringency control using hybridization temperature.
Melting curves of the hybridizations of PNA MB Dsoma0848 with 16S rRNAs showed that at the lowest hybridization temperature of 22°C, target 16S rRNA (D. suillum) exhibited a higher net fluorescence signal than nontarget 16S rRNAs with one and four mismatches (M. minutulum and M. methylotrophus, respectively) (Fig. 4). Consistent with the order of final hybridization signals presented in the kinetic experiments (Fig. 2 and 3a), the net fluorescence signal from M. methylotrophus (four mismatches) was higher than that from M. minutulum (one mismatch) at 22°C and subsequent temperatures evaluated. As the temperature was increased, the net fluorescence signals of all three melting curves increased slightly and then decreased. Between 64 and 70°C, the three melting curves reached their minimum values. At about 68°C, the net fluorescence signal from M. minutulum was zero and the signal from M. methylotrophus was low. Hence, 68°C was selected as the optimal hybridization temperature for PNA MB Dsoma0848.
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FIG. 4. Melting profiles of the hybridizations of PNA MB Dsoma0848 with its target and nontarget 16S rRNAs. The numbers in parentheses indicate the numbers of mismatches between 16S rRNA and PNA MB. The experiment was repeated, and similar profiles were obtained (data are shown in Fig. S1 in the supplemental material).
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To confirm the optimal hybridization temperature and demonstrate that elimination of signals from nontarget rRNA can be achieved in mixed cultures at optimized hybridization conditions, an artificial mixture containing equal amounts of 16S rRNA from target and nontarget with one mismatch (D. suillum and M. minutulum, respectively) was hybridized with PNA MB Dsoma0848 (Fig. 5). At the optimized hybridization temperature of 68°C, the net fluorescence signal from nontarget 16S rRNA with one mismatch was zero. The net fluorescence signals from the target and the artificial mixture were nearly identical, confirming that the nontarget 16S rRNA did not contribute to the signal. Thus, after optimization of hybridization conditions, PNA MBs can be used to quantify target 16S rRNA in samples containing mixtures of rRNA, such as environmental samples. In addition, the fluorescence signal at 68°C in the melting-curve experiment started at 22°C (Fig. 4) was similar to the fluorescence signal at 68°C in the melting curve experiment started at 60°C (Fig. 5), which verified that the 2-min time period was sufficient for the hybridization to reach equilibrium after each increase in temperature (Table 3).
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FIG. 5. Melting profiles of the hybridizations of PNA MB Dsoma0848 with 16S rRNAs of its target, nontarget, and an artificial mixture of the target and nontarget species. The numbers in parentheses indicate the numbers of mismatches between 16S rRNA and PNA MB. The experiment was repeated, and similar profiles were obtained (data are shown in Fig. S2 in the supplemental material).
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FIG. 6. Melting profiles of the hybridizations of PNA MB Dmonas0121 with its target and nontarget 16S rRNAs. The numbers in parentheses indicate the numbers of mismatches between 16S rRNA and PNA MB.
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FIG. 7. Effect of formamide concentration at 25°C on the net fluorescence signals from the hybridizations of PNA MB Dmonas0121 with its target and nontarget 16S rRNAs. Mean values of duplicates are reported, and the error bars represent the range for the duplicates. The numbers in parentheses represent the numbers of mismatches between 16S rRNA and PNA MB.
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Spike-in experiment.
The hybridization assay using PNA MB Dsoma0848 allowed quantification of target 16S rRNA (D. suillum spiked at different concentrations to RNA extracted from an environmental sample. The hybridization response of PNA MB Dsoma0848 was linear over the range of 0 to 30% of relative abundance for the 16S rRNA spiked to the RNA extract from an environmental sample and for the corresponding target 16S rRNA alone (i.e., 0 to 43 fmol of target 16S rRNA; Fig. 8). However, the environmental RNA extract spiked with the different concentrations of target 16S rRNA resulted in higher hybridization responses.
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FIG. 8. Net fluorescence signals from the hybridizations of PNA MB Dsoma0848 with a series consisting of various amounts of target 16S rRNA (D. suillum) spiked to RNA extracted from an environmental sample and with a series of samples containing only target 16S rRNA corresponding to the amounts of 16S rRNA target in the first series. The error bars represent standard deviations for five replicates.
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The kinetics of hybridization reactions depend on both forward and reverse reactions (i.e., association and dissociation processes). Solid surface hybridizations with linear DNA and PNA probes have been used to study association and dissociation rates. For example, using immobilized linear DNA oligonucleotide probes, Livshits and Mirzabekov demonstrated that the association rate constant was the same for target and nontarget DNA (27), and Dai et al. showed that nontargets exhibited higher dissociation rate constants than targets, which resulted in faster overall kinetics for nontarget (14). In contrast, immobilized linear PNA probes generally exhibited higher association rate constants and lower dissociation rate constants for targets than for nontargets (21). Unlike solid surface hybridizations, the solution-based hybridizations in this study do not allow separate analyses of association and dissociation processes. Based on conclusions presented by Jensen and coworkers (21), we suggest that the lower apparent rate constants in the hybridizations with target 16S rRNA (Fig. 2 and 3b) were the result of lower dissociation rate constants for target 16S rRNA.
The lower apparent rate constants for the hybridization of PNA MB with target 16S rRNAs demonstrated it was not feasible to use a kinetic approach to eliminate false-positive fluorescence signals due to nonspecific hybridization. Therefore, other approaches, such as optimizing the hybridization temperature and formamide concentration in the hybridization buffer, were used to control hybridization specificity for the PNA MBs Dmonas0121 and Dsoma0848. Before these approaches were tested, the salt concentration in the hybridization buffer was optimized.
Because 16S rRNAs were used as target molecules, the NaCl concentration in the hybridization buffer affected not only the hybridization between PNA MB Dsoma0848 and target molecules but also the secondary structures of the rRNA molecules. High salt concentrations (i.e., high ionic strength) in hybridization buffers favor the formation of RNA secondary structure and make the target sites in rRNA less accessible (48). A study of hybridizations between linear PNA probes and double-stranded-DNA oligonucleotide targets revealed that the initial association rates dropped as the NaCl concentrations increased from 20 to 50 mM (25). Unlike double-stranded-DNA oligonucleotides, 16S rRNAs exhibit a higher-order structure; thus, it was important to compare hybridization results for different NaCl concentrations.
It should be noted that the hybridization condition used in the kinetic experiments did not correspond to the optimized hybridization condition. As indicated above, the objectives of these experiments were to compare the kinetics of hybridizations of PNA MB to target and to nontarget 16S rRNAs, evaluate the effects of NaCl concentrations on PNA MB hybridization kinetics, and choose a NaCl concentration for experiments thereafter. Previous studies have evaluated the kinetics of hybridizations of PNA MB and DNA MB to target and nontarget DNA oligonucleotides (24) and target 16S rRNA (55). To our knowledge, this is the first study evaluating the effects of rRNA sequence and hybridization buffers on the kinetics of hybridizations of PNA MB to 16S rRNA.
The hybridization optimization experiments, with various hybridization temperatures and formamide concentrations in hybridization buffers, indicated the two PNA MB probes designed in this study required different optimization strategies (Fig. 4 to 7). A third PNA MB, Bact0338, previously designed and characterized by Xi and coworkers (55), was also included in our study. Xi et al. (55) defined the optimal formamide concentration as the condition that maximized the difference between the fluorescence signal of a hybridization reaction and the fluorescence signal of the control reaction containing only PNA MB. They demonstrated that hybridization under the optimized condition allowed differentiation of target and nontarget 16S rRNAs when their abundances were comparable. However, unpublished data from our study showed that the optimal hybridization condition as defined by Xi et al. (55) resulted in significant false-positive signals when the relative abundance of target 16S rRNA was low in an artificial mixture. Therefore, in the current study, melting-curve experiments were conducted for the PNA MB probe Bact0338 with target and nontarget 16S rRNAs to determine a condition that minimized the signal from nontargets. Unexpectedly, PNA MB Bact0338 exhibited melting profiles completely different from those shown in Fig. 4 and 6: the net fluorescence signals from both target and nontarget 16S rRNAs increased with hybridization temperatures (data not shown). Thus, we conclude that each newly designed PNA MB needs to be carefully characterized and may require different stringency control strategies.
The difference between the two series in Fig. 8 may be attributed to the presence of target 16S rRNA in the environmental sample. The environmental sample was collected from an anaerobic bioreactor, and the genus Dechlorosoma contains heterotrophic facultative anaerobic respiring bacteria (1). Alternatively, the difference may be the result of nonspecific hybridization and/or nonspecific opening of PNA MB due to binding to environmental substances in the samples. This possible nonspecific hybridization signal corresponded to about 5% of the total signal. In this experiment, we decided to spike RNA extracted from a pure culture of a target strain into RNA extracted from an environmental sample, rather than spiking target cells into an environmental sample followed by RNA extraction. The latter approach may overestimate the sensitivity of the method, because target cells grown in rich medium likely have higher levels of 16S rRNA than cells in environmental samples (22).
The relative abundance values of Dechlorosoma spp. determined using the 16S rRNA-targeted PNA MB hybridization assay and with the 16S rRNA gene-targeted clone library method were different. Both methods provided results that could be qualitatively linked to the performance of the bioreactor: the increase of Dechlorosoma spp. with time was consistent with improved perchlorate removal in the bioreactor (data not shown). Although the results obtained with the two methods differed substantially, such differences are not unusual, especially when methods subject to PCR biases are involved (2). It should also be noted that the target biomarkers for the two methods were different: the solution-based hybridization assay targets 16S rRNA, whereas the clone library method targets 16S rRNA genes. Others have shown substantial differences when such quantitative results were compared (8, 19).
We observed that PNA MB in the absence of rRNA produced substantial fluorescence signals at high temperatures or high formamide concentrations (Fig. 1). Bonnet et al. proposed a three-conformation model for DNA MB probes (5). The authors demonstrated that there were three conformations of structured DNA MB: DNA MBs hybridized to RNA molecules, free DNA MBs that do not contribute to fluorescence signals, and randomly coiled free DNA MBs that fluoresce. According to Bonnet et al., the third conformation usually occurs at high temperatures when hybrids between probe and target nucleic acid have melted and the stem structure of DNA MB is broken. In the current study, although the structure of PNA MBs is different from that of DNA MBs, it is reasonable to speculate that the majority of PNA MBs are present in a randomly coiled free form at high temperatures. The observed increases in net fluorescence signals in the presence of target and nontarget rRNAs (Fig. 4 and 5) suggest that rRNA molecules, independently of sequence, facilitate the formation of the coil-free PNA MB.
The negative values in net fluorescence signals (Fig. 4 to 7) may result from a quenching effect of nucleic acids on fluorophores. A study by Wang et al. suggested a quenching effect on TAMRA, the same dye used in the PNA MBs Dmonas0121 and Dsoma0848, when the dye is in proximity of a guanosine near the target site (53). In the current study, the fluorescence signals were reported as net fluorescence signals, the difference between the signals from controls containing only PNA MB and the signals from corresponding samples also containing rRNA molecules. Because the quenching effect is absent in the controls, the subtraction caused negative signals in the net fluorescence signals. It was noticed that the negative net fluorescence signals were more evident in the formamide experiment (Fig. 7) than in the melting-curve experiments (Fig. 4 to 6). This might be related to the fact that formamide is more efficient in causing nonspecific opening of PNA MB than temperature in controls (Fig. 1). Future studies should focus on designing new PNA MBs that maintain their loop structure even at stringent conditions when target rRNA is not present.
We appreciate helpful discussions with Chuanwu Xi and critical reviews of the manuscript by Diane Holder and three anonymous reviewers. We also thank Peter Adriaens and Jeremy Semrau for access to equipment.
Published ahead of print on 26 September 2008. ![]()
Supplemental material for this article may be found at http://aem.asm.org/. ![]()
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