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Applied and Environmental Microbiology, September 2001, p. 3771-3778, Vol. 67, No. 9
0099-2240/01/$04.00+0 DOI: 10.1128/AEM.67.9.3771-3778.2001
Copyright © 2001, American Society for Microbiology. All rights reserved.
MINIREVIEW
Measurement of Denitrification in Sediments with
the 15N Isotope Pairing Technique
Sandra Martina
Steingruber,*
Jana
Friedrich,
René
Gächter, and
Bernhard
Wehrli
Swiss Federal Institute for Environmental
Science and Technology (EAWAG), Limnological Research Center, 6047 Kastanienbaum, Switzerland
 |
INTRODUCTION |
Due to increasing nitrogen
concentrations in surface waters (6) and eutrophication of
coastal waters (14, 26, 51), the quantification of
denitrification rates in sediments of lakes, rivers, and estuaries has
gained importance. Different methods for measuring denitrification have
been developed: the acetylene inhibition technique (41),
measurement of nitrate disappearance (2), calculation of
nitrate fluxes into the sediment from pore water profiles
(20), the 15N nitrate dilution method
(16), direct measurement of N2 production (40), the nitrogen mass-balance approach (1),
and the 15N isotope pairing technique (IPT)
(23). All of these methods have advantages but also
potential problems and limitations (38, 39).
The acetylene inhibition technique is a very simple method. It is
widely used, and its sensitivity has been improved by N2 measurements based on N2/Ar ratios. However, many different
studies have documented that the acetylene method systematically
underestimates denitrification (20). Several causes may be
responsible for artifacts: (i) inhibition of coupled
nitrification-denitrification by acetylene (19), (ii)
incomplete blockage of N2O reductase at low nitrate
concentrations (3), (iii) incomplete blockage of
N2O reductase when sulfide is present (3),
(iv) diffusion of N2O toward deeper sediment layers and
reduction to N2 (39), and (v) catalytic
oxidation of NO into NO2 (4). The
disappearance of nitrate can overestimate denitrification because
nitrate may not only be denitrified but also reduced to ammonia
(16, 20) or assimilated (36). On the other
hand, it may also underestimate denitrification because it does not
consider coupled nitrification-denitrification. The calculation of
nitrate fluxes into the sediment from pore water profiles has the same
problems as described for the nitrate disappearance method. In
addition, the resulting fluxes across the sediment-water interface and
the diffusive boundary layer often underestimate denitrification,
because of insufficient vertical resolution of the profiles and because
only diffusive and not turbulent transport is considered when the
fluxes are calculated (11, 21). The 15N
nitrate dilution method with subsequent measurement of 15N
nitrate disappearance and 15N ammonia production quantifies
denitrification and nitrification but still neglects coupled
nitrification-denitrification and assimilation. Direct measurement of
N2 production has the advantage to include coupled
nitrification-denitrification but requires a very sensitive analysis
because of the small N2 production compared to the
N2 background. The mass-balance approach on larger systems
such as whole lakes may lead to considerable errors due to a
combination of the errors of each term in the mass-balance.
The 15N IPT has the advantage that denitrification of both
NO3
diffusing from the overlaying water and
NO3
from nitrification within the sediment
can be quantified.
The purpose of this study is to briefly describe the principles of the
15N IPT, to review the different applications of the
15N IPT in sediments, to point out the advantages and the
limitations of the method, and to assess the main research topics,
which benefit from different applications of the method. The review
covers publications between 1992 and 2000.
 |
PRINCIPLES OF THE 15N IPT |
Denitrification in the sediment can occur at the expense
of NO3
from the water column (DW)
or of NO3
produced within the sediment by
nitrification (Dn). These two pathways can be analyzed by
the 15N IPT, which was developed by Nielsen
(23). The method relies on stable isotope tracers. The
natural abundance of nitrogen isotopes is 99.64% of 14N
and 0.36% of 15N.
15NO3
tracer is added to the
sediment overlying water. This
15NO3
mixes with the
14NO3
present in the water column
and in the upper sediment layer. Denitrification of this nitrate
mixture (Dtot) produces N2 molecules with
possible molecular masses of 28, 29, and 30 according to the
isotopic signature of the tracer mixture.
From the production rate of 29N2
(r29) and 30N2 (r30) it
is possible to calculate denitrification of
15NO3
(D15) as
follows:
|
(1)
|
For the calculation of the denitrification rate D14 of
unlabeled 14NO3
, Nielsen
(23) derived the relation:
|
(2)
|
The total denitrification rate in the sediment is, of course:
|
(3)
|
The denitrification rate of
15NO3
(D15) allows us
to calculate denitrification of the 14N/15N
nitrate mixture diffusing from the water column into the sediment (D
):
|
(4)
|
where
represents the isotopic nitrate enrichment during the
incubation. It can normally be expressed as:
|
(5)
|
where the brackets indicate concentrations and the subscripts
a and b refer to after and before the
15NO3
tracer addition, respectively.
Finally, coupled nitrification-denitrification within the sediment
(Dn) can be estimated by the difference:
|
(6)
|
If we assume that D
follows a linear increase
with higher tracer concentrations, this rate can now be extrapolated
back to tracer-free conditions in order to obtain the natural
denitrification rate DW with nitrate diffusing from the
water column (15):
|
(7)
|
All of the parameters mentioned here are depicted schematically in
Fig. 1. Note that to simplify the figure
we neglected that nitrogen is naturally enriched with a small amount of
15N.

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|
FIG. 1.
Schematic representation of the transformation rates
during a 15NO3 tracer experiment.
D is the total denitrification of nitrate from the
water column. Dw is the denitrification of nitrate from the
water column without tracer addition. Coupled
nitrification-denitrification is given as Dn.
Dtot refers to the total denitrification rate during the
tracer experiment. The specific denitrification rates of
15N and 14N nitrate are given as
D15 and D14, respectively, and the production
rates of N2 with masses of 28, 29, and 30 are represented
by r28, r29, and r30,
respectively.
|
|
In the special case wherein there is initially no nitrate in the
water column, the added 15NO3
is
not diluted. Therefore, D
corresponds to
D15, DW is zero, and Dn equals
D14.
The reader is referred to the methodological studies (15,
23) for more details about the derivation of these equations.
 |
APPLICATION OF THE 15N IPT TECHNIQUE |
The 15N IPT technique has basically been
applied in four different ways: (i) in batch-mode assays (5, 7,
9, 10, 12, 13, 15, 17, 18, 19, 20, 23, 24, 25, 27, 28, 29, 30, 34, 35,
42, 43, 44, 45, 46, 47, 49, 50, 52, 53), (ii) in benthic flux
chambers (20, 24), (iii) in enclosures (34),
and (iv) in flow through systems (32, 33, 36, 37). A wide
range of aquatic systems have been investigated thus far. The
experimental conditions, and the resulting denitrification rates are
summarized in Table 1.
Batch-mode assays.
The batch-mode assay (Fig.
2a) developed by Nielsen
(23) has been applied to quantify denitrification in
sediments of streams (23, 30), lakes (20, 34, 42,
45, 47, 52), estuaries (5, 7, 9, 13, 17, 25, 27, 28, 29,
35), coastal waters (12, 15, 24, 43, 44, 46, 49, 50, 53), shelf sediments (19), shallow reservoirs
(10), and mangrove forests (18). In all
studies, undisturbed 3- to 15-cm-long sediment cores (internal
diameter, 2.6 to 20.0 cm) overlaid with 5 to 40 cm of water were
sampled. In most studies the cores were submersed uncapped into a tank
containing 10 to 70 liters of bottom water. In some studies the bottom
water was replaced with artificial water (23, 45, 47, 52).
The water overlying the sediment was stirred with a magnetic stirrer
(mostly 2 to 10 cm above the sediment) coupled to an external rotating
magnet. Lohse et al. (19) switched the momentum of these
magnets from clockwise to anticlockwise rotation every 5 s to
minimize the pressure gradient at the sediment water interface. Jensen
et al. (15) circulated the tank water with a pump. The
water temperature was held constant at in situ conditions.

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|
FIG. 2.
Set up of the application of the 15N IPT.
The gray area corresponds to the sediment, the dotted area indicates
the water without tracer, and the hatched area shows the water with
tracer addition. (a) Batch-mode assay. The figure represents a water
reservoir (labeled 1) with the incubation container filled with water
(labeled 2), with three cylinders containing sediment, water, and a
magnetic stirrer closed with rubber stoppers (black). (b) Flux chamber.
The figure represents a lander lowered at the sediment surface and
attached to a buoy; the flux chamber (labeled 1) is inserted in the
sediment with two empty and two filled sampling syringes (labeled 2)
and the magnetic stirrer. (c) Water enclosure. The figure represents
the cylinder (labeled 1) pushed into the sediment and the plastic bag
(labeled 2), which is open toward the sediment and toward the water
surface. (d) Flow through system. The figure represents a water
reservoir (labeled 1), with the incubation chamber (labeled 2) flowed
through by a water flux and containing sediment, water, and a magnetic
stirrer.
|
|
In most of the studies, 15NO3
was
added after 0 to 24 h of preincubation to the tank to final
concentrations of 5 to 333 µM. The final nitrate composition ranged
between 5 and 100% of 15NO3
.
After tracer addition, the water in the reservoir was allowed to
equilibrate with sediment pore water for 10 to 30 min, sometimes by
stirring the water manually with a rod. In order to obtain a
near-steady-state efflux of labeled dinitrogen, Kristensen et al.
(18) let the system equilibrate for 12 to 14 h.
Afterward, the cores were capped with rubber stoppers. Capping the
cores represents a reliable starting point for the accumulation of
labeled N2. The cores were sometimes incubated in the dark
to simulate in situ conditions (13, 15, 18, 20, 27, 34, 42, 45,
46, 47, 49), with a parallel daylight setup to study diurnal
variation of denitrification (5, 7, 25, 30, 35, 44, 53) or
by alternating light and darkness (10). During the
incubation lasting from 0.4 to 24 h (depending on the season and
on the station), the O2 concentration did not decrease to
below 80 to 70% of saturation. To maintain O2
concentration at near in situ levels, Nielsen and Glud
(24) purged the water with a N2-air mixture.
The nitrate concentration in the water tank was normally measured
before and after addition of the tracer in order to calculate the
15N enrichment
. The production of
29N2 and 30N2 was
determined in two ways: (i) by following the production of
29N2 and 30N2 over time
(time series experiment [15, 19, 23, 24, 34, 35, 52])
and (ii) by determining the concentration of 29N2 and 30N2 at the
beginning and the end of the incubation (endpoint experiment [5,
7, 9, 10, 12, 13, 18, 25, 27, 29, 30, 44, 45, 46, 47, 49, 53]).
The first approach sacrifices cores at time intervals, whereas the
second approach sacrifices all the cores at the same time. In fact, in
both experiments the incubation was stopped by mixing the whole
sediment or the upper centimeters of the sediment with the overlaying
water to a slurry. To stop bacterial activity, a ZnCl2
solution was added to the cores before mixing. The slurry samples for
29N2 and 30N2 analysis
were stored in gastight containers (exetainers), containing some drops
of a ZnCl2 solution. Entrapment of air was carefully avoided. Friedrich et al. (unpublished data) and Steingruber
(42) stored the samples in evacuated glass vials
containing some drops of a ZnCl2 solution, which were only
half filled to permit equilibration of 29N2 and
30N2 with the gas phase. In contrast,
Kristensen et al. (18) needed to sample only the water
phase because the long preincubation time after tracer addition (12 to
14 h) after tracer addition led to a steady-state efflux of
labeled dinitrogen.
Before mixing the water column with the sediment, Lohse et al.
(19), Nielsen and Glud (24), Friedrich et al.
(submitted for publication), and Steingruber (42) sampled
also the water column to determine the amount of
29N2 and 30N2 trapped
in the sediment. They found that >75, 80, >73, and >80%,
respectively, of 29N2 and
30N2 was trapped in the sediment.
The time-series and the endpoint experiments have both advantages and
drawbacks. The former permits one to control whether production of
29N2 and 30N2 occurs
linearly with time. The disadvantage is that a single denitrification
rate is based on a number of sediment cores, which may differ in
quality due to heterogeneity of the sediments. The endpoint experiment
avoids this problem because, for each incubated core, a specific
denitrification rate is determined. However, no information is obtained
about the linearity of the 29N2 and
30N2 production. Friedrich et al. (submitted
for publication) and Steingruber (42) combined the two
sampling methods to avoid the main disadvantages. They calculated the
production of 29N2 and
30N2 in the same way as described in the
endpoint experiment, obtaining a denitrification rate for each core. In
addition, they tested the linearity of the production by sampling the
water phase of the cores with a syringe during the incubation at
different time intervals. During the experiment the sampled water
volumes were automatically replaced by tank water. Of course, such a
linearity test in the overlying water rests on the assumption of a
close coupling between the water column and the processes in the
anerobic sediment horizons. The procedure will therefore be of limited value in sediments with a thick oxic layer.
Benthic flux chambers.
Application of the 15N IPT
to benthic chambers (Fig. 2b) is based on the same principles as the
batch-mode assay. However, addition of
15NO3
and sampling occur in situ
at the sediment surface and not in a water-filled container. Nielsen
and Glud (24) used this technique to study coastal
sediments, and Mengis et al. (20) adapted it to study deep
lake sediments. The flux chambers contained one to two chambers,
covering a sediment area between 400 and 900 cm2 and
enclosing 3 to 12 liters of water.
15NO3
was added from a syringe to
the sediment overlaying water reaching a concentration of 35 and 50 µM (24) and 119 µM (20). During the
experiment the water volume was continuously mixed with a magnetic
stirrer, keeping the diffusive boundary between 0.4 and 1 mm. Oxygen
was measured with sensors, and water samples were taken at regular time
intervals. Nielsen and Glud (24) incubated samples for
only 3 h, ensuring that oxygen was not depleted by more than 25%.
Risgaard-Petersen et al. (33) and Rysgaard et al.
(37) showed that the concentrations of the N species did not change linearly with time if the O2 concentration
decreased by more than 20%. Mengis et al. (20) incubated
samples for 60 h and, although oxygen was depleted by 75%,
NO3
, NH4+, and
N2 still changed linearly with time. After incubation the flux chambers were retrieved on deck. Water samples for determination of 29N2 and 30N2 were
filled in exetainers (12.4 ml) containing 250 µl of ZnCl2 (50% [wt/wt]) without entrapping gas bubbles and closed gastight (24). To extract 28N2,
29N2, and 30N2
entrapped in the sediment Nielsen and Glud (24) took
sediment cores from the chamber, mixed the sediment and the overlaying water gently, and sampled the mixture as described above. Mengis et al.
(20) did not sample the slurry and calculated the
denitrification from the increase of labeled dinitrogen in the sampled
water volumes. Mengis et al. (20) also included the
isotopic composition of NO3
and
NH4+ in their analysis in order to obtain a
mass balance of 15N.
Water enclosures.
Similar to the flux chambers, enclosures
(Fig. 2c) are setups permitting in situ measurements. However,
enclosures integrate over larger spatial scales. Mixing of the water is
promoted by wave forces and not by a magnetic stirrer. The enclosure of
Risgaard-Petersen et al. (34) consisted of a plastic bag
that was open on two sides, fixed to a metal cylinder (inner diameter,
150 cm; height, 120 cm), and pushed into the sediment of a shallow lake.
15NO3
was added to the water to
final concentrations of 30 and 100 µM. In order to estimate the
outgassing of N2, Ar was added as a second tracer to the
enclosure. During an incubation of 24 h, the water column and the
sediment were sampled with glass tubes. Samples of the sediment and the
water column were obtained with a Plexiglas tube and mixed after a
ZnCl2 solution was added to stop bacterial activity.
Samples were preserved with ZnCl2 and stored in exetainers
until analyses.
Flow through systems.
In contrast to the applications of the
15N IPT discussed thus far, flowthrough systems (Fig. 2d)
are operated at steady-state conditions (32, 36). Sediment
cores were incubated in gastight glass chambers connected to a
thermostated continuous flowthrough system. Artificial freshwater or
seawater was supplied via the inflow. The flow rate ranged from 17 to
300 ml h
1. Nitrate concentrations of the inflows ranged
from 50 to 200 µM, with about 13% to 99% as
15NO3
. Risgaard-Petersen et al.
(32, 33) and Rysgaard et al. (36, 37)
adjusted the oxygen and the N2 concentration in the
inflowing water with a gas-mixing system. The water in the chamber was
gently mixed by a magnetic stirrer not disturbing the sediment.
Preincubation for reaching steady-state conditions lasted between 7 and
14 days, and the incubation itself lasted between 12 and 32 days.
During the incubation inlet and effluent were sampled periodically. In the study of Rysgaard et al. (36), the outflowing water
passed through a 50-ml flask that was heated to 75°C to strip the
gases. Gas samples for analyses of isotopic composition of
N2 were taken with a syringe through a butyl stopper.
Oxygen concentrations were measured with a microsensor (36,
37).
As mentioned above, the application of the 15N IPT in a
flowthrough system has the advantage of operating at steady-state
conditions. For this reason the flowthrough system is suitable
for studying such different parallel processes as assimilation,
nitrification, and mineralization.
 |
ANALYSES AND CALCULATIONS |
Continuous-flow isotope ratio mass spectrometers are typically
used to perform analyses for the IPT. The sample preparation of such a
modern setup is much simpler than for conventional dual-inlet mass
spectrometers. To analyze the isotopic composition of N2 in
water samples, an He headspace is introduced into the exetainers and,
after vigorous shaking for a few minutes, more than 98% of the
N2 is found in the gas phase. The gas phase is then
injected into a gas chromatograph in line with a triple-collector mass spectrometer to obtain the isotopic composition of N2.
The concentrations of 29N2 and
30N2 in the water or slurry is calculated in
the following way:
|
(8)
|
where brackets indicate the concentrations and
[29N2] · [28N2]
1 is the ratio obtained
with mass spectrometry. [28N2] is calculated
with Henry's law:
|
(9)
|
where KH(T) is the temperature-dependent
Henry constant and pN2 is the
partial pressure of dinitrogen in the atmosphere (0.78 atm).
Calculation of the production rates of
29N2 (r29) and
30N2 (r30) depends on the
experimental setup. For the time-series incubations of the batch-mode
assay, production rates r29 and r30 are
obtained from a relation like the following (here shown for
r29):
|
(10)
|
where m29 is the slope of the linear regression line
of [29N2] plotted against time,
A is the surface of the incubated sediment, Vw is the incubated water volume,
Vs is the volume of the sediment (both in
liters), and
is the sediment porosity.
For the endpoint incubation in the batch-mode assay,
r29 and r30 are calculated as follows (here
shown for r29):
|
(11)
|
where [29N2]f and
[29N2]i represent the final and
initial concentrations of 29N2 and t
is the time interval. Initial concentrations can be determined by
analyzing the water phase before capping the cores or by scarifying a
reference core at the beginning of the experiment and measuring the
concentrations in the water-sediment slurry.
The production rates of labeled dinitrogen in the flux chambers
should be determined using the formula of the endpoint experiment (equation 11), where [29N2]f is
the concentration of 29N2 in the water-sediment
slurry of the core subsampled at the end of the experiment.
For calculating r29 and r30 in the enclosure,
equation 10 can be used. In this case, when
[29N2] and [30N2]
are plotted against time to obtain m29 and m30,
not only the amounts of 29N2 and
30N2 measured in the slurry should be
considered but also the amount lost to the atmosphere. The method used
to estimate the gas loss is described elsewhere (34).
The production rates r29 and r30 in the
flowthrough system are calculated as follows (here shown for
r29):
|
(12)
|
where [29N2]out and
[29N2]in are the concentrations
of 29N2 and 30N2 in the
outlet and in the inlet, respectively. F is the water flow
through the chamber.
The calculated production rates of 29N2
and 30N2 (r29 and r30)
can then be inserted in equations 1 to 6 to calculate the
denitrification of NO3
from the water column
and coupled nitrification-denitrification.
 |
DISCUSSION |
Assumptions of the 15N IPT.
The 15N
IPT is based on four assumptions (23, 35), which are
briefly discussed below.
(i) Added 15NO3
does not
interfere with denitrification of in situ
NO3
.
This requirement can be tested by
adding different amounts of 15NO3
to the sediment overlaying water (23). The rates obtained
from such experiments (Dw and Dn, Fig. 1)
should remain independent of the concentration of the added tracer. In
several studies (15, 19, 24, 29, 35, 45),
15NO3
was added from a minimum of
10 µM to a maximum of 400 µM without modifying the in situ
denitrification rate. However, this makes it not superfluous to test
the interference of the addition of 15NO3
before every experiment,
because the optimal tracer range depends not only on the nitrate
concentration but also on the heterogeneity, stability, and activity of
the sediment and the incubation process.
(ii) Denitrification of nitrate from the water column
(Dwtot) should increase linearly with the
nitrate concentration.
The calculation of Dw
(denitrification of in situ
14NO3
) from
Dwtot (denitrification of
14NO3
plus added
15NO3
) depends on this
assumption. This assumption can also be tested by adding different
amounts of the 15N tracer. At elevated nitrate
concentrations, denitrification may no longer depend linearly on the
concentration of nitrate. At high nitrate concentrations saturation
effects may occur due to limited supply of electron donors or
Michaelis-Menten-type saturation. In addition, the nitrate penetration
depth will increase and cause a nonlinear response of denitrification
rates to the concentration in the overlying water.
(iii) Labeling of in situ NO3
with
15NO3
in the water column and in
the sediment must be homogeneous.
Heterogeneity of the sediment
and bioturbation can affect the ratio between nitrification and
NO3
flux at different spots in the sediment.
As a result, dinitrogen is produced preferentially as isotope pairs
28N2 and 30N2. Higher
r30 and r28 rates compared to r29
cause an underestimation of D14 and D15 (see
equations 1 and 2). However, Nielsen (23) reports that at
higher concentrations of 15NO3
more of the denitrified 14NO3
will be measured as 29N2. As a result,
the possible miscalculation of 28N2 production
will be of less significance compared to situations with lower
concentrations of 15NO3
. Nielsen
suggests that the 15NO3
concentrations are high enough when D14 becomes independent
of the 15NO3
concentrations.
However, van Luijn et al. (52) argue that in the case of
anaerobic microsites that may exist in the aerobic layer, nitrifying
and denitrifying bacteria may be ideally positioned, allowing a tightly
coupled nitrification-denitrification. Accordingly, around these
microsites the condition of uniform labeling is still not fulfilled,
even when the 15NO3
concentration
increases, so that coupled nitrification-denitrification is still
underestimated. Middelburg et al. (22) demonstrated in a
modeling study that the condition of homogeneous labeling is fulfilled
only when nitrification and denitrification occur in distinct separate
zones. Small-scale heterogeneity supporting denitrification within the
aerobic layer interfere with this condition and may underestimate the
denitrification rate. A final resolution over the controversy of the
role of microsites is likely to come from studies combining microsensor
or tomographic work to characterize sediment heterogeneity. Nielsen et
al. (23) and Welsh et al. (53) also suggested
an underestimation of coupled nitrification-denitrification when the
sediments are colonized by macrophytes. The reason is that coupled
nitrification-denitrification can occur close to the roots deep in the
sediment remote from the diffusion zone of the 15N tracer.
(iv) A stable NO3
concentration gradient
across the sediment water interface must be established shortly after
15NO3
addition.
This is
important, because otherwise
15NO3
will not be immediately
available for denitrification, leading to an underestimation of the
initial denitrification rate. A too-short incubation time results in an
increasing production rate of 29N2 and
30N2. If
15NO3
is initially well mixed in
the water column, the time to establish a stable gradient depends on
the oxygen penetration depth. It determines the diffusion length of
nitrate molecules to reach denitrifying bacteria. The time to reach a
steady-state gradient depends on microbial activity: it will be longer
in oligotrophic than in eutrophic systems and longer in winter than in
summer. According to Nielsen (23), the equilibration time
was 8 min at an oxygen penetration depth of 1 mm. Dalsgaard
(8) developed a model that predicts the equilibration time
as a function of the oxygen penetration depth. Due to their long
preincubation times, the flowthrough systems exhibit the most stable
nitrate gradients.
To meet all four conditions, D14 must be independent of the
tracer concentration and D15 must increase linearly with
increasing 15NO3
concentrations.
Furthermore, measuring the production of labeled N2 in a
time series allows us to verify a constant denitrifying activity.
Whether the fulfillment of these tests also excludes the
underestimation of denitrification in the case of coupled nitrification-denitrification within microsites is still a matter of controversy.
Comparison of different applications and methods.
Lohse et al.
(19) and Svensson (45) compared the acetylene
inhibition technique with the 15N IPT in the batch-mode
assay. The 15N IPT yielded denitrification rates two
times (19) and three to eight times
(45) higher than the acetylene inhibition technique because acetylene inhibits also nitrification-denitrification, which
was the main denitrification mechanism. Similar observations were
reported by Seitzinger et al. (39). Van Luijn et al.
(52) observed that denitrification rates measured with the
15N IPT were also smaller than those estimated with the
N2 flux method. In contrast, Risgaard-Petersen et al.
(32) observed good agreement of the two methods in the
same flowthrough system. These authors concluded that the bad agreement
of the two methods described by van Luijn et al. (52) was
due to the longer preincubation time necessary for the N2
flux method, which caused an accumulation of nitrate and ammonia,
leading to an overestimation of denitrification. However, results from
the N2 flux experiment of van Luijn et al. (52) agreed well with the nitrogen mass-balance of the
studied lake, while the results obtained from the 15N IPT
in the batch-mode assay resulted in lower denitrification rates. These
authors proposed an underestimation by the IPT due to the presence of
coupled nitrification-denitrification in microsites within the aerobic
layer. In contrast, Nielsen et al. (25) found a good
agreement between the nitrogen mass-balance of an estuary and results
from the 15N IPT in the batch-mode assay. Similar results
were reported in two deep lakes (20). In the study of
Steingruber (42), denitrification rates from the
batch-mode assay were higher than the results from a mass-balance
calculation of a shallow lake. It was proposed that the sampled bottom
water for the incubation experiment may not have been representative
for the whole lake (differences in nitrate concentrations). Comparison
of the 15N IPT in the batch-mode assay and in an enclosure
experiment in a shallow lake yielded denitrification rates 6 to 26 times higher in the enclosure (34). In the same
lake the annual average denitrification estimated from whole lake
mass-balance calculations was about three times higher than the
rates estimated with the 15N IPT in the batch-mode assay.
These authors concluded that the batch-mode assay underestimated in
situ denitrification rates in shallow lakes due to lower turbulent
mixing and thus transport of nitrate into the sediment. Mengis et al.
(20) and Nielsen and Glud (24) compared the
application of the 15N IPT to the use of a benthic chamber
with the batch-mode assay. The two methods yielded similar results
which also corresponded well to the results from the mass-balance calculations.
In summary, the 15N IPT applied in different experimental
designs compared to other methods to measure denitrification yielded sometimes contradictory results. However, it seems that the application of the 15N IPT to the batch-mode assay, the flowthrough
system, and probably also the flux chamber may give correct results for
deep lakes or estuaries, while it may underestimate denitrification
rates in shallow waters due to suboptimal turbulent mixing in the setups.
Advantages and limitations of different applications of the
IPT.
Three major limitations of the IPT deserve further attention
independent of the mode of application. (i) So far no technique provides satisfactory simulation of the turbulent mixing conditions in
shallow lakes. In the future,
15NO3
tracer could be added to
whole ponds in order to incubate the tracer under the most realistic
conditions. (ii) It is still not clear whether an underestimation of
denitrification in the case of coupled nitrification-denitrification in
microniches of oxic zones can be excluded, when D14 is
proved to be independent of the amount of added tracer. More research
in order to clarify this issue is needed. (iii) The anaerobic oxidation
of ammonium into dinitrogen with nitrate serving as an electron
acceptor (anammox reaction), which has been recently reported to occur
in sea sediments (T. Dalsgaard, Abstr. ASLO Aquat. Sci. Meet.
2001), can also limit the application of the IPT. Ogilvie et al.
(27) suggested that in the presence of the anammox
reaction, coupled nitrification-denitrification may be overestimated,
while the total denitrification result would be correct. Further
research is needed regarding this issue.
The 15N IPT applied to the batch-mode assay is a
straightforward, quick, and reliable method to determine
denitrification rates. A major problem arises when denitrification
occurs deep in the sediment, causing an extended equilibration time
and, as a result, a changing production rate of dinitrogen. In such
cases the flowthrough system will provide more accurate results.
The flux chamber technique is more time-consuming. The quite complex
benthic chambers are difficult to transport and to deploy (48). However, it allows measurements with minimal
sediment disturbance under in situ conditions. The disadvantages of the 15N IPT in flux chambers are basically the same as for the
batch-mode assay. In addition, the mixing of the tracer at the
beginning of the experiment cannot be controlled manually. This usually causes a nonlinear production of labeled N2 during the
startup phase. When most labeled dinitrogen remains in the sediment
(24), denitrification has to be determined with an
endpoint experiment. This implies that a sediment-water slurry has to
be sampled on board. If degassing of the sediment due to decreased
pressure and/or manipulation cannot be prevented, this might cause a
problem. In addition, careful timing is essential for autonomous
benthic landers (48), because the time period between the
end of the incubation and the sampling of the slurry can be quite long.
Application of the 15N IPT to a flowthrough system requires
a relatively complicated technical setup. However, because steady-state conditions are maintained, this approach avoids problems of
inhomogeneous mixing of the tracer. Comparison of input and output
concentrations offers an additional way to determine denitrification
rates. It also allows experimental variation of parameters such as
light, concentrations of chemical species in the water, and
temperature. Long preincubation and incubation times, which may change
the microbial activity and concentration of chemical species in the sediment, are the major disadvantages of this method.
In conclusion, the 15N IPT is, in spite of its limitations,
a powerful technique for quantifying denitrification rates in aquatic systems if it is carefully applied and if the results are critically evaluated.
 |
ACKNOWLEDGMENTS |
We thank Antonin Mares and Christian Dinkel for their skilled
field and laboratory work. In particular, we are indebted to Martin
Mengis for measurements on the mass spectrometer and for suggestions
regarding the 15N IPT. We are also grateful to the
constructive comments of two anonymous reviewers.
We acknowledge a grant of EAWAG to S.M.S. and financial support from
the Swiss National Foundation for J.F. (project no. 31-54043.98).
 |
FOOTNOTES |
*
Corresponding author. Mailing address: Dipartimento del
Territorio, Divisione dell'Ambiente, Sezione Della Protezione
dell'Aria e dell'Acqua, Via Salvioni 2a, 6500 Bellinzona,
Switzerland. Phone: 41-91-814-38-35. Fax: 41 (0) 91 814 44 33. E-mail: S.Steingruber{at}ticino.com.
 |
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Applied and Environmental Microbiology, September 2001, p. 3771-3778, Vol. 67, No. 9
0099-2240/01/$04.00+0 DOI: 10.1128/AEM.67.9.3771-3778.2001
Copyright © 2001, American Society for Microbiology. All rights reserved.
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