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Applied and Environmental Microbiology, March 1999, p. 989-994, Vol. 65, No. 3
0099-2240/99/$04.00+0
Copyright © 1999, American Society for Microbiology. All rights reserved.

Steady-State Nitrogen Isotope Effects of N2 and N2O Production in Paracoccus denitrificans

Carol C. Barford,1,* Joseph P. Montoya,2,dagger Mark A. Altabet,3 and Ralph Mitchell1

Division of Engineering and Applied Sciences1 and Biological Laboratories,2 Harvard University, Cambridge, Massachusetts 02138, and Center for Marine Science and Technology, University of Massachusetts, Dartmouth, North Dartmouth, Massachusetts 027473

Received 21 August 1998/Accepted 4 December 1998


    ABSTRACT
Top
Abstract
Introduction
Materials and Methods
Results
Discussion
References

Nitrogen stable-isotope compositions (delta 15N) can help track denitrification and N2O production in the environment, as can knowledge of the isotopic discrimination, or isotope effect, inherent to denitrification. However, the isotope effects associated with denitrification as a function of dissolved-oxygen concentration and their influence on the isotopic composition of N2O are not known. We developed a simple steady-state reactor to allow the measurement of denitrification isotope effects in Paracoccus denitrificans. With [dO2] between 0 and 1.2 µM, the N stable-isotope effects of NO3- and N2O reduction were constant at 28.6per thousand  ± 1.9per thousand and 12.9per thousand  ± 2.6per thousand , respectively (mean ± standard error, n = 5). This estimate of the isotope effect of N2O reduction is the first in an axenic denitrifying culture and places the delta 15N of denitrification-produced N2O midway between those of the nitrogenous oxide substrates and the product N2 in steady-state systems. Application of both isotope effects to N2O cycling studies is discussed.


    INTRODUCTION
Top
Abstract
Introduction
Materials and Methods
Results
Discussion
References

The importance of denitrification in microbial ecology, N2O production, agricultural N loss and wastewater treatment has prompted a large body of research over the last 25 years. Although the basic pathway is well known (36),
<UP>NO</UP><SUB><UP>3</UP></SUB><SUP><UP>−</UP></SUP><UP>→NO</UP><SUB><UP>2</UP></SUB><SUP><UP>−</UP></SUP><UP>→NO→N<SUB>2</SUB>O→N<SUB>2</SUB></UP> (1)
the regulation and distribution of denitrification remain poorly understood. The sensitivity of denitrification to oxygen tension is of particular interest due to (i) the recent demonstration of denitrification under aerobic conditions (40, 41), (ii) increased N2O production under these conditions (12, 20, 28), (iii) the importance of linked nitrification-denitrification in N cycling in natural environments (11, 14), and (iv) development of "single-sludge" wastewater treatment as a low-cost alternative to traditional strategies that employ separate aerobic and anoxic reactors (26, 34, 47).

The natural-abundance 15N ratios of nitrogenous materials have been used to identify or quantify denitrification activity in low-oxygen environments, including the marine water column (24, 53, 54, 55), groundwater (15), sediments (1), and soil (25). These studies exploit the variation in the ratio of 15N to 14N in nitrogenous material that results from the isotopic discrimination of denitrification, in which 14N reacts faster than 15N. Thus, natural-abundance 15N ratios provide a small (approx 0.366% 15N) but endogenous in situ tracer of denitrification activity, in contrast to large 15N additions (50 to 99% 15N) traditionally used to trace biological N fixation and other N transformations. However, published estimates of the extent of isotopic discrimination, or isotope effect (varepsilon ), of denitrification range from 13 to 40per thousand , reflecting the variety of experimental methods and denitrifying cultures used (5, 6, 10, 13, 27, 50, 52). Because the varepsilon  of denitrification lies between those of other N transformations, such as N assimilation at 10per thousand (9, 19, 30) and nitrification at 13 to 16per thousand in situ (21) or 30 to 60per thousand in vitro (27, 52), it is desirable that varepsilon  be better constrained. In addition, possible variation in varepsilon  as a function of oxygen tension has not been investigated heretofore.

We measured varepsilon  of denitrification in pure cultures of Paracoccus denitrificans under dissolved-oxygen concentrations between 0 and 1.2 µM. We also measured a unique varepsilon  for N2O reduction in these cultures. For these experiments, we developed a simple, steady-state reactor which does not require a dedicated mass spectrometer or online sample preparation system, thus offering a flexible approach to investigators who do not routinely use stable-isotope techniques. The reactor was also used to measure oxygen isotope effects, which are reported elsewhere (4). This information expands the utility of stable isotope studies of denitrification in low-oxygen (<10 µM) environments. Here we describe the necessary steady-state fractionation models and the reactor configuration and performance and report the N stable-isotope effects for denitrification.


    MATERIALS AND METHODS
Top
Abstract
Introduction
Materials and Methods
Results
Discussion
References

Experimental design. Continuous cultures were used to control the dissolved-oxygen concentration ([dO2]) more easily and to exploit the simplicity of steady-state fractionation models, which relate kinetic varepsilon  values directly to the isotopic compositions of reactants and products. The isotopic composition of nitrogenous material is commonly expressed as a delta -value relative to atmospheric N2:
&dgr;<SUP>15</SUP><UP>N</UP> (‰)=[(R<SUB><UP>sample</UP></SUB>−R<SUB><UP>N</UP><SUB>2</SUB></SUB>)/R<SUB><UP>N</UP><SUB><UP>2</UP></SUB></SUB>]<UP> × 1,000</UP> (2)
where R = 15N/14N. In a single first-order reaction, in which the substrate pool is infinitely large, varepsilon  closely approximates the difference between the delta  values of the substrate and product (16). The isotopic dynamics of steady-state anoxic denitrification may be idealized as such a one-step process:
<UP>ϵ<SUB>0</SUB> = &dgr;<SUP>15</SUP>NO</UP><SUB><UP>3</UP></SUB><SUP><UP>−</UP></SUP><UP> − &dgr;<SUP>15</SUP>N<SUB>2</SUB></UP> (3)
where varepsilon 0 is the overall varepsilon  of denitrification. Alternatively, this pseudo-varepsilon may be partitioned: varepsilon 1, delta 1varepsilon 2, delta 2 delta 15NO3- right-arrow delta 15N2right-arrow delta 15N2 (4)

where varepsilon 1 and varepsilon 2 are the varepsilon  values of NO3- and N2O reduction, respectively, and delta 1 and delta 2 are the isotopic compositions of the instantaneous products of the two reactions. At steady state, delta 15N2O and delta 15N2 are constant; thus, delta 1 and delta 2 both equal delta 15N2. Applying the principle of equation 3 to equation 4 yields the following relationships:
ϵ<SUB>1</SUB>=&dgr;<SUP>15</SUP><UP>NO</UP><SUB>3</SUB><SUP>−</SUP>−&dgr;<SUB>1</SUB> (5a)
ϵ<SUB>2</SUB>=&dgr;<SUP>15</SUP><UP>N<SUB>2</SUB>O</UP>−&dgr;<SUB>2</SUB> (5b)
When delta 15NO3-, delta 15N2O, and delta 15N2 are measured experimentally and delta 15N2 is substituted for delta 1 and delta 2, equations 5a and 5b may be solved for varepsilon 1 and varepsilon 2, respectively. Note that varepsilon 1 = varepsilon 0, which is generally true for unbranched, nonreversible reaction pathways (37).

The approach described above allows the calculation of varepsilon 1 and varepsilon 2 by measuring delta 15N of three species at a single steady state. Independent checks of varepsilon 1 were calculated from isotopic mass balances of the reactor at multiple steady states. Because denitrification intermediates constituted very small fractions of reactor N at steady state, N isotope mass balances were written as follows:
D [<UP>NO</UP><SUB>3</SUB><SUP>−</SUP>]<SUB><UP>i</UP></SUB>&dgr;<SUP>15</SUP><UP>N<SUB>i</SUB></UP>=D [<UP>NO</UP><SUB>3</SUB><SUP>−</SUP>]<SUB><UP>ss</UP></SUB>&dgr;<SUP>15</SUP><UP>N<SUB>ss</SUB></UP>+R (&dgr;<SUP>15</SUP><UP>N<SUB>ss</SUB></UP>−ϵ<SUB>1</SUB>) (6)
where D is reactor dilution rate (time-1), R is the denitrification rate ([N] time-1), delta 15N is the delta  value of NO3-, and the subscripts "i" and "ss" refer to initial and steady state, respectively. Equation 6, like equation 3, implies that varepsilon 1 is equal to the steady-state difference between delta 15NO3- and delta 15N2. Because R equals the product of D and the concentration of substrate consumed in a continuous culture (chemostat) at steady state, equation 6 can be rewritten to eliminate R:
D [<UP>NO</UP><SUB>3</SUB><SUP>−</SUP>]<SUB><UP>i</UP></SUB>&dgr;<SUP>15</SUP><UP>N<SUB>i</SUB></UP>=D [<UP>NO</UP><SUB>3</SUB><SUP>−</SUP>]<SUB><UP>ss</UP></SUB>&dgr;<SUP>15</SUP><UP>N<SUB>ss</SUB></UP>+D ([<UP>NO</UP><SUB>3</SUB><SUP>−</SUP>]<SUB><UP>i</UP></SUB>−[<UP>NO</UP><SUB>3</SUB><SUP>−</SUP>]<SUB><UP>ss</UP></SUB>) (&dgr;<SUP>15</SUP><UP>N<SUB>ss</SUB></UP>−ϵ<SUB>1</SUB>) (7)
and may be rearranged into linear form:
&dgr;<SUP>15</SUP><UP>N<SUB>ss</SUB></UP>=ϵ<SUB>1</SUB>([<UP>NO</UP><SUB>3</SUB><SUP>−</SUP>]<SUB><UP>i</UP></SUB>−[<UP>NO</UP><SUB>3</SUB><SUP>−</SUP>]<SUB><UP>ss</UP></SUB>)/[<UP>NO</UP><SUB>3</SUB><SUP>−</SUP>]<SUB><UP>i</UP></SUB>+&dgr;<SUP>15</SUP><UP>N<SUB>i</SUB></UP> (8a)
&dgr;<SUP>15</SUP><UP>N<SUB>ss</SUB></UP>=ϵ<SUB>1</SUB>(f)+&dgr;<SUP>15</SUP><UP>N<SUB>i</SUB></UP> (8b)
where f is the fraction of NO3- consumed at steady state and varepsilon 1 equals the slope of steady-state delta 15NO3- as a function of f (17). Different values of f were achieved by manipulating the dissolved-oxygen concentration ([dO2]). Experimental [dO2] treatments were 0, 0.1, 0.3, and 1.2 µM.

Reactor configuration. The reactor system consisted of a medium reservoir, growth chamber, waste carboy, and connecting tubing and flow controls (Fig. 1). The 20-liter Pyrex carboy in which media were sterilized also served as the reservoir. A heavy-gauge aluminum lid and rubber gasket were secured to the reservoir with a collar and screws. The lid contained ports for gas entry, gas and medium exit to the growth chamber, and venting. Gas mixing and flow to the reservoir were controlled by a gas proportioner (Alltech, Deerfield, Ill.). Gas was conducted to the reservoir in 1/8-in. stainless steel tubing, through a 0.5-µm nominal matrix filter (Nupro, Willoughby, Ohio) and a sparging stone. Medium flow from the reservoir to the growth chamber was caused by positive pressure in the reservoir, which was in turn controlled by the sparging rate. Two needle valves (Nupro) were added to enable finer control of medium flow rate to the growth chamber. This mode of medium delivery was chosen over pumping due to the difficulty of maintaining absolutely anoxic connections between steel tubing and peristaltic pump tubing.


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FIG. 1.   Reactor configuration.

The growth chamber was a 2-liter Pyrex cylinder equipped with a magnetic stirrer and a stainless steel lid similar to the reservoir lid. In addition to gas and liquid entry ports, it contained a septum port for sampling by syringe, ports to accommodate a pH probe (Orion, Boston, Mass.), and a dO2 probe (Ingold, Wilmington, Mass.), a 3/8-in. port for gas and liquid exit to the waste carboy, and a 3/8-in. port fitted with a shutoff valve for headspace sampling. The pH probe was connected to a pH controller (Cole Parmer, Chicago, Ill.), which activated a peristaltic pump equipped with microbore tubing to introduce HCl into the growth chamber. This tubing entered the growth chamber through the septum port. The waste port was situated to give the growth chamber a working volume of 1.75 liters. Waste liquid and gas were forced by positive pressure into the 20-liter vented waste carboy through 3/8-in. stainless steel tubing.

Organism and media. P. denitrificans ATCC 17741, a relatively oxygen-sensitive, classic denitrifier, was chosen for the experiments (2). Cultures were purchased from the American Type Culture Collection (Rockville, Md.) and reconstituted in nutrient broth (Difco, Detroit, Mich.) at 30°C. Subcultures were frozen in glycerol and stored at -20°C until needed. The defined medium for continuous-culture experiments contained 30 mM nitrate and 20 mM acetate, which was the sole electron donor, carbon source, and limiting substrate (39). The composition of denitrification medium was as follows (in grams per liter): KNO3, 3.03; CH3COONa · 3H2O, 2.72; K2HPO4, 0.8; KH2PO4, 0.3; NH4Cl, 0.4; MgSO4 · 7H2O, 0.4; trace-elements solution, 2 ml liter-1. The trace-elements solution was modified from that of Vishniac and Santer (48) and contained (in grams per liter) EDTA, 50.0; ZnSO4, 2.2; CaCl2, 5.5; MnCl2 · 4H2O, 5.06; FeSO4 · 7H2O, 5.0; (NH4)6Mo7O24 · 4H2O, 1.1; CuSO4 · 5H2O, 1.57; CoCl2 · 6H2O, 1.61.

Reactor operation and sampling. Denitrification medium was autoclaved in 16-liter batches at 121°C and 15 lb/in2 for 80 min. Beginning immediately after sterilization, the reservoir was sparged with ultra-high-purity helium or O2 in helium (Med-Tech Gases, Medford, Mass.). The growth chamber, dO2 probe, liquid-sampling needle, waste vessel, and tubing were autoclaved and connected while hot. The pH probe was calibrated with standard buffers (Fisher Scientific, Fair Lawn, N.J.), surface sterilized with 70% ethanol, and inserted into the growth chamber. The chamber was filled to working volume with medium, which was sampled with a syringe when cool. The culture was then inoculated with 30 ml of stationary-phase P. denitrificans and grown in batch mode at 30°C to approximately 108 cells ml-1. Medium was then added at an appropriate dilution rate, and the pH was maintained at 8.0 by automatic addition of 1 M HCl. The [N2O] of the headspace gas was monitored daily until it stabilized within a few ppm (by volume). At this point, the reactor was assumed to have reached steady state (see below).

Once steady state was established for a given experimental [dO2] treatment, samples of each type were taken in triplicate. Liquid samples were drawn with a syringe and processed for either dissolved inorganic nitrogen concentrations (DIN) or cell N analysis. Samples (10 ml) for DIN analyses were filtered through 0.2-µm-pore-size cartridges (Gelman, Ann Arbor, Mich.), split into subsamples, and frozen until analysis of DIN or delta 15N. Unfiltered liquid samples for cell counts were preserved in 5% formalin and stored at 10°C until analysis. Unfiltered samples for direct cell N measurement were processed immediately after sampling, as described below.

Gas samples were collected in preevacuated, U-shaped Pyrex tubes (34-ml volume) fitted on either end with vacuum stopcocks (Ace Glass, Vineland, N.J.). For N2 collection, the U-tubes were coupled to the gas-sampling port of the growth chamber by using compression fittings with Teflon front ferrules and nylon back ferrules (Swagelok, Solon, Ohio). Each N2 collection tube contained several granules of silica gel for cryogenic absorption of N2 gas (33). With the growth chamber waste vent closed, U-tubes were opened and flushed with outgoing headspace gas (100 ml min-1) for at least 5 min. Each grab sample was then isolated by closing first the stopcock near the sampling port and then the outlet stopcock. This order was necessary to maintain atmospheric pressure and to enable back-calculation of the N2 production rate. Samples were stored in U-tubes for up to 2 days until purified and used for manometric determination of N2.

N2O was quantified by gas chromatography. Samples for gas chromatography were collected by flushing a 30-ml serum bottle with outgoing headspace gas via the gas sampling port. N2O samples for delta 15N and delta 18O determination were collected by trapping N2O out of the outgoing gas stream. This was necessary because the headspace [N2O] was too low (approx 0.1 µM) for grab samples of reasonable volume to yield the 2 to 6 µmol of N required for mass spectrometry. The N2O trap was a U-tube packed with borosilicate glass beads, which increased the trap surface area and dispersed the gas flow enough to trap N2O when chilled in liquid nitrogen (LN2). The efficiency of the N2O trap was verified by measuring zero N2O in the trap effluent. CO2 was removed from N2O samples by a scrubber in line between the growth chamber and the N2O trap. The scrubber consisted of a standard gas purification cartridge (Alltech) packed with a 3-cm layer of Carbosorb granules (Elemental Microanalysis, Manchester, Mass.) between two layers of indicating silica gel.

Cryogenic distillation. Gas samples were purified by standard cryogenic techniques (7). U-tubes were first immersed in LN2 to freeze the N2 or N2O sample onto silica gel or glass beads, respectively. The large overburden of helium carrier gas was then removed with a vacuum pump. N2 samples were further purified of CO2 and H2O by a LN2-cooled trap; O2 was removed by passing the sample over copper filings at 550°C. The purified N2 was quantified by using a capacitance manometer (MKS Baratron). N2O samples were further purified of H2O by using a glass trap cooled in an ethanol-dry ice slurry. Each N2 or N2O sample was refrozen in a Pyrex ampoule, sealed, and stored until analysis by continuous-flow isotope ratio mass spectrometry.

Analytical methods. Nitrate [NO3-] and nitrite [NO2-] concentrations were measured by the spongy cadmium reduction method (22). The ammonia [NH3 + NH4+] concentration was determined by the colorimetric method of Strickland and Parsons (45). The delta 15N of (NO3- + NO2-) was measured by the ammonia diffusion method as modified by Sigman et al. (43).

The N in bacterial cells was quantified by acridine orange direct counting (18) and a conversion factor for cell N concentration, which was found by performing cell counting and direct cell N measurement on the same samples over a range of cell densities. Direct measurements of cell N were made with a Europa elemental analyzer. To prepare a sample containing 2 to 6 µmol of N, approximately 1.0 ml of cell suspension was filtered onto a precombusted 25-mm-diameter GF/F filter. The filters were dried at 55°C and packed in tin boats before analysis. Cell N was calculated from the following regression (r2 = 0.8835, n = 4):
<UP>Micrograms of cell N per milliliter = 1.84 × 10</UP><SUP><UP>−8</UP></SUP> (9)
(<UP>cells per milliliter</UP>)<UP> − 13.16</UP>
N2O production was monitored by using a Hewlett-Packard 5890A gas chromatograph equipped with an electron capture detector (23). A 1/8-in.-diameter stainless steel column packed with Hayesep Q 80/100 mesh was used at 40°C. The injector and detector temperatures were 100 and 350°C, respectively, and the carrier gas was 5% methane in argon at 30 ml min-1. Under these conditions, N2O eluted approximately 1.9 min after sample injection. Calibration curves were prepared daily by using a standard gas mixture of 101 ppm (volume) N2O in N2 (Scott Specialty Gases, Reading, Mass.). Standard injections were performed periodically to check for signal drift.

The delta 15N of N2O, N2, and (NO3- + NO2-) and the delta 18O of N2O were measured on a Finnigan Mat 251 mass spectrometer (55). Samples were conducted by helium carrier flow (50 ml min-1) through Carbosorb and magnesium perchlorate traps to remove trace CO2 and H2O, respectively. The mass 29/28 ratio was measured for N2 samples and expressed as delta 15N relative to atmospheric N2. Injections of working standard N2 were made through a septum port in line with the carrier flow. For N2O samples, the mass 45/44 ratio, yielding delta 15N values, and the mass 46/44 ratio, yielding delta 18O values, were both measured for each sample. The mass spectrometer was calibrated with a standard of pure N2O gas kindly provided by T. Yoshinari, New York State Department of Health. N2O delta  values were expressed relative to the delta 15N and delta 18O of atmospheric N2 and O2, respectively.

Budget calculations. Dissimilatory (denitrification) and assimilatory N budgets were calculated for the reactor system. Each term in the dissimilatory budget was expressed as a percentage of the NO3- supplied in the medium:
<FR><NU>[<UP>NO</UP><SUB>3</SUB><SUP>−</SUP>]<SUB><UP>ss</UP></SUB></NU><DE>[<UP>NO</UP><SUB>3</SUB><SUP>−</SUP>]<SUB><UP>i</UP></SUB></DE></FR> (100%)+<FR><NU>[<UP>NO</UP><SUB>2</SUB><SUP>−</SUP>]<SUB><UP>ss</UP></SUB></NU><DE>[<UP>NO</UP><SUB>3</SUB><SUP>−</SUP>]<SUB><UP>i</UP></SUB></DE></FR> (100%)+% <UP>N<SUB>2</SUB>O<SUB>ss</SUB></UP>+% <UP>N<SUB>2ss</SUB> = % recovery</UP> (10)
The NO3- and NO2- terms were their respective steady-state concentrations (denoted by the subscript "ss") expressed as percentages of the initial NO3- concentration. The N2O term (%N2Oss) was the N2O-N production rate expressed as a percentage of the NO3- supply rate:
% <UP>N<SUB>2</SUB>O<SUB>ss</SUB></UP>=<FR><NU>(X<SUB><UP>N<SUB>2</SUB>O</UP></SUB>)(<UP>gas flow, liters/min</UP>)<FENCE><FR><NU><UP>1 mol</UP></NU><DE><UP>22.4 liters</UP></DE></FR></FENCE><FENCE><FR><NU><UP>2N</UP></NU><DE><UP>N<SUB>2</SUB>O</UP></DE></FR></FENCE>(<UP>100%</UP>)</NU><DE>([<UP>NO</UP><SUB><UP>3</UP></SUB><SUP><UP>−</UP></SUP>]<SUB><UP>i</UP></SUB><UP>1, mol/liter</UP>)(<UP>feed, liters/min</UP>)</DE></FR> (11)
where XN2O is the mole fraction of N2O in growth chamber headspace gas. The analogous N2 term, %N2ss, is shown below. The first factor in this equation was the amount of N contained in a 34-ml grab sample, which was measured manometrically during cryogenic distillation:
% <UP>N<SUB>2ss</SUB> = </UP><FR><NU><FENCE><FR><NU><UP>&mgr;g−atoms of N</UP></NU><DE><UP>0.034 liter of sample</UP></DE></FR></FENCE>(<UP>gas flow, liters/min</UP>)<FENCE><FR><NU><UP>1 mol</UP></NU><DE><UP>10<SUP>6</SUP> &mgr;g−atoms</UP></DE></FR></FENCE>(<UP>100%</UP>)</NU><DE>([<UP>NO</UP><SUB><UP>3</UP></SUB><SUP><UP>−</UP></SUP>]<SUB><UP>i</UP></SUB><UP>, mol/liter</UP>)(<UP>feed, liters/min</UP>)</DE></FR>
(12)

The assimilatory N budget consisted of the sum of cell N and NH3-N present at steady state, expressed as a percentage of NH3 supplied in the medium. Dissolved organic nitrogen compounds which may have been synthesized from NH3 were not included in the budget.


    RESULTS
Top
Abstract
Introduction
Materials and Methods
Results
Discussion
References

Reactor performance. Dissimilatory N recovery from the reactor system was near 100% over a range of dilution rates (Fig. 2). Residual [NO3-] increased with increasing dilution rate, but the cultures were not in danger of washout at the rates tested (39). Dissimilatory N recovery varied as a function of the sparging rate (Fig. 3), with particularly high N2 recovery at the lowest sparging rate, as discussed below. Assimilatory N recovery was 80 to 100% over the same range of dilution and sparging rates (data not shown). Dilution and sparging rates of 0.7 day-1 and 100 ml min-1, respectively, were held constant in further experiments, in which variable [dO2] was the sole experimental treatment.


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FIG. 2.   Dissimilatory N budget as a function of the dilution rate. Symbols are means and SE (n = 3). NO2- and N2O made up less than 1% of total N.


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FIG. 3.   Dissimilatory N budget as a function of the sparge rate. Symbols are means and SE (n = 3).

Experimental results. Under anoxic steady-state conditions, the reactor system yielded delta 15NO3-, delta 15N2O, and delta 15N2 of 15.5per thousand  ± 0.3per thousand , 0.08per thousand  ± 3.1per thousand , and -11.0per thousand  ± 1.2per thousand , respectively (mean ± standard error [SE], n = 6). According to these data and equations, 5a and 5b, varepsilon 1 = 26.5per thousand  ± 1.2per thousand and varepsilon 2 = 11.1per thousand  ± 3.1per thousand under anoxic conditions. The independent estimates of varepsilon 1 calculated from equation 8b and delta 15NO3- and delta 15N2O from multiple steady states at different [dO2] are similar although more variable (26.9per thousand  ± 2.6per thousand and 24.3per thousand  ± 4.0per thousand , respectively). However, varepsilon 1 calculated from delta 15N2 from multiple steady states was approx 14per thousand (Fig. 4). This discrepancy and the high N2 recovery at the low sparging rate (Fig. 3) suggested that significant isotopic signal from atmospheric N2 had biased the delta 15N2 values. To quantify this bias, the response of measured delta 15N2 to systematic air contamination, or a "handling blank," was simulated (Fig. 5). The expected delta 15N2 was first calculated by subtracting the slope of the NO3- regression in Fig. 4 (i.e., varepsilon 1) from points on that regression. The resulting straight line represents the delta 15N2 expected from constant fractionation and no air contamination. The expected delta 15N2 for the highest [dO2] treatment (the least biogenic N2) was compared to the measured value, and the amount of atmospheric N2 necessary to create the difference was calculated by mass balance. Simulation of constant fractionation with constant air contamination was then made by adding the isotopic contribution of this amount (0.5 µmol) of atmospheric N2 to the constant-fractionation values. The resulting curve fits very closely with the measured delta 15N2, suggesting that both varepsilon 1 and the amount of air contamination during sampling were constant for all [dO2] treatments.


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FIG. 4.   delta 15N as a function of NO3- consumption (f). Different fractions of f were caused by dO2 treatments. Symbols are means and SE (n = 3). The slope and SE of the slope of regressions of delta 15N versus f are 14.5 and 2.0 (N2), 24.3 and 4.0 (N2O), and 26.9 and 2.6 (NO3-). The asterisk represents the delta 15N of the NO3- supplied (-3.6per thousand ).


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FIG. 5.   Comparison between measured delta 15N2 from dO2 experiments (solid triangles) and dilution rate experiments (open triangles), the expected delta 15N2 given constant fractionation (straight line), and the expected value with a constant amount of air contamination (curved line). See the text for details.

To compare varepsilon 1 and varepsilon 2 between dO2 treatments, the delta 15N2 data were transformed to eliminate the effect of air contamination. This was done by subtracting from each measured delta 15N2 value the isotopic bias inherent in 0.5 µmol of atmospheric N2. The corrected delta 15N2 values for each treatment were then averaged, and these means were subtracted from the corresponding mean values of delta 15NO3- and delta 15N2O to yield varepsilon 1 and varepsilon 2, respectively (Table 1). Analysis of variance indicates that varepsilon 1 and varepsilon 2 varied more between reactor runs than between [dO2] treatments. The 1.2 µM dO2 treatment was excluded from the analysis of variance because low biogenic N2 production made delta 15N2 very sensitive to the mass balance correction (Table 1). Given the supporting evidence for systematic air contamination and the good agreement between intratreatment estimates of varepsilon 1 and regression models of intertreatment delta 15N2O and delta 15NO3- (Fig. 4), varepsilon 1 and varepsilon 2 were assumed to be constant over the range of dO2 treatments and are reported as the grand means 28.6per thousand  ± 1.9per thousand and 12.9per thousand  ± 2.6per thousand , respectively (means ± SE, n = 5).

                              
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TABLE 1.   Isotope effects for different dO2 treatments, calculated from transformed delta 15N2


    DISCUSSION
Top
Abstract
Introduction
Materials and Methods
Results
Discussion
References

The value of varepsilon 1 reported here falls well within the range in the literature (Table 2). All estimates of biological fractionation are well below 90per thousand , the maximum theoretical fractionation of N---O bond rupture (50). The precision of varepsilon 1 as measured in our steady-state system compares favorably with that measured by batch culture experiments (5, 13), in which varepsilon 1 was calculated by using the classic Rayleigh equation, which is sensitive to error in f (46). The value and precision of varepsilon 1 are similar to those reported by Mariotti et al. (27), who measured f by the acetylene block technique.

                              
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TABLE 2.   Measured values of the overall isotope effect of denitrification

The results reported here indicate that varepsilon 1 in P. denitrificans is constant over a range of dO2 concentrations. This constancy supports the validity of using varepsilon 1 to quantify, identify, or rule out denitrification fluxes in environments containing [dO2] gradients. However, other work indicates that biological kinetic fractionation can vary with environmental conditions. For sulfate reduction, Rees (38) hypothesized that the greater fractionation often measured in situ is due to slower growth in the field than in pure culture, but our dilution rate experiments indicated that the growth rate per se did not cause varepsilon 1 to vary (Fig. 5). Bryan et al. (8) showed that the overall varepsilon  of denitrification does vary with the denitrification rate in whole cells and cell extracts of Pseudomonas stutzeri limited by [NO2-], increasing to a maximum value of 25per thousand  ± 3.2per thousand at initial [NO2-] > 2.5 mM. The electron acceptor concentrations in our experiments were well within the asymptotic range reported by Bryan et al. (above 2.5 mM). These authors also found a negative correlation between varepsilon  and denitrification rate when the rate was increased by higher electron donor concentrations.

The isotopic composition of N2O in our experiments was quite distinct from both delta 15N2 and delta 15NO3-. The combined effects of varepsilon 1 and varepsilon 2 resulted in delta 15N2O being about 13per thousand heavier and 15per thousand lighter than delta 15N2 and delta 15NO3-, respectively, at steady state. To our knowledge, this is the first report of an isotope effect for nitrous oxide reduction in a denitrifying system. Yoshida et al. (53) cited unpublished data which yielded a value of 27per thousand for varepsilon 2 in P. denitrificans, but they did not specify whether the bacteria were supplied with N2O, NO2-, or NO3-. Yamazaki et al. (51) reported a maximum varepsilon  of 39per thousand for N2O reduction by the N2 fixer Azotobacter vinelandii, but nitrogenase, not nitrous oxide reductase, appeared to be responsible for the observed activity.

The expression of isotopic fractionation by P. denitrificans was strongly influenced by [dO2]. Within the narrow range between 0 and slightly more than 1.2 µM dO2, the delta 15N of NO3- and N2O varied up to 26per thousand and delta 15N2 probably varied to an equal extent (Fig. 4). However, the usefulness of [dO2] as a predictor of delta 15N in denitrifying environments may be limited to the extent to which it controls NO3- consumption. The expression of varepsilon  in natural and applied systems will also depend on the distribution of denitrifiers. P. denitrificans is very sensitive to dO2 in comparison to some denitrifiers, such as Comamonas sp. (35) and Thiosphaera pantotropha (39), which under aerobic conditions maintain 40 and 25% of their anaerobic denitrifying activity, respectively. However, Pseudomonas fluorescens, which frequently dominates denitrifying environments, denitrifies over approximately the same range of [dO2] as P. denitrificans (28). Chemostat studies of P. halodenitrificans revealed only slightly higher tolerance to dO2, to ~2 µM (20).

It is hoped that varepsilon 1 and varepsilon 2 may be used to help distinguish between denitrification and nitrification as sources of N2O and may serve as in situ tracers of both processes. For example, if the delta 15N of the substrate pools for both processes, NO3- and NH4+, respectively, are assumed to be zero, then denitrification- and nitrification-produced delta 15N2O in open systems at steady state would be ca. -15per thousand and -65per thousand , respectively (52). However, the isotopic composition of substrate pools in real systems could obscure this distinction. The delta 15N of NO3- and NH4+ vary from -23 to +43per thousand and -20 to +50per thousand , respectively, depending upon the source and the combined fractionation effects of redox reactions in the environment (49). Given these ranges, it is possible that denitrification- and nitrification-produced delta 15N2O would be indistinguishable. Linked nitrification-denitrification may also confuse delta 15N2O signatures by increasing the range of potential substrate molecules, which may in turn may have variable delta 15N (56). In environments such as sediments and biofilms, spatial linkage between nitrification and denitrification is on the order of 1 mm or less, and in single microorganisms such as Thiosphaera pantotropha, which both denitrifies and nitrifies in aerobic environments, N2O may be produced from NH4+, NO3-, and NO2- (3). However, in many environments (9, 19, 29, 31), the delta 15N of substrate pools can be constrained within a range of 10per thousand (see, e.g., references 1, 32, and 42), and the isotopic composition of N2O could provide a simple index to the relative contribution of the two processes producing N2O.


    ACKNOWLEDGMENTS

We thank J. Nevins for generous technical assistance and M. Hullar and J.-D. Gu for helpful discussion.

This work was supported in part by NASA NAG 2-843 (awarded to R.M.), NSF OCE-95-30187 and NSF DEB-96-33510 (awarded to J.P.M.), and NSF OCE-95-26356 (awarded to M.A.A.).


    FOOTNOTES

* Corresponding author. Mailing address: Department of Earth and Planetary Sciences, Harvard University, 20 Oxford St., Cambridge, MA 02138. Phone: (617) 495-9624. Fax: (617) 495-2768. E-mail: ccb{at}io.harvard.edu.

dagger Present address: School of Biology, Georgia Institute of Technology, Atlanta, GA 30332.


    REFERENCES
Top
Abstract
Introduction
Materials and Methods
Results
Discussion
References

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Applied and Environmental Microbiology, March 1999, p. 989-994, Vol. 65, No. 3
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