Combining Heat Flow Measurements and Paleo
Climatic studies using R/V Marion Dufresne's unique coring capabilities
Louis Géli1,
François Harmegnies1, Yvon Balut3,
Jean-Louis Turon2, Daniel Aslanian1,
Paul Beuzart1, Jim Cochran4,
Jean Francheteau5, Jean-Yves Landuré1,
Raymond Le Suavé1, Alain Mazaud6,
Elizabeth Michel6, Alain Normand1,
Jean-Jacques Pichon2, Maurice Recq5,
Ivan Vlastelic7
1Ifremer, BP 70, 29280 Plouzané, France,
2Université de
Bordeaux-I, Avenue des
Facultés, 33405 Talence, France, 3Institut
français de Recherche Polaire, BP 75, 29280 Plouzané,
4Lamont Doherty Geological
Observatory, Palisades,
10964, New York, USA, 5Université de
Bretagne Occidentale, Institut Universitaire Européen de
la Mer, Place Nicolas, Copernic, 29280 Plouzané, France,
6Laboratoire des Sciences de l'Environnement, CNRS-CEA, 91198, Gif s/ Yvette, France, 7Max
Planck Institut für Chimie, Postfach 3060, 55020 Mainz, Germany.
For the first time, heat flow measurements and paleo oceanographic
studies were combined during the MD120-ANTAUS expedition of R/V
Marion Dufresne, the vessel of the French Polar Institute
(Fig.1). This program, which was conducted between October
12th and November 7th, from Fremantle (Australia) to La Réunion
Island, results from a collaboration between Ifremer, IFRTP, the
University of Bordeaux and the French Laboratory for Climate and
Environment Sciences (LSCE : Laboratoire des Sciences de l'Environnement
et du Climat). It also includes research scientists from Brest
and Mainz Universities, and from Lamont Doherty Geological Observatory.
Figure 1a :
R/V Marion Dufresne (photograph : courtesy of
IFRTP - See also Fig. 6) Named after Marc-Joseph Marion Dufresne
(1724-1772), R/V Marion Dufresne is a multi-purpose, 130 m long,
research and supply vessel having two main missions : logistics
for the French Austral Islands (Crozet and Kerguelen archipelagoes,
Amsterdam and Saint-Paul Islands) and oceanographic research.
Specifically designed for very severe weather conditions, she
benefits from an exceptional sea behaviour allowing full performance
in rough seas. The vessel is equipped with the full suite of geophysical
facilities (including multi beam bathymetry and imagery) and has
unique capabilities for raising long sediment cores, up to 60
meters (her record core being 58 meters), with a capacity for
110 passengers, allowing large scientific parties to embark for
multidisciplinary programmes. Facing an increasing scientific
demand, the French Ministry of Research decided in 1999 to reduce
the ship time devoted to logistical operations to 120 days/year
and allow the French Polar Institute (IFRTP : Institut Français
pour la Recherche et la Technologie Polaires) to conduct research
in all oceans, world-wide, 245 days/year. Therefore, the ship
is no longer confined to the Indian Ocean (for example, several
months in 1999 were spent coring for paleo-climatic purposes in
the North Atlantic). This paves the road for new approaches and
the development of integrated, multidisciplinary programs, as
recently evidenced by the MD120-ANTAUS expedition.
The primary objective of this cruise was to study terrestrial
heat flow variations along an isochron paralleling the South-East
Indian Ridge (SEIR) between the Saint-Paul/Amsterdam hotspot and
the Australian-Antarctic Discordance (AAD), an anomalously deep
section of the Mid-Ocean Ridge between Australia and Antarctica,
often attributed to a mantle " cold spot " (Fig.
3). Heat flow measurements were obtained in the region of
the AAD as part of reconnaissance surveys in the 1960's and 1970's
[Von Herzen and Langseth, 1966, Langseth and Taylor, 1967,
Anderson et al, 1977]. In some cases, conductivity measurements
were obtained from cores collected at the same location and at
a few sites, the maximum depths to which temperature was measured
was 3 to 10 meters. In addition, near-surface temperature gradients
are modified by bottom water temperature variations, calling for
temperature measurements deeper in the sedimentary column.
In order to interpret heat flow variations in this region of thin
and patchy sediment cover, it is not only necessary to obtain
more data, but to collect data that can also be used to trace
water circulation and discriminate between the conductive and
the convective components of the measured heat flow (Anderson
et al, 1979). To accomplish this, we collected long sediment
cores, along with heat flow data to greater depths. The cores
will be used to study the physical properties of the sediments
and also for 3He/4He studies, in order to investigate the role
of water cirulation using helium isotopic ratios as tracers of
hydrothermal activity. Our need for long cores led naturally to
an interdisciplinary program in which the heat flow objectives
are complemented by a study of paleoclimate variations. A total
of 25 terrestrial heat flow measurements were collected, using
9 autonomous digital temperature probes fitted on a 18 m-long,
13 cm-diameter, gravity corer (Fig. 2 and Table II).
Figure 2 : Temperature probes welded onto the gravity corer onboard
Marion Dufresne . Inset shows sketch of the Micrel THP autonomous
temperature probe (see performances in table I).
Table I : Main
technical characteristics of the Micrel THP autonomous pressure
tested temperature probe used during the MD120-ANTAUS expedition.
| Range |
-2° + 35°C |
| Resolution |
0,7 m°C à
20°C |
| |
Measurement possible
until + 70°, the resolution is then of about 9 m°C |
| Precision (linearity,
hysteresis, repeatibility) |
+/-7 m°C |
| Clock variation |
1 mn/month |
| Sampling rate |
Programmable, from 1s
to 99 h |
| Memory size |
254 ko with data compression
= 3 years on record mode at the rate of 1 hour, for a signal
varying of 0,1° every hour |
| Memory type |
Flash memory, recoverable
even if batteries are damaged |
| PC interface |
Electromagnetic transmission
without connector |
| Energy |
2 lithium batteries :
range > 3 years on record mode at 1 h, 21 days at 5 s |
| Pressure |
600 bars |
| Tube material |
Titanium |
| Lap material |
Ketron |
| Dimensions |
Probe length : 130 mm
; data logger pressure case : length = 183 mm ; diameter = 28
mm
Weight 0,280 kg |
Table II : Site locations and conductivity values. Note that
the average thermal conductivity increases progressively from
east to west, due to the change from siliceous to carbonate content,
as previously observed by Anderson et al (1977).
|
Core number |
Latitude |
Longitude |
Depth |
Core length |
Conductivity W/m/K |
| MD002362 |
S45°27,13 |
E123°27,31 |
4 740 m |
06,66 m |
0,687 |
| MD002363 |
S45°26,58 |
E123°32,16 |
4 520 m |
06,52 m |
0,729 |
| MD002364 |
S45°31,18 |
E123°32,94 |
4 380 m |
15,87 m |
0,717 |
| MD002365 |
S44°54,95 |
E125°34,29 |
4 700 m |
08,32 m |
0,701 |
| MD002366 |
S44°56,61 |
S125°25,54 |
4 400/ 4
450 m ? |
05,73 m |
0,789 |
| MD002367 |
S45°53,62 |
E129°57,77 |
4 380 m |
06,80 m |
0,8 |
| MD002368 |
S45°58,07 |
E130°01,08 |
4 500 m |
07,80 m |
0,764 |
| MD002369 |
S45°16,75 |
E120°01,59 |
4 430 m |
10,52 m |
0,717 |
| MD002370 |
S45°23,00 |
E119°51,96 |
4 240 m |
06,26 m |
0,788 |
| MD002371 |
S45°23,85 |
E113°29,50 |
4 120 m |
06,42 m |
0,782 |
| MD002372 |
S44°08,23 |
E105°49,48 |
3 840 m |
06,58 m |
0,883 |
| MD002373 |
S43°29,98 |
E99°58,99 |
3 750 m |
06,76 m |
0,956 |
| MD002374 |
S46°02,508 |
E96°29,493 |
3 320 m |
42,46 m |
|
| MD002375 |
S45°42,76 |
E86°45,01 |
3 500 m |
17,24 m |
0,797 |
Full penetration of 18 m was regularly achieved. In some places,
we used the " PO-GO " multiple-entry technique, allowing
series of 3 to 4 closely spaced measurements to be made for assessing
the local variability of heat flow. Fourteen gravity cores (with
lengths ranging between 6 m and 17.80 m) were collected. In addition,
one 42-m long core was obtained (the longest ever in this part
of the world ocean) using the R/V Marion Dufresne giant
piston corer, named Calypso, providing information on the
global climate changes that occured during the last 400 000 years.
These sediment cores form a good complement to the database of
the IMAGES (International Marine Global Change Study) program,
a part of the International Global Change Program (IGCP).
| Sediment redistribution in the ocean
basin south of the SEIR is controlled by relatively strong currents
associated with the Antarctic Circumpolar Current and the Antarctic
Bottom Water. These currents have a strong erosive capacity,
resulting in a large crestal area with a non uniform, thin (if
any) sediment cover. The heat flow measurement sites were located
along a 14 Ma isochron, parallel to the SEIR (Fig. 3).
Seismic data from USNS Eltanin and R/V Vema collected in the
60's and early 70's indicate that these sites are all located
in " grade C " or " grade D " environment,
according to the classification of Sclater et al (1976) : areas
of rough topography (ocean floor with greater than 400 m relief
and wavelength of 5-10 km) with a thin, variable sediment cover
(< 200 m) and basement outcropping within 15 km of the station.
In this type of environment, most of the scatter in closely spaced
heat flow measurements results from hydrothermal circulation.
To characterize and tentatively model this circulation, sediment
samples clamped in 25 cm-long copper tubes were systematically
taken at different depths in each sediment core for 3He/4He studies.
Samples were taken at 15 cm from the extremity of each 1.5 m-long
core section, 2 to 4 hours after the core was onboard, in order
to avoid the diffusion of Helium out ot the sediments. If water
has circulated within the crust, then the 3He/4He isotopic signature
should theoretically be that of the crust and upper mantle ;
if water circulation has been confined to the sediment layer,
then the 3He/4He isotopic signature will be that of the ocean
and atmosphere. |
Figure 3 : Site locations (see exact coordinates in table II).
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The quality of the heat flow data is illustrated by
the example in Figure 4, showing depth-temperature data
for the longest core recovered (17.25 m). The temperature gradient
is almost perfectly linear and equal to G = 69.8 ± 0.83
mK/m (Fig. 4a). Thermal conductivity, which was measured
onboard every 25 cm along the core length, exhibits important
variations, up to 30 % (note however that when the " equivalent
conductivity (k) " is considered - 1/k=1/nxS(1/ki),
where n is the number of 25 cm-long segments -, the uncertainty
on k is only 8 %). In order to account for these variations,
we introduce, following Bullard (1939), a thermal resistance
x, such as : dx=dz/k.
Heat flow, obtained as the slope of T(x),
integrates the variations in thermal conductivity. Its value
is : qBullard=dT/dx= 55.4
± 4.5 mWm-1. The product of G by the "
equivalent conductivity " value yields : q = 55.6 mWm-2 ±
6.7 mWm-2, which is very close to qBullard.
Because they are of short wavelength (< 1 m), thermal conductivity
variations do not significantly affect the estimation of heat
flow, which is based on temperature probes spaced every 2 meters.
In the few cases where heat flow measurements have been made
in DSDP and ODP drill holes and compared to nearby surface heat
flow measurements, good agreement has been found, suggesting
that standard heat flow measurements made with typical penetrations
of 3 to 4 m are reliable enough to model deep seated thermal
processes [e.g. Erickson et al, 1975 ; Hyndman et al, 1984 ;
Horai and Von Herzen, 1985 ; Fischer et al, 1997]. Data collected on the South-East
Indian flanks with R/V Marion Dufresne using autonomous temperature
probes welded onto a 18 m long core show that this is not always
the case : in the study area, the agreement between surface heat
and deep seated heat flow is rarely met. Most often, indeed,
the temperature gradients that we obtained are not linear.
Figure 4 :
4a. Temperature vs depth curve at core site MD-002375 ; Thermal
conductivity vs depth for core MD-002375 corrected from temperature
and pressure ; 4c : Temperature vs integrated thermal resistance
(x) for core MD-002375.
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Figure 5 shows three examples of temperature data collected
at three different sites. Each temperature measurement being
systematically duplicated by two sensors spaced by 64 mm, experimental
effects cannot explain the observed non-linearity (in addition,
tests performed onboard after recovery clearly preclude systematic
errors resulting from errors of calibration or from drift of
a thermistor). The observed non linearity, which is too important
to be explained by variations in thermal conductivity, results
from either one or from the combination of two natural effects
: variations in bottom water temperature and vertical advection
of water into the sediments. At two sites (MD002369 and MD002371),
the existence of vertical temperature gradients between two successive
temperature sensors indicates the probable presence of an aquifer
within the sediment column, the effect of which needs to be taken
into account to estimate the conductive component of heat flow.
Further analysis, including hydrology and He results, is needed
to interpret the data and determine the contribution of each
different effect.
The above points out some advantages of combining coring and
heat flow measurements at great depths within the sediments .
R/V Marion Dufresne has the capacity to take ultra long cores
(up to 60 meters) using the Calypso giant corer. Theoretically,
the longer the core, the more information on the heat flow at
depth. In practice, however, there are some limitations in core
length. Tests performed on the Meriadzeck Plateau in 1999 using
25-m-long piston corers have clearly shown that adding temperature
probes on the tube multiplies by a factor of 2 the required traction
for pulling the corer out of the sediments. Heat flow measurements
at depths of 30 to 40 m is thus an objective that seems feasible,
although difficult to reach in routine. But for all R/V Marion
Dufresne's coring programmes that require gravity cores for preserving
surface sediments, heat flow measurements could be routinely
and systematically performed in the future without any additional
shiptime using 15 m to 25 m-long pipes. This would dramatically
increase the number of heat flow measurements in the world ocean.
Figure 5 :
Temperature vs depth curve at core sites : 5a) MD-002369. Note
that between 10.2 m and 12.8 m, temperature is constant ; 5b)
MD-002370 ; 5c) MD002371. Note that between 2.15 m and 4.35 m
and between 8 .75 m and 10.94 m, temperature is constant.
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Acknowledgments : We acknowledge the effective collaboration
of Captain R. Gauthier which gave much freedom for initiatives
by the scientific team enabling collection of record gravity and
CALYPSO cores ; the professional efficiency of the team handling
the cores on the fantail ; and the excellent station-holding capability
of the R/V Marion Dufresne, even in very bad weather.
*****************
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mechanism of heat transfer through the floor of the Indian Ocean,
J. Geophys. Res., 82, 3391, 1977
- Anderson, R. N., Hobarth, M. A., and Langseth, M. G., Geothermal
Convection Through Oceanic Crust, Science, 204,
823, 1979
- Bullard, E. C., Heat flow in South Africa, Proc. R. Soc.
London Ser., A, 173, 474, 1939
- Erickson, A.J., Von Herzen, R.P., Sclater, J. G., Girdler,
R.W., Marshall, B.V., Hyndman, R., Geothermal Measurements in
Deep-Sea Drill Holes, J. Geophys. Res., 17, 2515-2528,
1975
- Langseth, M. A., and Taylor, P. I., Recent measurements in
the Indian Ocean, J. Geophys. Res., 72, 6249, 1967
- Horai, K., Von Herzen, R.P., Measurement of Heat Flow on
the Leg 86 of the Deep Sea Drilling Project, Initial Report
of Deep Sea Drilling Project, 1985
- Hyndman, D.R., Langseth, M.G., Von Herzen, R.P., Review of
deep sea drilling project geothermal measurements through leg
71, Initial Report of Deep Sea Drilling Project, 78B,
813-823, 1984
- Duyker, E., An Officer of the Blue, Marc-Joseph Marion Dufresne,
South Sea Explorer, 1724-1772, Melbourne University Press, 229
p., 1994
- Sclater, J. G., Crowe, J., and Anderson, R. N., On the reliability
of oceanic heat flow averages, J. Geophys. Res., 81,
2997, 1976
- Von Herzen, R.P., Langseth, M.G., Present Status of Oceanic
Heat-Flow Measurements, Phys. Chim. Earth, 365, 1966
- Fisher, A.T., Becker, K., and Davis, E.E., The permeability of young
oceanic crust east of Juan de Fuca Ridge determined using borehole thermal
measurements. Geophys. Res. Lett., 24, 1311-1314, 1997
Figure 6 :
Death of Nicolas-Joseph Marion Dufresne (crayon, pencil and chalk
sketch of Charles Meryon, 1821-1868). Born in Saint-Malo, northern
France, to a family of merchants, Marion Dufresne embarked at
the age of 11 with the French East India Company. In 1771, he
sailed from Mauritius to Tahiti in command of two ships of the
French Navy that were returning Tahitian chief Ahu-toru from France
to Tahiti. Soon after leaving Mauritius, Ahu-toru died of smallpox.
Consequently, instead of continuing on to Tahiti, Dufresne set
out to explore the extreme southern part of the Indian Ocean in
search of Terra Australis, and discovered Marion, Crozet and Prince
Edward Islands. While in New Zealand, he undertook coastal explorations
and established friendly contacts with the native Maori. However,
on January 12, 1772, Dufresne and some of his men were attacked
and killed by the Maori. Dufresne's surviving officers made important
contributions to the study of Maori life and culture, noting the
similarities between the Maori language and that of the Polynesian
inhabitants of Tahiti. Moreover, scientists with the expedition
made some of the earliest studies of ocean temperatures and salinity
levels at varying depths (See book of Duyker, 1994).
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