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Applied and Environmental Microbiology, May 2007, p. 3189-3195, Vol. 73, No. 10
0099-2240/07/$08.00+0 doi:10.1128/AEM.02609-06
Copyright © 2007, American Society for Microbiology. All Rights Reserved.
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Department of Crop and Soil Sciences, Cornell University, Ithaca, New York 14853
Received 8 November 2006/ Accepted 12 March 2007
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While nucleic acid SIP provides a powerful tool for characterizing microbial activity under in situ conditions, the method has notable limitations (5, 19, 22, 25, 26, 35, 36). One consideration that can complicate the interpretation of DNA-SIP experiments is the effect that genome G+C content has on the buoyant density of DNA (39). This relationship between DNA G+C content and buoyant density in CsCl gradients is described by the equation
= (0.098[G+C]) + 1.66, where
represents density in g ml1 and [G+C] is the mole fraction G+C content (1). Thus, the native buoyant density of DNA in a CsCl gradient can differ by as much as 0.05 g ml1 over the range of genome G+C contents that can occur in complex communities. This natural variation in DNA density explains why DNA from complex communities can occur as a "smear" extending over a range of densities in a CsCl gradient (35). Since fully 13C-labeled DNA increases in buoyant density by 0.036 g ml1 relative to unlabeled DNA (1), there arises the very real possibility that "heavy" fractions will contain isotopically labeled DNA, as well as unlabeled DNA, from organisms with a high genome G+C content (19, 25, 36). This problem can be compounded if the incubation conditions used for DNA-SIP experiments result in the unintended growth of high-G+C organisms as a result of changes in soil moisture, temperature, bottle effects, or other artifacts associated with substrate amendment.
While the G+C problem is a potential concern in any DNA-SIP experiment, it represents a fundamental obstacle to the successful application of DNA-SIP with 15N as an isotopic label. The change in DNA buoyant density for fully 15N-labeled DNA (0.016 g ml1 [1]) is less than half of the change in density that occurs naturally as a result of natural variation in the genome G+C content. Thus, there is a considerable potential for 15N-labeled DNA to cooccur with unlabeled DNA. This problem has been emphasized in recent attempts to use 15N-labeled compounds in DNA-SIP that have found significant overlap in the buoyant densities of 15N-labeled and unlabeled DNA in CsCl gradients (2, 3), but the extent to which variation in the genome G+C content poses a problem in complex communities has not been systematically examined.
To illustrate the nature of this problem, calculations were performed to examine the theoretical effects of genome G+C content and isotope incorporation on DNA density in a CsCl gradient (Fig. 1). The buoyant density of unlabeled DNA with a G+C content between 30% and 80% was calculated to range from 1.689 to 1.738 g ml1, respectively (Fig. 1). It was calculated that 100% 13C-labeled DNA which has less than 40% G+C content will have the same buoyant density as unlabeled DNA which has more than 65% G+C content (Fig. 1). As expected, considerably more overlap between unlabeled and labeled DNA was calculated to occur for 100% 15N-labeled DNA and for DNA that is only partially labeled (Fig. 1). For example, Fig. 1 predicts that 100% 15N-labeled DNA from an organism with a 51% genome G+C content, such as Escherichia coli, will have the same buoyant density as unlabeled DNA from an organism with a 67% genome G+C content, such as Pseudomonas aeruginosa.
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FIG. 1. Expected relationship between genome G+C content and buoyant density in a CsCl gradient represented for unlabeled DNA and DNA that is partially or completely labeled with either 13C or 15N. The shaded region of the chart represents the range of densities over which unlabeled DNA would be expected to occur based on biologically meaningful values of genome G+C content (30% to 80% G+C content).
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1)]/(v4 x r2 x S), where
is particle density in g ml1, ß° is the density gradient proportionality constant (1.14 x 109 for 1.7 g ml1 CsCl at 20°C), v is rotor velocity in rpm, r is the expected radius that the particle will occupy at equilibrium, and S is the sedimentation coefficient of the particle (1). It is apparent that the time required for a particle to reach equilibrium can be reduced greatly by increasing the rotor velocity. However, higher rotor speeds result in steeper density gradients, which are not optimal for separating particles having small differences in density. Thus, it is important to consider the effect of the DNA molecular weight on the time required to reach equilibrium. We used the above expression to calculate the impact that the DNA molecular weight has on the time required for a particle of 1.71 g ml1 to reach equilibrium in a CsCl density gradient formed at 55,000 rpm (164,000 x g maximum) in a TLA110 rotor (see Fig. S1 in the supplemental material). The sedimentation coefficient of DNA was estimated as 2.8 + (0.00834 x M0.479), where M is the molecular weight of a linear DNA fragment (43). Based on the results of these calculations, we chose to use DNA of no less than 4,000 bp for all CsCl gradient experiments.
CsCl gradient formation.
High-molecular-weight genomic DNA for use in CsCl gradients was extracted from E. coli (ATCC 9637) and P. aeruginosa (ATCC 10145) by spooling as described previously (40). 15N labeling of E. coli DNA was accomplished by growth in minimal M9 medium (40) to which either NH4Cl or 98 atom% 15NH4Cl (Aldrich) was added in defined proportions to obtain different amounts of 15N label incorporation into DNA. Cultures were transferred twice in medium containing the desired proportion of 15NH4Cl, and the inocula were kept small (1/100 volume) to minimize 14N carryover from starter cultures.
Primary CsCl gradients were formed by filling 4.7-ml polyallomer Optiseal tubes (Beckman) with 4.3 ml of 1.762-g ml1 CsCl in gradient buffer (15 mM Tris-HCl, 15 mM KCl, 15 mM EDTA, pH 8.0) and 0.45 ml of DNA in TE buffer (50 mM Tris-HCl, 15 mM EDTA, pH 8.0). CsCl concentrations were determined by using a Reichert AR200 handheld digital refractometer. The CsCl concentration was calculated from the refractive index using the equation
= anc b, as described previously (1), where
is the density in g ml1, nc is the corrected refractive index, and a and b are coefficients of values 10.927 and 13.593, respectively, for CsCl at 20°C. The corrected refractive index of CsCl in gradient buffer was calculated as nc = nobserved (nbuffer nwater), where nbuffer is the refractive index of the gradient buffer and nwater is that of water. Unless explicitly stated, CsCl gradients were loaded with 10 µg of DNA. Tubes were balanced and then sealed and mixed to obtain a homogeneous CsCl density of 1.69 g ml1. Centrifugation was carried out for 66 h at 55,000 rpm (164,000 x g maximum) and 20°C in an Optima Max-E tabletop ultracentrifuge (Beckman-Coulter) equipped with a TLA110 rotor.
Secondary CsCl gradients were used to disentangle the effects of isotope incorporation from genome G+C content. These secondary CsCl gradients were prepared as described above with the exception that 8 µl of 10-mg/ml bis-benzimide (Hoechst no. 33258; Sigma-Aldrich) was added to the DNA sample.
Gradient fractionation.
Immediately following centrifugation, a fraction recovery system (Beckman) was used to collect 45 fractions of 100 µl from each CsCl gradient. The fraction collection method has been described previously (25, 26) with the exception that in the current experiment, 4.7-ml centrifuge tubes and 100-µl fractions were used to enhance the resolution of gradient fractionation. Fractions were displaced by using a syringe pump (KD Scientific) to dispense mineral oil into the tops of sealed tubes at a rate of 200 µl min1. Fractions were collected through a side port needle inserted through the bottom of the tube. The density of each fraction was determined immediately by measurement of the refractive index using an AR200 digital refractometer (Reichert) which was modified to allow measurement from 5-µl volumes by covering the prism surface with a mask fashioned from black electrical tape with a 1.5-mm-diameter hole. CsCl was removed from DNA by ethanol precipitation and resuspended in 25 µl of 50 mM Tris-HCl, pH 8.0, and stored at 20°C.
Quantification of DNA in gradient fractions.
The distribution of DNA in primary CsCl gradients was determined by using the Quant-iT PICO Green dsDNA assay (Invitrogen) as per the manufacturer's instructions. A total of 5 µl of purified DNA from each fraction was used in each assay, and the assays were carried out in optically clear 96-well plates (Costar); fluorescent intensity was quantified by using a Fluor-S Multimager (Bio-Rad). Secondary CsCl gradients generally contained less DNA than primary gradients, and so quantitative PCR was used to determine the number of 16S rRNA genes in each fraction of these gradients. Quantitative PCR was conducted with primers Bact519F (5'-CAG CMG CCG CGG TAA NWC-3') and Bact907R (5'-CCG TCA ATT CMT TTR AGT T-3'), which target bacterial 16S rRNA genes (41). Reactions were carried out in 50-µl volumes containing 1 µl of template DNA with each primer at a concentration of 0.3 µM, each deoxynucleoside triphosphate at a concentration of 50 µM, and 1x iTaq SYBR Green Supermix with ROX (Bio-Rad). Each PCR consisted of a 50°C hold for 2 min and a 95°C hold for 10 min, followed by 40 cycles of 15 s at 95°C and 60 s at 60°C. Reactions were carried out in an Applied Biosystems 7900 HT sequence detection system (ABI). E. coli 16S rRNA gene sequences were amplified by PCR and gel purified for use as a standard to relate threshold cycle values to the number of 16S rRNA genes present in each reaction.
Analysis of soil community DNA.
A soil sample was collected from a plot on Caldwell Field (Ithaca, NY) that has been maintained as a fallow for more than 30 years. DNA was extracted from four samples of 0.25 g soil using the UltraClean soil DNA extraction kit (MoBio, Inc.) as per the manufacturer's instructions, and these DNA extracts were subsequently pooled. DNA was further purified by electrophoresis through a 1% low-melting-temperature agarose gel to remove DNA fragments smaller than 4 kbp. DNA of greater than 4 kbp was excised from the gel, agarose removed by digestion with agarase (New England Biolabs) as per the manufacturer's instructions, and DNA obtained by ethanol precipitation. Analysis of a subsample of the DNA extract by Pico Green assay (Invitrogen) revealed total recovery of 1.8 µg of DNA per g of soil. This DNA sample was equilibrated in a primary CsCl gradient as described above, and the gradient was fractionated and gradient fractions analyzed by 16S rRNA gene terminal restriction fragment length polymorphism (T-RFLP) analysis.
T-RFLP analysis of 16S rRNA genes was carried out using the PCR primers Bact8F (5'-AGA GTT TGA TCM TGG CTC AG-3'), labeled at the 5' end with the dye 6-carboxy-fluorescein, and the primer Univ1390R (5'-GAC GGG CGG TGT GTA CAA-3') (15). Reactions were carried out in 100-µl volumes containing 2 µl of template DNA with the 6-carboxy-fluorescein-labeled primer at a concentration of 0.5 µM and unlabeled primer at 0.3 µM, each deoxynucleoside triphosphate at a concentration of 50 µM, 2.5 mM MgCl2, 5 U of AmpliTaq Gold DNA polymerase (Applied Biosystems, Foster City, CA), and 1x PCR buffer (supplied with the Taq enzyme). Each PCR consisted of a 95°C hold for 5 min followed by 35 cycles of 45 s at 95°C, 30 s at 55°C, and 30 s at 72°C. Following amplification, PCR products were desalted using Micro Bio-Spin P-30 Tris chromatography columns (Bio-Rad) and concentrated using an evaporative centrifuge (Eppendorf). PCR products were resuspended in 50 mM Tris-HCl, pH 8.0, and 250 to 400 ng of this DNA was digested with MspI (New England Biolabs) in 30-µl reaction volumes as per the manufacturer's instructions; the enzyme was subsequently inactivated by incubation at 65°C for 20 min. The digested PCR products were desalted and concentrated again and then resuspended in formamide loading buffer and resolved on an Applied Biosystems Automated 3730 DNA analyzer.
T-RFLP data were used to determine the density profiles of individual terminal restriction fragments (TRFs) in primary CsCl gradients. In addition, to determine whether genome G+C content influences the distribution of community DNA in CsCl gradients, overall similarity in T-RFLP patterns was determined with respect to gradient density. Similarity in T-RFLP profiles was determined by using the Sorenson index of similarity: S = (2 x ab)/(a + b), where a and b are the numbers of TRFs in any two samples and ab is the number of TRFs shared between those samples (23).
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FIG. 2. Effect of 15N enrichment and genome G+C content on DNA distribution in CsCl density gradients. Lines indicate the density of unlabeled E. coli DNA ( ), 100% 15N-labeled E. coli DNA (), or unlabeled P. aeruginosa DNA ( ). The genome G+C contents of E. coli and P. aeruginosa are approximately 51% and 67%, respectively.
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FIG. 3. Fluorescence intensities of TRFs from soil DNA equilibrated in a CsCl density gradient and subjected to T-RFLP of 16S rRNA genes in gradient fractions. TRFs were selected to demonstrate that the buoyant densities of individual TRFs can vary between 1.69 g ml1 and 1.73 g ml1 in density gradients. Fluorescence intensity is shown as a ratio of the maximum value of fluorescence intensity that was observed for each TRF. The TRFs shown for panels A through I are 102 bp, 242 bp, 512 bp, 500 bp, 372 bp, 288 bp, 144 bp, 121 bp, and 177 bp, respectively.
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FIG. 4. Ability of bis-benzimide to disentangle effects of stable isotope incorporation and genome G+C content on DNA density in CsCl gradients. (A) In the absence of bis-benzimide, it is impossible to resolve 100% 15N-labeled E. coli DNA from unlabeled P. aeruginosa DNA in a mixture of unlabeled E. coli DNA, 100% 15N-labeled E. coli DNA, and unlabeled P. aeruginosa DNA ( ). (B) In the presence of bis-benzimide, it is possible to resolve 100% 15N-labeled E. coli DNA from unlabeled P. aeruginosa DNA in a mixture of the two (). The density distribution of a pure sample of unlabeled P. aeruginosa DNA from a second gradient is depicted for reference ( ).
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FIG. 5. Secondary CsCl gradients containing bis-benzimide allow detection of small amounts of 15N-labeled DNA in the presence of excess unlabeled DNA. In separate experiments, either 2 µg ( ) or 200 ng ( ) of 15N-labeled E. coli DNA was mixed with 10 µg of unlabeled P. aeruginosa DNA, and following primary centrifugation, 0.8 to 1.0 µg of this DNA with density of 1.725 g ml1 was resolved in secondary CsCl gradients containing bis-benzimide. The peaks corresponding to 15N-labeled E. coli DNA and unlabeled P. aeruginosa DNA are labeled for clarity.
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Variability of genome G+C content within microbial communities has previously been suggested as a factor that needs to be considered during the interpretation of DNA-SIP experiments (36), but the magnitude of this problem has not before been demonstrated empirically. The use of DNA from pure cultures reveals the extent to which genome G+C content can affect DNA buoyant density (1, 3), and microbial communities have been shown to contain a complex mixture of genomes with a range of G+C contents (11, 12, 32, 33). However, in complex mixtures of DNA (and in the absence of intercalating agents that enhance differences in DNA buoyant density), interactions between DNA molecules could affect the apparent buoyant density of DNA fragments, thereby reducing the ability of DNA G+C content to affect buoyant density. For example, changes in DNA conformation can influence DNA buoyant density in CsCl density gradients, since native and denatured DNA from E. coli can differ in buoyant density by 0.015 g ml1 and circular and linear forms of the same DNA molecule will also differ in buoyant density (1). Thus, it could be hypothesized that DNA fragments from a complex mixture would be normally distributed within a density gradient, with a mean buoyant density corresponding to the mean G+C content of the community. However, Fig. 3 and Fig. S3 in the supplemental material provide separate lines of evidence that clearly demonstrate that this hypothesis is false. First, individual TRFs with distinct buoyant densities can be identified from soil DNA equilibrated in a density gradient (Fig. 3), and the range of buoyant densities spanned by these TRFs matches the range over which variation in genome G+C content is expected to influence DNA buoyant density based on theoretical predictions (Fig. 1). Second, analysis of T-RFLP profiles from soil DNA equilibrated in a density gradient reveals that the taxonomic composition of gradient fractions varies as a function of gradient density, consistent with the expectation that differences in genome G+C content affect the buoyant densities of DNA fragments within complex mixtures (see Fig. S3 in the supplemental material). The extent of the problem that variation in G+C content poses to DNA-SIP experiments can be easily seen, since the 102-bp TRF in Fig. 3A has a mean buoyant density of approximately 1.69 g ml1 and if the DNA from this organism was fully 13C labeled it would be expected to have a buoyant density of 1.726 g ml1, which overlaps considerably with unlabeled DNA from organisms with TRFs of 144 bp, 121 bp, and 177 bp (Fig. 3G, H, and I). These results, when considered in conjunction with the observation that the distribution of G+C contents in a microbial community can change in response to environmental characteristics (11, 12, 32, 33), emphasize the necessity of the proper use of controls in DNA-SIP experiments (22).
Our calculations show that DNA molecular weight is also a concern that must be considered when designing DNA-SIP experiments (see Fig. S1 in the supplemental material). Small DNA fragments below 2 kbp in length are commonly present in DNA preparations that use bead beating to achieve cell lysis (34), and this method of lysis is commonly employed for the extraction of DNA from environmental studies. These small DNA fragments may not reach equilibrium under the conditions typically used for establishing density gradients (see Fig. S1 in the supplemental material). An additional concern is that G+C content can vary locally within a genome, such that the G+C content of individual DNA fragments can vary from the mean genome G+C content. Thus, as a genome is cut into smaller and smaller fragments, the variation between the G+C contents of the individual fragments and the G+C content of the genome will tend to increase (44). The anticipated result would be that the range of densities occupied by DNA from a given genome (i.e., the width of the band in the gradient) would increase as the molecular weight of DNA fragments decreases. Thus, the G+C content of DNA fragments that are smaller than 5 kbp can vary by as much as 13% for a single genome (44). These effects may help to explain why low but detectable amounts of nucleic acids can be recovered throughout density gradients (8, 16, 19, 25, 37). Removal of DNA fragments smaller than 4 kbp (see Fig. S1 in the supplemental material) prior to ultracentrifugation is therefore a reasonable precaution that can potentially increase the resolution of DNA within density gradients.
One common concern associated with nucleic acid SIP experiments is that cross-feeding and trophic cascades can result in the movement of an isotopic label into nucleic acids from nontarget functional groups (5, 35, 36). The isotopic signature of nucleic acids from organisms involved in cross-feeding or secondary consumption should, as a natural consequence of label dilution, be less than that of primary consumers until the isotopic label saturates the community. Thus, by following the incorporation of the isotopic label into the community over time, it is possible to track the movement of the label from a substrate into particular functional groups and then into other components of the soil food web (5, 13, 18, 21). As a result, DNA from isotopically enriched environmental samples can contain a range of isotopic signatures from 0% to 100% label incorporation (28, 30, 45). It is possible to use nucleic acid fingerprinting methods to determine the degree of isotope incorporation by particular microbial groups by fingerprinting gradient fractions from isotopically labeled samples relative to controls (19, 20, 25). However, to identify the organisms that assimilated the label, it is necessary to match TRFs from particular gradient fractions with sequences obtained in clone libraries, a task which can prove difficult with complex communities (4, 7, 17). Also, the possibility that two or more organisms may share a particular TRF (7, 14, 27) can lead to difficulties in interpreting these data. The use of secondary density gradients containing bis-benzimide to purify isotopically labeled DNA from unlabeled DNA should be useful in these applications.
It is important to note that the behavior of DNA in density gradients differs considerably from that of rRNA. rRNA has greater buoyant density and lower molecular weight than DNA. It also has a more narrow range of G+C contents (more than 90% of 16S rRNAs have G+C content between 50% and 60%; personal observation calculated from 24,000 16S rRNA sequences) and extensive regions of secondary and tertiary structure (10). Variability in denaturing conditions during equilibration of rRNA molecules in density gradients can affect rRNA secondary structure, and as a result, rRNA from different species can have buoyant densities that range over 0.08 g ml1 (19). Thus, isotopically labeled rRNA may be expected to cooccur with unlabeled rRNA under certain circumstances but, unlike the case with DNA, this phenomenon is less likely to be driven by differences in nucleic acid G+C content. Thus, additional experiments and validation would be needed to determine whether the method we describe would be applicable to RNA-SIP applications.
The centrifugation and fractionation conditions that we describe are optimized to resolve DNA molecules that have very small differences in buoyant density. The collection of 100-µl fractions from density gradients allows for increased resolution of buoyant density relative to existing methods and results in highly reproducible density profiles with respect to fraction number (data not shown). In addition, the removal of small DNA fragments prior to centrifugation is a simple step that should theoretically enhance gradient resolution (see Fig. S1 in the supplemental material), but the magnitude of this effect still needs to be confirmed experimentally. These efforts to improve gradient resolution likely contributed to our ability to resolve differences in T-RFLP profiles and the distribution of individual TRFs that result from the effect of genome G+C content on DNA buoyant density in complex communities (Fig. 3). The use of gradient fractionation and T-RFLP fingerprinting of gradient fractions make it possible to identify gradient fractions that contain isotopically labeled DNA even when it cooccurs with unlabeled DNA. Subsequent purification of those target fractions in secondary density gradients containing bis-benzimide will facilitate separation of labeled DNA from unlabeled DNA and enable the identification and characterization of isotopically labeled organisms. This approach will make it possible to effectively use 15N-labeled compounds in DNA-SIP experiments and will be beneficial in a range of 13C-DNA-SIP applications.
Published ahead of print on 16 March 2007. ![]()
Supplemental material for this article may be found at http://aem.asm.org/. ![]()
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