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TRANSCRIPT
Aerosol isotopic ammonium signatures over the remote Atlantic Ocean
C.T. Lin*, T.D. Jickells, A.R. Baker, A. Marca and M.T. Johnson
Centre for Ocean and Atmospheric Sciences
School of Environmental Sciences
University of East Anglia,
Norwich Research Park, Norwich, NR4 7TJ, UK
* Corresponding author
Now at
Greenhouse Gas Reduction Management Office,
Environmental Protection Administration,
Executive Yuan, Taiwan (R.O.C.)
Abstract
We report aerosol ammonium 15N signatures for samples collected from research cruises on the South Atlantic and Caribbean using a new high sensitivity method. We confirm a pattern of isotopic signals from generally light (δ15N -5 to -10‰), for aerosols with very low (<2nmol m-3) ammonium concentrations from the remote high latitude ocean, to generally heavier values (δ15N +5 to +10‰), for aerosols collected in temperate and tropical latitudes and with higher ammonium concentrations (>2nmol m-3). We discuss whether this reflects a mixing of aerosols from two end-members (polluted continental and remote marine emissions), or isotopic fractionation during aerosol transport.
Keywords
Atlantic Ocean, Ammonium aerosol, 15N
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Introduction
The cycling of ammonia through the atmosphere represents a major component of the global nitrogen
cycle (e.g. Fowler et al., 2013, Gruber and Galloway, 2008). The cycle involves both gaseous
ammonia and aerosol ammonium, neither of which are oxidised in the atmosphere on the time scales
of a few days, and can therefore be transported through the atmosphere and deposited over the oceans.
In remote ocean regions, atmospheric nitrogen deposition represents an important nutrient source
which can increase marine productivity (Duce et al., 2008). However, the net significance of the
atmospheric ammonia/ammonium contribution to this deposition flux depends critically on whether
the ammonia/ammonium source is predominantly terrestrial, and hence a new source of nitrogen to
the marine environment, or from ammonia emissions from seawater that are being recycled and hence
will not result in a net increase in ocean productivity. A net marine ammonia emission source to the
atmosphere has been proposed (e.g. Voss et al., 2013 and refereces therein, Fowler et al., 2013)
although it has been argued that the net direction of this flux may have been reversed in the industrial
period so that it now flows from land to sea as a result of the increases in atmospheric ammonia
emissions from human activity (Galloway et al., 1995). New comparisons of model and field data lead
to a rather lower estimate of the global marine emission than previously suggested (Paulot et al.,
2015). A recent study has suggested that the ocean ammonia emissions can be the dominant source of
ammonium in rainfall on Bermuda, despite this being a region downwind of major terrestrial
anthropogenic sources in North America (Altieri et al., 2014). However, another recent study has
suggested that terrestrial ammonia emissions are the main source for ammonium in rainwater on
Bermuda (Keene et al., 2014). Hence there is still considerable uncertainty over even the direction,
leave alone the magnitude of the air-sea ammonia flux.
Due to the strong temperature dependence of ammonia solubility, it has been argued that marine
ammonia emissions to the atmosphere are likely to be more important from warmer rather than cold
ocean waters, with net emissions at high latitude from the ocean to the atmosphere difficult to achieve
at the low water temperatures, under typical surface ocean and marine atmosphere conditions
(Johnson et al., 2008, Paulot et al., 2015). Gas phase ammonia measurements from the remote marine
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atmosphere boundary layer would be useful for understanding the marine ammonia cycle. However,
such gas phase ammonia concentrations are very poorly constrained, with few measurements, mostly
with high uncertainties (Paulot et al., 2015). However, high sensitivity measurements suggest that gas
phase ammonia and aerosol phase ammonium concentrations may be of similar magnitude to each
other over the open ocean (Norman and Leck, 2005). Ammonia emissions from seawater can react
rapidly in the marine atmosphere to form ammonium aerosols in the presence of acidic species. Given
the rapid removal of any free nitric acid by reaction with sea-salt in the marine atmosphere (Baker et
al., 2006, Andreae and Crutzen, 1997), the most likely salts to be formed by marine ammonia
emissions are with sulphuric acid. We have previously assumed that these salts would not
disproportionate into gas phase components (Jickells et al., 2003, Paulot et al., 2015) and hence will
not isotopically fractionate once in the aerosol phase. Indeed for dry ammonium sulphate and
ammonium bisulphate salts, the partial pressure of ammonia is very low. However, these salts will
attract water potentially allowing a pH dependent bidirectional exchange of ammonia between aerosol
and gas phases at high humidity in the marine boundary (Johnson et al., 2008, Quinn et al., 1992),
consistent with limited field and laboratory data (Harrison and Kitto, 1992, Scott and Cattell, 1979).
Johnson and Bell (2008) derive the following relationship from the Aerosol Inorganics Model (Clegg
et al., 1998) at high relative humidity appropriate for the marine boundary layer:
pNH3 = 0.00016 e^(0.124T + 4.6R)
where pNH3 is the partial pressure of ammonia over the aerosol in nmol/m3, T is the temperature in
Celsius and R is the molar NH4:nss-SO4 (nss – non-sea-salt sulphate) ratio in the aerosol. This
equation predicts pNH3 comparable to or greater than typically observed marine boundary layer
ammonia concentrations at NH4:nss-SO4 ratios above ~1.2, and such ratios occur at least in parts of
the Atlantic Ocean marine boundary layer (Norman and Leck, 2005). Thus ammonia-ammonium
partitioning in the marine atmosphere is likely to be very dependent on aerosol pH (Johnson and Bell,
2008), which is also not particularly well known (Pszenny et al., 2004, Kerkweg et al., 2008).
The magnitude of marine ammonia emissions and their significance for ocean productivity is
therefore still rather uncertain and requires further study, particularly given the scale and significance
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of the human perturbation of the global nitrogen cycle. Isotopic measurements have the potential to
provide additional insight into the marine atmosphere ammonia cycle, and indeed the basis of the
arguments for a major marine ammonia emission source dominating ammonium deposition over the
North Atlantic (Altieri et al., 2014) are predominantly isotopic measurements. In the latter paper
evidence from an earlier study by us of the aerosol ammonium isotopic composition in the remote
marine atmosphere (Jickells et al., 2003) was used to help make the case in support of a marine
source. However, while there have been several studies describing the isotopic signature of ammonia
emissions and the abundance of ammonia/ammonium in rain, aerosol and the gas phase in relatively
polluted areas (Yeatman et al., 2001, David Felix et al., 2013, Fukuzaki and Hayasaka, 2009, Xiao et
al., 2015) there have been less studies in remote areas. In our earlier study (Jickells et al., 2003) we
reported a systematic decrease in the isotopic ammonium signature with decreasing ammonium
concentration which was interpreted as resulting from two end-member mixing of isotopically light
marine emissions of ammonia with isotopically heavy terrestrial ammonia emissions. However, the
nitrogen content of samples from the remote marine atmosphere approached our detection limit for
isotopic analysis in that earlier study, and it is possible that some of the trends in isotopic composition
with concentration reported could reflect uncertainties around detection limits.
We now report here analyses of aerosols collected along the Atlantic Meridional Transect AMT
(Robinson et al., 2006) between the UK and Southern Ocean for ammonium ion isotopic composition
using an improved method with greatly enhanced sensitivity. This allows us to test the validity of the
trends seen in our previous study. The analysis of additional aerosol samples from the Caribbean is
also reported and used to further consider the validity of the two end-member mixing model, between
high concentration and isotopically heavy ammonia from strong terrestrial emission sources regions
and a background low concentration marine emission of isotopically light ammonia.
Methods
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Aerosol data reported here are based on samples collected on two cruises AMT15, sampling from
approximately 10oN to 40oS in the Atlantic, and JC18 (Figure 1). Our aerosol sampling and
contamination control methods, as well as our procedures for calculating air-mass back trajectories,
have been described in detail in previous publications (Jickells et al., 2003, Baker et al., 2010), and
are therefore only briefly summarised here. Aerosol samples were collected by high volume aerosol
sampling with a Sierra Type cascade impactor and the results presented here are for fine mode aerosol
(<1µm diameter aerosol and where most of ammonium is found Baker et al., 2006) collected on
Whatman 41 filter. Sample filters were subsequently frozen for return to our home laboratory. Filters
were later thawed, major ions water extracted from a fraction of the filter and this extract
subsequently analysed by ion chromatography (anions and ammonium) and ICP-OES (for the other
cations). The ammonium isotopic composition was measured on the water extract of a separate
fraction of the aerosol filter using essentially the same method as Altieri et al. (2014), although
independently developed and described in detail elsewhere (Lin, 2010) 1. This method is much more
sensitive than the method used in our previous study. The method is based on chemical conversion of
ammonium to nitrite and then to N2O which is then cryogenically pre-concentrated and analysed by
isotope-ratio mass spectrometry on a Europa GEO 20-20 (McIlvin and Altabet, 2005, Zhang et al.,
2007, Altieri et al., 2014). The isotope ratios are calibrated against standard reference materials IAEA
N1 and USGS 25 and 26 as well as an internal laboratory N2O gas standard. Results are expressed
here in the standard δ15N notation. The method can successfully measure isotopic ratios on as little as
10nmol of ammonium. Blanks of chemicals and sample preparation yield a beam area of only 10% or
less of samples and are corrected for in the data reported here. The average precision based on
replicate analyses of the standards is +0.2‰ or better.
Results
Figure 2a shows the results for AMT15 samples with the aerosol ammonium δ15N isotopic
composition values plotted against the ammonium concentration. Ammonium concentrations show a
1 https://ueaeprints.uea.ac.uk/19108/1/2010LinCTPhD.pdf
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strong gradient of concentrations with low values at high latitudes consistent with the trend reported
by Norman and Leck (2005). Since ammonia can have both marine and terrestrial sources, it is not an
unambiguous tracer of terrestrial sources, but since the emissions on land are so much larger than
those from the oceans, the gradient in aerosol ammonium is consistent with the mixing of low
concentration ammonium aerosol from remote region air masses with high concentration terrestrial
sources. Nitrate concentrations are an alternative unambiguous tracer of terrestrial emissions. Total
aerosol ammonium and nitrate are well correlated with an essentially zero intercept along the AMT
transect, despite the different aerosol size distributions of nitrate and ammonium due to the reaction of
nitric acid with seasalt (Baker et al., 2006) and this correlation is also seen in the this data set (results
not shown here but available in Lin, 2010). In Figure 2a most of the samples have ammonium δ15N in
the range 0 to +6 ‰ (and occasionally higher), but there are a group of samples with low ammonium
ion concentrations (<2nmolm-3) and much lower ammonium δ15N values (-4 to -6‰). All these latter
samples are from samples collected in air flowing from the remote South Atlantic which had not been
over land masses for the 5 days before sampling (all trajectories available in Lin, 2010 and data are
classified by trajectory in Figure 2c). These air-parcel back-trajectories describe only where the air
sampled has been over the last 5 days and do not preclude a continental source affecting the air prior
to this time. In addition similar air masses may contain very different concentrations due to variations
in precipitation along the trajectory. However, despite these caveats such trajectories have proven a
valuable tool for interpreting data from the Atlantic in many previous studies (Baker et al., 2006). The
overall pattern in Figure 2a is essentially the same as reported previously using a less sensitive δ15N
method (Jickells et al., 2003) from a different AMT cruise 3 years previously. The positive δ15N
values in Figure 2a are all for samples collected in the tropical South Atlantic with 5 day air parcel
back trajectories crossing tropical ocean waters and in most cases approaching, but not reaching, the
African continent, except for one sample where trajectories approached the South American
continent. This latter sample had a very low ammonium concentration but relatively heavy isotopic
signature (0.5nmol m-3 and δ15N +6.2‰).
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In Figure 2b we report a similar plot of the data from the JC18 cruise in the Caribbean which
encountered air with relatively low ammonium concentrations, and in which we find broadly similar
δ15N values to those seen on AMT15. However, there are two samples that have low δ15N values
despite having relatively higher ammonium concentrations and two samples with low ammonium
concentrations which have particularly heavy δ15N signatures. In the case of one of these samples with
higher δ15N values, the air sampled had relatively recently crossed Guadeloupe. All samples collected
on this cruise were sampling air that may have passed relatively close to a number of Caribbean
islands, although the ammonium and other major ion concentrations suggest little enhancement over
background concentrations from anthropogenic or volcanic sources for any of the JC18 samples.
We therefore conclude that the pattern (Figure 2a & b) of high δ15N ammonium in aerosols which
have relatively high ammonium concentrations due to a stronger influence from terrestrial sources
over the tropical Atlantic, and low δ15N for low concentration ammonium aerosols sampled over the
Southern Ocean reported previously (Jickells et al., 2003) is reproduced in this new data set collected
separately and analysed by the new more sensitive method. The new data from the Caribbean are
broadly consistent with this pattern, although they include some low aerosol ammonium concentration
samples which have heavier isotopic signatures.
In Figure 2c we combine all of the new data with that reported by Jickells et al. (2003) and classify
the samples by trajectory to emphasise the similar overall pattern in both data sets. Thus we suggest
the pattern reported is likely to be real and not an analytical artefact associated with the limited
sensitivity of the methods used for isotopic analysis in the earlier study. This figure illustrates that the
isotopically light samples are all associated with low ammonium concentrations and South American,
Southern Ocean or Caribbean trajectories. Such isotopically light signatures have also been reported
in air masses with low ammonium concentrations crossing the remote high latitude North Atlantic
(Jickells et al., 2003). Heavy isotopic signatures are seen for high ammonium concentration samples
from both hemispheres. There are also some low ammonium concentration aerosol samples that have
heavier signatures. Hence there is no simple linear relationship between isotopic composition and
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concentration, but the low δ15N ammonium in aerosols appear to be characteristic of high latitude
systems with low ammonium concentrations.
We have previously argued that fine mode aerosol is likely to be acidic and hence to retain
ammonium aerosol (and any gaseous ammonia) effectively as ammonium sulphate (Jickells et al.,
2003, Paulot et al., 2015) as discussed earlier, and hence that the pattern in Figure 2 is unlikely to be a
sampling effect associated with dissociation of aerosol ammonium salts. We also previously
suggested that the low ammonium δ15N values in air over the remote Southern Ocean and North
Atlantic may represent the isotopic signature of marine emissions which would be more readily
detectable in air in this remote region which is less impacted by terrestrial emissions. Hence we
suggested that the pattern in Figure 2 can be interpreted to represent a two end-member mixing series
between high concentration and isotopically heavy terrestrial ammonia sources (consistent with other
published data for terrestrial ammonia/ammonium Altieri et al., 2014, Jickells et al., 2003, Rolff et al.,
2008, Xie et al., 2008, Yeatman et al., 2001) and low concentration isotopically light marine ammonia
emissions (David Felix et al., 2013). However, it has been argued that at low surface-ocean
temperatures there should be little or no emission of ammonia from the oceans (Johnson et al., 2008),
challenging the idea that the light ammonium isotopic signature could be derived from marine
ammonia emissions from high latitude waters. We now use the additional data from the JC18 and
AMT15 cruises to consider this issue further.
The samples collected on JC18 provided the opportunity to sample air with low ammonium aerosol
concentrations with apparently little influence from local terrestrial emissions and underlain by warm
ocean waters from which emission of ammonia is thermodynamically more favourable. We find a
similar range of δ15N values to those sampled on AMT15 (Figure 2), and the values are also broadly
similar to those reported for Bermuda rainwater of -5.5+2.9‰ (Altieri et al., 2014), although aerosol
and rainwater may not be directly comparable if there is isotopic fractionation during rainwater
scavenging.
The results presented here for both cruises do approximate to the two end-member mixing model
described, but this does not readily explain the heavier isotopic signatures at low ammonium
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concentrations. However, the Henry’s Law for ammonia suggests that marine ammonia emissions
should have a greater impact in low atmospheric ammonia/ammonium marine atmosphere overlying
warm waters, and yet the data from JC18 cruise (Figure 2b) include samples with similar light
isotopic signatures to those seen in samples collected in air arriving from the Southern Ocean. An
alternative explanation may be that the trends in the isotopic signature of ammonium seen along the
AMT transect (Figure 2a&c) indicate isotopic fractionation of aerosol ammonium during long-range
transport resulting in light δ15N signature in the very remote atmosphere overlying the Southern
Ocean.
We can therefore envisage two possible scenarios to explain the observation of isotopically light
ammonium in air of marine origin:
1. Firstly as has been previously postulated that an isotopically light signal represents ammonia
emitted from the ocean to the atmosphere, during which we would expect strong fractionation
compared to marine ammonium favouring emission of the isotopically light form of ammonia
(Jickells et al., 2003, David Felix et al., 2013).
2. The second option is that terrestrial ammonium transported over the ocean at high relative
humidity are able to equilibrate with gas phase ammonia from marine or terrestrial sources
and that this can lead to isotopic fractionation either directly, or via the selective loss of
isotopically heavier aerosol or ammonia gas during long range transport. Substantial
fractionations have been reported between ammonia and ammonium on land (Xiao et al.,
2015, Fukuzaki and Hayasaka, 2009) although in these cases ammonium nitrate is likely to be
present which is more able to dissociate than ammonium sulphate (Paulot et al., 2015). Such
simple dilution and loss of terrestrial ammonia emissions during long range transport with
little substantial impact from marine ammonia emissions is consistent with the strong
correlations between ammonium and nitrate with an intercept close to the origin for aerosol
samples collected along the AMT transect (Baker et al., 2006) discussed earlier.
As outlined in Johnson and Bell (2008), in a situation where ammonia can exchange between the gas
and aerosol phases there is a direct connection through a series of thermodynamic equilibria between
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ammonium in the ocean surface and ammonia in the gas phase. This implies that any net acidity
transported in the aerosol over the ocean will tend to take up ammonia from the atmosphere and
consequently lead to an ammonia emission from the ocean to compensate; the logical conclusion of
which being that ammonia (and at least some of the ammonium) in the remote marine environment
will be of marine origin, although this in itself does not mean that this marine ammonia will be
isotopically distinguishable from terrestrial sources. Norman and Leck (2005) have estimated the
residence time of ammonia in the marine boundary layer to be only a few hours requiring either a
marine ammonia source or rapid aerosol/gas exchange, or both, to sustain the observed gaseous
marine concentrations in the remote marine atmosphere.
How then can the field observations of Johnson et al 2008, predicting an air to sea flux of ammonia
predominantly at lower latitudes be reconciled with the isotopic evidence here and in Jickells (2003),
which implies a marine ammonia source at temperate high latitudes? Johnson et al (2007) report
observations of high ammonium concentrations in the surface ocean following a phytoplankton bloom
that could drive an ammonia flux out of the ocean even in the relatively cold waters of the Northeast
Atlantic. Hence a seasonal bias in the observations here and in the earlier paper could resolve the
inconsistency. Alternatively, if the major control on atmospheric ammonia concentration is the pH of
the aerosol phase, then this suggests that atmosphere and ocean should tend to being close to
equilibrium, with a small net flux out of the ocean and into the aerosol phase as net acidity is added
from e.g. sulfate produced by DMS emissions (Johnson and Bell, 2008, Lin et al., 2012, Paulot et al.,
2015). This is not necessarily inconsistent with the observations of Johnson et al (2008), as the
uncertainties on gas phase ammonia concentrations can be considerable, as noted earlier.
In conclusion therefore, our results demonstrate a clear geographical range of aerosol ammonium
isotopic signatures. While this can be explained in part by mixing of an isotopically light marine
ammonium source with an isotopically heavier terrestrial source, this requires that a substantial part of
the marine ammonia emission takes place at high latitudes, where thermodynamics predict that this
emission would be smallest. There are mechanisms that can rationalise this dilemma, such as
emissions during strong algal blooms, and we therefore urge more studies of marine ammonia
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emissions. An alternative explanation for the isotopically light ammonium aerosol signature is that it
arises from fractionation during long range transport, and we therefore also suggest that further
studies of ammonium aerosol cycling and associated isotopic fractionation would be valuable,
although this will not be simple to investigate over long transport times at low concentrations.
The resolution of the causes of the isotopic signatures we see will then open the way for more
effective use of ammonium aerosol isotopic signatures to study ammonium cycling and resolve the
major uncertainty over the significance of marine ammonia emissions.
Acknowledgements
We gratefully acknowledge the NOAA Air Resources Laboratory for the provision of the HYSPLIT
transport and dispersion model and ready website (http://www.arl.noaa.gov/ready.html) used in this
publication. We thank Jenni Barclay and her colleagues for the opportunity to sample on JC18
supported by NERC grant NE/B50461411.We acknowledge the support of the AMT programme for
sampling opportunities and for funding via NERC grant NER/O/S/2001/00680 and thank three
anonymous referees for their constructive and valuable comments on earlier versions of this
manuscript.
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Figure 1a. Cruise track for AMT15 (17 Sept to 29 Oct 2004) large circles and solid line. Air flow was
from the east until approximately 5oN and then further south from the west based on air-mass back
trajectories which are available in full elsewhere (Lin, 2010). The cruise track for the cruise used for
samples for Jickells et al (2003) sampling is shown as dotted line.
Figure 1b. Sampling stations on JC18, 4-14 Dec 2007. The ship was stationary and head to wind at the
various sampling stations with air flow for essentially all the cruise from the NE except sample 9 from
the SW. Clarify what the yellow and blue lines are
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0.0 2.0 4.0 6.0 8.0 10.0 12.0
-15.0
-10.0
-5.0
0.0
5.0
10.0
Aersol Ammonium Concentration nmolm-3
δ15N
Aer
sol A
mm
oniu
m ‰
Figure 2a Aerosol ammonium isotopic composition plotted against aerosol ammonium concentrations
for AMT15
1.0 2.0 3.0 4.0 5.0 6.0 7.0 8.0 9.0 10.0
-10.0
-5.0
0.0
5.0
10.0
15.0
Aerosol Ammonium Concentration nmol m-3
δ15N
Aer
osol
Am
mon
ium
‰
Figure 2b Aerosol ammonium isotopic composition plotted against aerosol ammonium concentrations
for JC18
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0 5 10 15 20 25 30 35
-15
-10
-5
0
5
10
15
20
δ15N vs. Atmospheric NH4 (by trajectory)
US/EUSaharaAfricaSouth AmericaRemote OceanJC18
Atmospheric NH4 (nmol/m3)
δ15
N (‰
)
Figure 2c Aerosol ammonium data from Figures 2a and 2b plus data previously reported for aerosol
data collected over the Atlantic(Jickells et al., 2003) with samples coded based on the air parcel
trajectory.
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