ArticlePDF Available

Did the opening of the Drake Passage play a significant role in Cenozoic cooling?

Authors:

Abstract and Figures

Following the Early Eocene climatic optimum (~55-50 Ma), climate deteriorated and gradually changed the earth from a greenhouse into an icehouse. It is widely believed that the opening of the Drake Passage had a marked impact on the cooling. Here, we infer from climate model simulations that the early opening of the Drake Passage played only a limited role, while the later constriction of the Tethys and Central American Seaways is more important in explaining the observed Cenozoic cooling. Based upon an Early Eocene model simulation, we study the sensitivity of the climate to major tectonic events such as the closing of the West Siberian Seaway, the deepening of the Arctic-Atlantic Seaway, the opening of the Drake Passage, and the constriction of the Tethys and Central American seaways. The opening of the Drake Passage weakens the Southern Ocean Deep Water (SODW) dominated ocean circulation and cools the earth weakly. It might have been a cause for the symmetrical cooling in the Early Cenozoic, together with the closing of the West Siberian Seaway, and the deepening of the Arctic-Atlantic Seaway. However, the constriction of the tropical seaways causes the development of ocean circulation dominated by North Atlantic Deep Water (NADW). The transition of ocean circulation from SODW-dominated to NADW-dominated mode results in significant cooling in the South Hemisphere. In particular, the closing of the Tethys Seaway appears to be key in the transition.
Content may be subject to copyright.
ATMOSPHERIC AND OCEANIC SCIENCE LETTERS, 2010, VOL. 3, NO. 5, 288292
Has the Drake Passage Played an Essential Role in the Cenozoic Cooling?
ZHANG Zhong-Shi
1,2
, YAN Qing
2
, and WANG Hui-Jun
2
1
Bjerknes Centre for Climate Research, UniResearch, Bergen N-5007, Norway
2
Nansen-Zhu International Research Center, Institute of Atmospheric Physics, Chinese Academy of Sciences, Beijing 100029, China
Received 29 August 2010; revised 12 September 2010; accepted 12 September 2010; published 16 September 2010
Abstract The Drake Passage is the seaway between
South America and Antarctica. It is widely believed that
the thermal isolation effects caused by the opening of the
Drake Passage played an important role in the abrupt
cooling that occurred at the Eocene-Oligocene boundary
in the Cenozoic. These effects are also thought to be in-
dependent of the geometry of the passage. Here, the au-
thors demonstrate that the climate impacts of the Drake
Passage depend on the passage geometry by comparing
the climate’s sensitivity to the opening of the Drake Pas-
sage under the present and the Early Eocene land-sea
configurations. These experiments show that the thermal
isolation effects caused by the passage are much stronger
under the present land-sea configuration. In comparison,
under the Early Eocene land-sea configuration, the weak
anomalies in heat transport caused by the opening of the
narrow and shallow Drake Passage are not strong enough
to thermally insulate Antarctica. The climate effects of the
Drake Passage on the Cenozoic cooling have been over-
estimated in previous sensitivity studies carried out using
the present land-sea configuration. Thus, it is unlikely that
the opening of the Drake Passage played an essential role
in the abrupt Cenozoic cooling, especially in the abrupt
cooling at the Eocene-Oligocene boundary.
Keywords: Drake Passage, land-sea configuration, Ce-
nozoic cooling
Citation:
Zhang, Z.-S., Q. Yan, and H.-J. Wang, 2010:
Has the Drake Passage played an essential role in the Ce-
nozoic Cooling? Atmos. Oceanic Sci. Lett., 3, 288–292.
1 Introduction
The Drake Passage is the seaway between the southern
tip of South America at Cape Horn, Chile, and the South
Shetland Islands of Antarctica. At present, the passage is
more than 800 km wide and greater than 4000 m deep.
About 60 million years (Ma) ago, the Drake Passage
had not yet opened, and South America was still con-
nected with Antarctica. The Drake Passage opened later
and gradually expanded in the Cenozoic. There is evi-
dence indicating an early shallow opening in the Early
Eocene (Livermore et al., 2005) and subsequent deepen-
ing at ~ 41 Ma in the Middle Eocene (Scher and Martin,
2006). However, the age estimates for the opening of the
Drake Passage are still under debate (Barker, 2001).
The opening of the Drake Passage is thought to have
been essentially important in the Cenozoic cooling. In the
Cenozoic, the Early Eocene (~50 Ma) was an extremely
Corresponding author: ZHANG Zhong-Shi, zhongshi.zhang@uni.no
warm period (Zachos et al., 2001). The temperature in the
deep ocean was above 10C (Lear et al., 2000). The level
of warmth in the Arctic is thought to have been similar to
that in today’s subtropical region (Sluijs et al., 2006).
Later, the earth gradually developed from a greenhouse to
an icehouse climate, with abrupt cooling and Antarctic
glaciation occurring at the Eocene-Oligocene boundary
(~34 Ma, Zachos et al., 2001). The opening of the Drake
Passage has been suggested to have enabled the develop-
ment of the Antarctic Circumpolar Current (ACC), which
thermally insulated Antarctica through reduced southward
heat transport (Toggweiler and Bjornsson, 2000) and
caused significant cooling over Antarctica at the Eo-
cene-Oligocene boundary (Kennett, 1977). The thermal
isolation effects of the opening of the Drake Passage have
been analyzed by many modeling studies based on the
present land-sea configuration (e.g., Nong et al., 2000;
Sijp and England, 2004). These effects have also been
thought to be independent of the geometry of the Drake
Passage (Toggweiler and Bjornsson, 2000).
However, the role of the Drake Passage has been chal-
lenged by an increasing number of studies. Geological
studies (Livermore et al., 2005; Scher and Martin, 2006)
indicate that the opening of the Drake Passage might have
occurred much earlier than the Eocene-Oligocene bound-
ary. A modeling study has shown that the ACC becomes
sluggish with a narrow and shallow Drake Passage in the
Eocene land-sea configuration (Huber and Sloan, 2001).
The reduction in ocean heat transport caused by the open-
ing of the Drake Passage has been suggested to have had
a smaller effect than that expected from decreasing levels
of atmospheric CO
2
in the transition from the greenhouse
to the icehouse climate (DeConto and Pollard, 2003;
Huber and Nof, 2006). The tropical seaways may have
also played a more important role than the Drake Passage
in understanding the abrupt cooling events of the Ceno-
zoic (Zhang et al., 2009).
It is obvious that the above modeling studies, carried
out with different land-sea configurations, show varying
degrees of importance for the opening of the Drake Pas-
sage, which brings uncertainty to the above debate. In this
study, using the climate model FOAM (the Fast Ocean
Atmosphere Model), we compared the climate’s sensitivity
to the opening of the Drake Passage under two land-sea
configurations. One is the present land-sea configuration,
and the other is the Early Eocene land-sea configuration.
2 Model and experiment design
Version 1.5 of FOAM is a fully coupled General Cir-
NO. 5 ZHANG ET AL.: WAS THE DRAKE PASSAGE IMPORTANT TO THE CENOZOIC COOLING? 289
culation Model (GCM) run without flux corrections
(Jacob et al., 2001). The atmospheric component in
FOAM is run with a horizontal resolution of R15 (4.5 ×
7.5 degrees) and 18 vertical levels. The ocean component
is a finite-difference z-coordinate ocean model with a
horizontal resolution of 1.4 × 2.8 degrees, 24 vertical lev-
els, and a free surface. This version of FOAM provides a
good simulation of the mean and variability of the modern
climate (e.g., Liu et al., 2000). It also has been widely
used in paleoclimate studies (e.g., Donnadieu et al., 2006;
Zhang et al., 2009).
We designed two groups of experiments. The first
group was based on the present land-sea configuration
and bathymetry condition, but with (experiment PRE,
present) or without (experiment PRENDP, present without
the Drake Passage) the Drake Passage open. The Drake
Passage was about 1400 km wide (ten model grids) with a
maximum depth of 3000 m in experiment PRE. The sec-
ond group was based on the Early Eocene land-sea con-
figuration and bathymetry condition established by Zhang
et al. (2009), again with the Drake Passage open (experi-
ment EOC, Eocene) or closed (experiment EOCNDP,
Eocene without the Drake Passage). The Drake Passage
was about 700 km wide (five model grids) with a maxi-
mum depth of about 150 m in experiment EOC.
In these four experiments, the solar constant and orbital
parameters were set to present conditions. The vegetation
on land was prescribed as shrubland/grassland. The con-
centration of atmospheric CO
2
was set to eight times the
pre-industrial level, following estimates for the Early Eo-
cene (Royer, 2006).
Experiments PRE and EOC were spun up for 1500
years from the same preset initial conditions. Then, these
two experiments were continued for 500 years. Starting
from the end of the 1500-year spin ups of experiments
PRE and EOC, respectively, experiments PRENDP and
EOCNDP were carried out for 500 years. All of the results
reported here are the averages of the last 100 years of
each experiment.
3 Climate sensitivities
The model, FOAM, simulated a reasonable strength for
the ACC. For the present climate with atmospheric CO
2
level set at 350 ppmv, the simulated strength of the ACC
was about 160 Sv. In experiment PRE, with the atmos-
pheric CO
2
level set at 2240 ppmv, the strength of the
ACC was about 25 Sv. The weak ACC in experiment PRE
resulted from the extremely warm conditions, with deep
ocean temperatures above 10C in the experiment. After
the Drake Passage was opened under the present land-sea
configuration, the ACC occurred around Antarctica in
experiment PRE (Fig. 1a). In comparison, the strength of
the ACC was significantly weaker, about 4 Sv, in experi-
ment EOC. No clear development of the ACC was ob-
served with the opening of the Drake Passage in experi-
ment EOC (Fig. 1b).
With the development of the ACC, thermal isolation
effects were observed in experiment PRE. Significant
cooling occurred at the surface of the South Atlantic and
the Southern Ocean after the Drake Passage was opened
in experiment PRE (Fig. 2a). Although the cooling around
Western Antarctica was stronger, almost the whole South-
ern Ocean and Antarctica were cooled. The mean SST
decreased by about 1.5C at the surface of the Southern
Ocean. The SST changes in the Southern Ocean were
similar to those in the simulations carried out by Sijp and
England (2004). Warming appeared in the Northern
Hemisphere. This pattern of SST change, with strong
cooling in the Southern Hemisphere but warming in the
Northern Hemisphere, agrees well with earlier studies
(e.g., Nong et al., 2000; Sijp and England, 2004).
However, the cooling effect caused by the opening of
the Drake Passage was significantly weaker under the
Figure 1 ACC anomalies (cm s
–1
) after the Drake Passage was opened under (a) the present and (b) the Early Eocene land-sea configurations. Ar-
rows show current directions for current speeds larger than 0.5 cm s
–1
. The color scale shows current speeds. Areas with current speeds larger than 1
cm s
–1
are shaded.
290 ATMOSPHERIC AND OCEANIC SCIENCE LETTERS VOL. 3
Figure 2 SST (C) and SSS (psu) anomalies after the Drake Passage was opened. (a) SST anomalies and (b) SSS anomalies under the present
land-sea configuration; (c) SST anomalies and (d) SSS anomalies under the Early Eocene land-sea configuration; Comparison of zonal mean (e) SST
anomalies and (f) SSS anomalies in the Atlantic, respectively. Only SST or SSS changes with confidence levels greater than 95% are illustrated.
Early Eocene land-sea configuration (Fig. 2c). Only small
changes of SST were observed at the surface of the Atlan-
tic and the global ocean. A cooling center occurred in the
South Atlantic in experiment EOC. However, SST de-
creased by only about 0.1–0.4C in the cooling center.
The response of sea surface salinity (SSS) to the open-
ing of the Drake Passage was also larger under the present
land-sea configuration than under the Early Eocene
land-sea configuration (Figs. 2b and 2d). After the Drake
Passage was opened in experiment PRE, SSS decreased
by 3–4 psu in the South Atlantic. In comparison, SSS de-
creased by only 0.3–0.5 psu in the South Atlantic in ex-
periment EOC.
The opening of the Drake Passage results in more heat
transport from the Southern Hemisphere to the Northern
Hemisphere in the models. The modification of heat
transport can be clearly observed, especially in the Atlan-
tic basin (Fig. 3). However, the modification caused by
the opening of the Drake Passage is much stronger under
the present land-sea configuration than under the Early
Eocene land-sea configuration (Figs. 3e and 3f). As a re-
sult, significant SST anomalies occur after the Drake
Passage is opened in experiment PRE, but weak SST
anomalies occur in experiment EOC.
4 Implications for the Cenozoic cooling
It should be noted that FOAM might have underesti-
mated the strength of the ACC in experiment PRE and
experiment EOC, although the extremely warm condi-
tions are one of the reasons for the sluggish simulation of
the ACC. These simulations of the ACC need to be re-
peated using other models. However, the above simula-
tions demonstrate that the development of the ACC de-
pends on the geometry of the Drake Passage. The strength
of the ACC is about five times larger in experiment PRE
under the present land-sea configuration than in experi-
ment EOC under the Early Eocene land-sea configuration.
The thermal isolation effects caused by the opening of
the Drake Passage also depend on the passage geometry
associated with the land-sea configuration. These results
do not support the early study carried out with a highly
idealized model (Toggweiler and Bjornsson, 2000), which
showed that the channel geometry of the Drake Passage
was relatively unimportant to its climate effects. It should
be noted that this earlier study used a highly idealized
bathymetry, a “water planet” with two islands located at
the two poles and one land barrier connecting the two
islands. With this idealized bathymetry, the importance of
NO. 5 ZHANG ET AL.: WAS THE DRAKE PASSAGE IMPORTANT TO THE CENOZOIC COOLING? 291
Figure 3 Heat transports (PW) examined in the experiments. Heat transport in the global ocean basin under (a) the present land-sea configuration
and (c) the Early Eocene land-sea configuration; Heat transport in the Atlantic Ocean Basin under (b) the present land-sea configuration and (d) the
Early Eocene land-sea configuration; Comparison of (e) global heat transport anomalies and (f) Atlantic heat transport anomalies after the Drake
Passage was opened under the two land-sea configurations, respectively. Heat transport was calculated by integrating the meridional velocity and
temperature.
the land-sea configuration and bathymetry was com-
pletely ignored. Hence, the salinity response to the open-
ing of the Drake Passage was overestimated. The salinity
response is highly related to fresh water input associated
with the land-sea configuration and bathymetry conditions.
As our simulations demonstrate, only weak SSS anoma-
lies occur after the Drake Passage is opened under the
Early Eocene land-sea configuration (Fig. 2d). These
weak changes in salinity could not have caused a large
reorganization of ocean circulation resulting in a climate
response.
In the earlier sensitivity experiments (e.g., Nong et al.,
2000; Sijp and England, 2004), the cooling effect of the
Drake Passage on the Cenozoic cooling was overesti-
mated because they were carried out with the present to-
pography and bathymetry conditions. It is likely that the
Drake Passage opened in the Early Eocene (Livermore et
al., 2005), and it might have reached a depth of 1000 m in
the Middle Eocene (Scher and Martin, 2006). Therefore,
the opening was much earlier than the abrupt cooling
event at the Eocene-Oligocene boundary, about 34 Ma.
Although the age estimates for the opening of the Drake
Passage are still under debate (Barker, 2001), there is no
doubt that the Drake Passage was narrow and shallow
following its initial opening. As the present study demon-
strates, a narrow opening of the Drake Passage could not
have caused strong cooling, even if the opening happened
at the Eocene-Oligocene boundary. Thus, it is unlikely
that the thermal isolation effects caused by the opening of
the Drake Passage played an important role in the dete-
rioration from a greenhouse to icehouse climate in the
Cenozoic. There must be other more important factors
that contributed to the abrupt cooling and Antarctic glaci-
ation at the Eocene-Oligocene boundary.
However, the impact of the expansion of the Drake
Passage on the long-term Cenozoic cooling trend should
not be neglected, although the model simulations pre-
sented here and the recent studies of DeConto and Pollard
(2003), Huber et al. (2004), Huber and Nof (2006), and
Zhang et al. (2009) indicate that the Drake Passage plays
a minor role in cooling the Antarctic continent. With the
gradual expansion and deepening of the Drake Passage,
the increased strength of the ACC could be expected to
contribute to the observed long-term global cooling in the
Cenozoic.
5 Summary
In summary, we compared the climate’s sensitivity to
the opening of the Drake Passage under the present and
292 ATMOSPHERIC AND OCEANIC SCIENCE LETTERS VOL. 3
the Early Eocene land-sea configurations with four nu-
merical experiments. These experiments show that the
thermal isolation effects caused by the opening of the
passage are much stronger under the present land-sea
configuration. The opening of the Drake Passage under
the present land-sea configuration causes more heat
transport to the Northern Hemisphere and reduces heat
transport to Antarctica, hence leading to a significant
cooling around Antarctica. In comparison, the climate
sensitivity to the opening of the Drake Passage is much
weaker under the Early Eocene land-sea configuration.
The opening of a narrow and shallow Drake Passage only
causes weak anomalies in heat transport and global sur-
face temperature, which are not strong enough to ther-
mally insulate Antarctica. These experiments demonstrate
that the climate impact of Drake Passage depends on the
passage geometry. In earlier sensitivity experiments that
were carried with the present topography and bathymetry
conditions, the cooling effect of the Drake Passage has
been overestimated in explaining the Cenozoic cooling. It
is unlikely that the opening of the Drake Passage played
an important role in the Cenozoic cooling, especially in
the abrupt cooling at the Eocene-Oligocene boundary.
Acknowledgements. This work was supported by the National
Natural Science Foundation of China under Grant 40902054 and the
Earth System Model Modeling project supported by Statoil, Nor-
way.
References
Barker, P. F., 2001: Scotia Sea regional tectonic evolution: Implica-
tions for mantle flow and palaeocirculation, Earth Sci. Rev., 55,
1–39.
DeConto, R. M., and D. Pollard, 2003: Rapid Cenozoic glaciation of
Antarctica induced by declining atmospheric CO
2
, Nature, 421,
245–249.
Donnadieu, Y., R. Pierrehumbert, R. Jacob, et al., 2006: Modelling
the primary control of paleogeography on Cretaceous climate,
Earth Planet. Sci. Lett., 248, 426–437.
Huber, M., H. Brinkhuis, C. E. Stickley, et al., 2004: Eocene circu-
lation of the Southern Ocean: Was Antarctica kept warm by sub-
tropical waters? Paleoceanography, 19, PA4026, doi:10.1029/
2004PA001014.
Huber, M., and D. Nof, 2006: The ocean circulation in the southern
hemisphere and its climatic impacts in the Eocene, Palaeogeogr.
Palaeoclimatol. Palaeoecol., 231, 9–28.
Huber, M., and L. C. Sloan, 2001: Heat transport, deep waters, and
thermal gradients: Coupled simulation of an Eocene greenhouse
climate, Geophys. Res. Lett., 28, 3481–3484.
Jacob, R., C. Schafer, I. Foster, et al., 2001: Computational design
and performance of the Fast Ocean Atmosphere Model, version
one, in: Proc. 2001 International Conference on Computational
Science, V. N. Alexandrov et al. (Eds.), Springer-Verlag, Berlin
Heidelberg, 175–184.
Kennett, J. P., 1977: Cenozoic evolution of Antarctic glaciation, the
circum-Antarctic ocean, and their impact on global paleocean-
ography, J. Geophys. Res., 82, 3843–3859.
Lear, C. H., H. Elderfield, P. A. Wilson, 2000: Cenozoic deep-sea
temperatures and global ice volumes from Mg/Ca in benthic fo-
raminiferal calcite, Science, 287, 269–272, doi:10.1126/science.
287.5451.269.
Liu, Z., J. Kutzbach, and L. Wu, 2000: Modeling climate shift of El
Niño variability in the Holocene, Geophys. Res. Lett., 27(15),
2265–2268, doi:10.1029/2000GL011452.
Livermore, R., A. Nankivell, G. Eagles, et al., 2005: Paleogene
opening of Drake Passage, Earth Planet. Sci. Lett., 236, 459–
470.
Nong, G. T., R. G. Najjar, D. Seidov, et al., 2000: Simulation of
ocean temperature change due to the opening of the Drake Pas-
sage, Geophys. Res. Lett., 27, 2689–2692.
Royer, D. L., 2006: CO
2
-forced climate thresholds during the Phan-
erozoic, Geochim. Cosmochim. Acta, 70(23), 5665–5675.
Scher, H. D., and E. E. Martin, 2006: Timing and climatic conse-
quences of the opening of Drake Passage, Science, 312, 428–
430.
Sijp, W. P., and M. H. England, 2004: Effect of the Drake Passage
throughflow on global climate, J. Phys. Oceanogr., 34, 1254–
1266.
Sluijs, A. S., M. Schouten, M. Pagani, et al., 2006: Subtropical Arc-
tic Ocean temperatures during the Palaeocene/Eocene thermal
maximum, Nature, 441, 610–613, doi:10.1038/nature04668.
Toggweiler, J. R., and H. Bjornsson, 2000: Drake Passage and pa-
leoclimate, J. Quat. Sci., 15, 238–319.
Zachos, J. C., M. Pagani, L. Sloan, et al., 2001: Trends, rhythms,
and aberrations in global climate 65 Ma to present, Science, 292,
686–693.
Zhang, Z. S., H. J. Wang, and Z. T. Guo, 2009: Transition of ther-
mohaline circulation modes and its impact on Cenzoic climate,
Quat. Sci. (in Chinese), 29(6), 1064–1070.
ResearchGate has not been able to resolve any citations for this publication.
Article
Full-text available
An ocean general circulation model (GCM) is used to test the hypothesis that the opening of Drake Passage in the Oligocene may have lead to cooling in southern high latitudes. Results of previous studies show that no ocean models using restoring boundary conditions for the surface heat flux could reveal substantial southern high latitude cooling without prescribing atmospheric cooling a priori. To compute the surface heat flux that would be free from the restoring constraints we use another method, which is derived from an atmospheric energy balance model with lateral heat transport. In experiments conducted with both idealized and realistic topography the energy balance method produces substantial cooling not only in high latitudes but in deep waters as well.
Article
Full-text available
The effect of Drake Passage on the Earth's climate is examined using an idealised coupled model. It is found that the opening of Drake Passage cools the high latitudes of the southern hemisphere by about 3°C and warms the high latitudes of the northern hemisphere by nearly the same amount. This study also attempts to determine whether the width and depth of the Drake Passage channel is likely to be an important factor in the thermal response. A deeper channel is shown to produce more southern cooling but the magnitude of the effect is not large. Channel geometry is relatively unimportant in the model because of a haline response that develops when the channel is first opened up. Published in 2000 by John Wiley & Sons, Ltd.
Article
Full-text available
A coupled ocean-atmosphere general circulation model is used to investigate climatic shift of El Nino in the Holocene. The model simulates a reduced ENSO intensity in the early and mid-Holocene, in agreement with paleoclimate record. The ENSO reduction is proposed to be caused by both an intensified Asian summer monsoon and a warm water subduction from the South Pacific into the equatorial thermocline.
Article
The Palaeocene/Eocene thermal maximum, ~55 million years ago, was a brief period of widespread, extreme climatic warming, that was associated with massive atmospheric greenhouse gas input. Although aspects of the resulting environmental changes are well documented at low latitudes, no data were available to quantify simultaneous changes in the Arctic region. Here we identify the Palaeocene/Eocene thermal maximum in a marine sedimentary sequence obtained during the Arctic Coring Expedition. We show that sea surface temperatures near the North Pole increased from 18°C to over 23°C during this event. Such warm values imply the absence of ice and thus exclude the influence of ice-albedo feedbacks on this Arctic warming. At the same time, sea level rose while anoxic and euxinic conditions developed in the ocean's bottom waters and photic zone, respectively. Increasing temperature and sea level match expectations based on palaeoclimate model simulations, but the absolute polar temperatures that we derive before, during and after the event are more than 10°C warmer than those model-predicted. This suggests that higher-than-modern greenhouse gas concentrations must have operated in conjunction with other feedback mechanisms—perhaps polar stratospheric clouds or hurricane-induced ocean mixing – to amplify early Palaeogene polar temperatures.
Article
For the first time, a coupled general circulation model with interactive and dynamical atmospheric, oceanic, and sea-ice components, is used to simulate an Eocene (∼50 Ma) “greenhouse” climate. We introduce efficient ocean spin-up methods for coupled paleoclimate modeling. Sea surface temperatures (SSTs) and salinities evolve unconstrained, producing the first proxy data-independent estimates for these Eocene climate parameters. Tropical and extratropical model-predicted SSTs are warmer than modern values, by 3 and 5°C, respectively. Salinity-driven deep water formation occurs in the North Atlantic and Tethys. The zonal average overturning circulation is weaker than modern. Eocene ocean heat transport is 0.6 PW less than modern in the Northern Hemisphere and 0.4 PW greater in the Southern Hemisphere. The model-predicted near-modern vertical and meridional Eocene temperature gradients imply that the dominant theory for maintaining low gradients—increased ocean heat transport—is incorrect or incomplete and other mechanisms should be explored.
Article
Deep-sea drilling in the Antarctic region (Deep-Sea Drilling Project legs 28, 29, 35, and 36) has provided many new data about the development of circum-Antarctic circulation and the closely related glacial evolution of Antarctica. The Antarctic continent has been in a high-latitude position since the middle to late Mesozoic. Glaciation commenced much later, in the middle Tertiary, demonstrating that near-polar position is not sufficient for glacial development. Instead, continental glaciation developed as the present-day Southern Ocean circulation system became established when obstructing land masses moved aside. During the Paleocene (t=~65 to 55 m.y. ago), Australia and Antarctica were joined. In the early Eocene (t=~55 m.y. ago), Australia began to drift northward from Antarctica, forming an ocean, although circum-Antarctic flow was blocked by the continental South Tasman Rise and Tasmania. During the Eocene (t=55 to 38 m.y. ago) the Southern Ocean was relatively warm and the continent largely nonglaciated. Cool temperate vegetation existed in some regions. By the late Eocene (t=~39 m.y. ago) a shallow water connection had developed between the southern Indian and Pacific oceans over the South Tasman Rise. The first major climatic-glacial threshold was crossed 38 m.y. ago near the Eocene-Oligocene boundary, when substantial Antarctic sea ice began to form. This resulted in a rapid temperature drop in bottom waters of about 5°C and a major crisis in deep-sea faunas. Thermohaline oceanic circulation was initiated at this time much like that of the present day. The resulting change in climatic regime increased bottom water activity over wide areas of the deep ocean basins, creating much sediment erosion, especially in western parts of oceans. A major (~2000 m) and apparently rapid deepening also occurred in the calcium carbonate compensation depth (CCD). This climatic threshold was crossed as a result of the gradual isolation of Antarctica from Australia and perhaps the opening of the Drake Passage. During the Oligocene (t=38 to 22 m.y. ago), widespread glaciation probably occurred throughout Antarctica, although no ice cap existed. By the middle to late Oligocene (t=~30 to 25 m.y. ago), deep-seated circum-Antarctic flow had developed south of the South Tasman Rise, as this had separated sufficiently from Victoria Land, Antarctica. Major reorganization resulted in southern hemisphere deep-sea sediment distribution patterns. The next principal climatic threshold was crossed during the middle Miocenc (t=14 to 11 m.y. ago) when the Antarctic ice cap formed. This occurred at about the time of closure of the Australian-Indonesian deep-sea passage. During the early Miocene, calcareous biogenic sediments began to be displaced northward by siliceous biogenic sediments with higher rates of sedimentation reflecting the beginning of circulation related to the development of the Antarctic Convergence. Since the middle Miocene the East Antarctic ice cap has remained a semipermanent feature exhibiting some changes in volume. The most important of these occurred during the latest Miocene (t=~5 m.y. ago) when ice volumes increased beyond those of the present day. This event was related to global climatic cooling, a rapid northward movement of about 300 km of the Antarctic Convergence, and a custatic sea level drop that may have been partly responsible for the isolation of the Mediterranean basin. Northern hemisphere ice sheet development began about 2.5-3 m.y. ago, representing the next major global climatic threshold, and was followed by the well-known major oscillations in northern ice sheets. In the Southern Ocean the Quaternary marks a peak in activity of oceanic circulation as reflected by widespread deep-sea erosion, very high biogenic productivity at the Antarctic Convergence and resulting high rates of biogenic sedimentation, and maximum northward distribution of ice-rafted debris.
Article
The role of the Southern Ocean in global climate is examined using three simulations with a coupled model employing geometries different only at the location of Drake Passage (DP). The results of three main experiments are examined: 1) a simulation with DP closed, 2) an experiment with DP at a shallow (690 m) depth, and 3) a realistic DP experiment. The climate with DP closed is characterized by warmer Southern Hemisphere surface air temperature (SAT), little Antarctic ice, and no North Atlantic Deep Water (NADW) overturn. On opening the DP to a shallow depth of 690 m there is an increase in Antarctic sea ice and a cooling of the Southern Hemisphere but still no North Atlantic overturn. On fully opening the DP, the climate is mostly similar in the Southern Hemisphere to DP at 690 m, but the model now simulates NADW formation and a warming in the Northern Hemisphere. This suggests the North Atlantic thermohaline circulation depends not only on the existence of a DP throughflow, but also on the depth of the sills in the Southern Ocean. The closed DP experiment exhibits a large amount of deep-water formation [57 Sv (Sv 10 6 m 3 s 1)] in the Southern Hemisphere; this reduces to 39 Sv for the shallow DP case and 14 Sv when DP is at 2316 m, its modern-day depth. NADW formation is shut down in both DP closed and shallow experiments, which accounts for the warming in the Northern Hemisphere observed when the DP is opened. SAT differences between the DP open and closed climate are seasonal. The largest SAT changes occur during winter in areas of large sea ice change. However, summer conditions are still significantly warmer when DP is closed (regionally up to 4C). Summer SAT is the most important factor determining whether an Antarctic ice sheet can build up. Therefore our study does not exclude the possibility that changes in ocean gateways may have contributed to the glaciation of Antarctica. Overall, these experimental results support paleoclimatic evidence of rapid cooling of the Southern Ocean region soon after the isolation of Antarctica.