Nong et al.
Year :
1999)
2000|
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X
a
5
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3 qag0)
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00 L
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40 60 80
Cumulative percentage of profiles (%)
ZU
10u
FIGURE 7 | Cumulative percentage of Argo profiles that reached a given
Dressure (in 50-dbar intervals from 0 to 2,000 dbar) in each year from 1999 to
2019, For example, the percentage of profiles that sampled to at least 1,600
dbar increased from onlv 10% in 1999 to 80% in 2019
early float models were only capable of profiling from shallower
pressures (1,000, 1,200, or 1,500 dbar), particularly in the tropical
oceans due to limited buoyancy generation and battery energy.
As the buoyancy issue was resolved and floats became capable
of profiling from as deep as 2,000 dbar, some floats adopted
a scheme of only sampling from 2,000 dbar every 3rd or 4th
profile (and from shallower pressures for other profiles) to save
battery energy. Float lifetimes are ultimately limited by battery
exhaustion, and many Argo floats were originally deployed
with alkaline batteries. Over time, the use of lithium batteries
became more common, and most floats now use them. Lithium
batteries have more than twice the energy density of alkalines,
hence considerably extending float lifetimes. Presently, with the
transition from alkaline to lithium batteries, and the increased
capacity of the buoyancy engines, modern Argo floats operate to
pressures of 2,000 dbar on nearly every profile. Some new models
of floats may have suflicient battery energy for 10 years of 10-day
cycling to 2,000 dbar.
In recent years, float models have been developed that are
capable of 4,000 dbar and 6,000 dbar operations over a duration
of several years (Roemmich et al., 2019). Improvements have also
been made to the accuracy and stability of the CTDs used on
these deep floats, so that they are suitable for sampling the small
temperature and salinity signals of the abyssal oceans. In 2016,
rontiers in Marine Science | www.frontiersin.or.
Argo Data 1999-2019
the first Argo profiles deeper than 2,000 dbar became available.
These technological developments have enabled the formulation
of the Deep-Argo program, which will extend Argo’s sampling
pressure ranges to full-ocean depths except over the deepest
abyssal plains and trenches.
For most profiling floats, the CTD pump is normally
switched off at around 5 dbar during ascent, in order to avoid
contamination of the conductivity cell from the ingestion of
material on the sea surface. Some floats now profile to within 2
dbar of the sea surface, as the pressure sensors have become more
accurate and thus the risk of surfacing with the CTD pump on
is much less. Several float types also continue to sample up to
the sea surface with the pump off, or carry auxiliary modules for
high-resolution near-surface sampling.
Geographical Coverage
The geographical coverage of Argo has expanded over the past
20 years largely due to the use of Iridium communications
(Figure 3). ARGOS floats deployed in the equatorial region
(5°S—5°N) tended to disperse poleward via Ekman transport
while on the sea surface. Similarly, ARGOS floats in marginal
seas or in near-coastal regions tend to have a higher probability of
grounding because their prolonged surface times expose them to
more cross-bathymetric wind transport. With their short surface
times, Iridium floats are subjected to less Ekman divergence
and wind transport, and therefore tend to disperse less in the
equatorial and near-coastal regions.
The use of Iridium has also enabled the geographical coverage
of year-round Argo data to expand to the seasonal sea ice zones
in the Southern Ocean (Wilson et al., 2019) and in the Arctic
Ocean (Smith et al., 2019). Early attempts to sample the ice-
covered polar oceans showed high instrument mortality rates,
either because of crushing between ice floes at the sea surface or
hitting the bottom of the ice packs during ascent. However, the
inclusion of a robust ice avoidance algorithm in the float software
has enabled floats to operate more successfully in the seasonal
sea ice zones without additional hardware requirements. The ice
avoidance algorithm (originally called the ice sensing algorithm,
[SA) was first developed at the Alfred Wegener Institute (AWTI)
for Polar and Marine Research, and was based on the assumption
that the likelihood of the presence of sea ice was related to the
temperature of the water column below (Klatt et al., 2007). In
practice, the algorithm computes the median temperature of the
near-surface mixed layer between depths Zi and Z, as the float
ascends. If the median temperature is less than a prescribed
threshold T,ef, the presence of sea ice is assumed, and the float will
abort its ascent to the sea surface, store the profile data onboard,
and descend to park pressure to begin its next cycle. For floats
that use the Iridium satellite system for data communication,
under-ice profiles that are collected and stored onboard the floats
during winter are transmitted when surface conditions become
ice-free during early summer (Riser et al., 2018).
The ice avoidance algorithm was first implemented by AWI on
floats in the Weddell Sea in 2002 (Klatt et al., 2007). The first AWI
algorithm set Zı = 50 m, Z2 = 20 m, and T,ef = —1.79°C. In 2007,
the University of Washington began deploying floats around
the Antarctic continent with a version of the AWI algorithm
Qanteambear 2020 1 Valııme 7 | Article Z01