Site U1393 |
Site U1394 |
Site U1395 |
Site U1396 |
Site U1397 |
Site U1398
IODP Expedition 340: Lesser Antilles Volcanism and Landslides
Site U1399 Summary
PDF file is available for download.
Background and objectives
Integrated Ocean Drilling Program (IODP) Site U1399 (CARI-08B, 14°23.24'N, 61°42.69'W, 2900 mbsl) is located west of Martinique. The
objective of Site U1399 is to characterize the processes accompanying debris
avalanche emplacement and associated erosion. The seismic and bathymetric
survey for Site U1399 revealed that this site is located on one of the main chaotic
deposits and that coring at this site will most likely retrieve volcanic and
biogenic sediments with intercalated, large, chaotic debris avalanche deposits
of the so called debris avalanche deposit 1. In detail, we hope to be able to
characterize and quantify the erosional processes of the upper sedimentary
layers deposited in the Grenada Basin associated with such debris avalanches
and their subsequent incorporation into the flow. Finally, we are going to
compare the characteristics of debris avalanches deposits from Dominica and
Martinique to constrain possible differences in erosional capability and
mobility. The sediments above the debris avalanche deposit 1 will be used to
better constrain the age of the slide event.
Scientific Results
Site U1399 (CARI-08B) consisted of three holes. The original plan called for two holes
to be cored to ~290 mbsf. The first hole was successfully cored and was
terminated at 275 mbsf. The second hole was piston cored to 183 mbsf and
abandoned when the hole became too unstable to continue coring operations. Thus
the planned logging operations for this hole were abandoned too. Instead the
decision was made to drill a dedicated logging hole to 240 mbsf – Hole
U1399C. The logging program, including the triple combo, FMS-sonic and VSI tool
strings, was completed as planned. A total of 393 m of core (101% recovery) was
obtained with the APC coring system, whereas 9 m of core (14% recover) was
obtained with the XCB coring system. The overall core recovery for Site U1399 is
89%. The total time spent on Site U1399 was 160.00 hours.
The
sediments cored at Site U1399 are again dominated by a combination of
hemipelagic mud with interbedded tephra and volcaniclastic turbidites as well as various types of
deformed sedimentary intervals that occur at different depths. Eight lithostratigraphic units (Unit A to Unit H) have been
defined based either on characteristic changes throughout the cored material or
distinct marker layers. Unit A (0 to 24 mbsf in Hole U1399A; 0 to 12 mbsf in
Hole U1399B) is mainly composed of hemipelagic mud with abundant interbedded tephra layers. In Hole U1399A, several small
turbidites are also interbedded in the hemipelagic
mud, whereas only one turbidite could be identified
in Hole U1399B. Most of the tephra and turbidite
layers contain pumice in variable abundances (5% to 65%). Unit B (24 to 50 mbsf
in Hole U1399A; 12 to 29 mbsf in Hole U1399B) is composed of a thick sequence
of variably deformed hemipelagic sediment with several areas of inclined and
convoluted banding. This unit also contains debris flow deposits (debrites) with a muddy-sand matrix. Dispersed lava clasts and deformed tephra layers are often found within the debrites. Unit C (50.5 to 72 mbsf in Hole U1399A;
29 to 53 mbsf in Hole U1399B) consists of hemipelagic mud with interbedded tephra layers and thin turbidites (less than 1
m thick). The base of Unit C is composed of a 1 m thick interval of hemipelagic
mud overlain by a turbidite. This basal turbidite is 8.2 m thick in Hole U1399A and 2.1 m thick in Hole U1399B. In Unit D (72 to 76 mbsf in Hole U1399A; 53 to 68.5 mbsf in Hole U1399B)
the upper part is composed of deformed sediment with inclined contacts between
zones of different colored mud, whereas the lower part is composed of weakly
deformed hemipelagic mud with inclined green laminae.
Unit E (76 to 112 mbsf in Hole U1399A; 68.5 to 102.7 mbsf in Hole U1399B)
consists of a succession of alternating layers of non-deformed hemipelagic mud with interbedded tephras and
thin turbidites, deformed hemipelagic mud, debrites,
and thick turbidites. Unit F (114 to 142.5 mbsf in Hole U1399A; 102.7 to 129
mbsf in Hole U1399B) is composed of a thick sequence of highly deformed and
contorted sediment, including some turbidites and contorted tephra layers. Unit
G (142.5 to 191.7 mbsf in Hole U1399A; 129 to 182.3 mbsf in Hole U1399B) is mainly composed of thick sequences of pumice-rich turbidites with interbedded
hemipelagic mud containing a few tephra layers. The proportion of hemipelagic
mud in this unit is low. Unit H (191.7 to 270 mbsf in Hole U1399A) is mainly
composed of hemipelagic mud, with interbedded tephra
layers and pumice-rich turbidites. The proportion of hemipelagic mud (70%) is
higher than in preceding units, and tephra layers are frequently observed.
As shown by the carbonate analysis of 33 samples throughout the entire cored interval calcium
carbonate concentrations are highly variable and are lower in intervals with
higher proportions of volcanic material and presumably terrestrial clay. The
maximum concentration is about 35%, which partly also reflects the absence of
significant aragonite preservation.
The core catcher samples taken from Site U1399 for biostratigraphic
studies contain calcareous nannofossils and planktic and benthic foraminifera of varying abundances and at varying levels of preservation. The calcareous nannofossil and planktic foraminifera datums
obtained from the cored material indicate that the sediments sampled have been
deposited during the Late Pleistocene, indicating an extremely high
sedimentation rate for this site. Reworking of much older (Early Pleistocene
and Late Pliocene) material is evident in several samples. Many of the core
catcher samples at Site U1399 consisted of very coarse-grained material,
containing numerous shallow water benthic foraminifera and fragments of shell
and coral. Well preserved pteropod and heteropod shells, otoliths and
sponge spicules (Demospongiae) were also found in
some of the hemipelagic samples. Observed nannofossil
species are Gephyrocapsa oceanica, Gephyrocapsa parallela, Helicosphaera hyalina, Emiliania huxleyi as well as Ceratolithus cristatus and Ceratolithus telesmus.
Encountered reworked specimens are Pseudoemiliania lacunosa, Calcidiscus macintyrei, Sphenolithus neoabies/abies and Binatholithus sparsus. The assemblage
of observed planktic foraminifera was diverse, but
dominated by Globigerinoides ruber (white and pink), Globigerinoides sacculifer and Neogloboquadrina dutertrei (dextral). Other abundant species includeGloborotalia truncatulinoides andGloborotalia tumida. The assemblage does not change
significantly throughout the site and all species present are indicative of
warm sub-tropical waters. Several datum species were found, however, reliable
datum species were generally not found in samples with low planktic
foraminifera abundance. Globorotalia flexuosa
(0.07-0.40 Ma) and Globigerinella calida (base
of occurrence at 0.22 Ma) were only found in low numbers. The last occurrences
of these datum species are not clearly defined and no reliable planktic foraminifera datum was found at the base of either holes. Reworked planktic
foraminifera included Globorotalia tosaensis
(top of occurrence 0.61 Ma), Globorotalia exilis (top of occurrence at 2.10 Ma), Globorotalia miocenica
(top of occurrence at 2.39 Ma), Dentoglobigerina altispira (top of occurrences at 3.13 Ma), Sphaeroidinellopsis seminulina
(top of occurrence at 3.16 Ma), and possiblyGlobigerinoides mitra (Early
to Late Miocene).
Interpretation
of the behavior of the geomagnetic field during the deposition of the cored
sediments to derive at a magnetostratigraphy is solemnly
based on the data from the non-chaotic intervals. This is roughly 20% of the paleomagnetic directional data obtained from Site U1399. Between
0 and 207.5 mbsf in Hole U1399A and all of Hole U1399B SRM and discrete
inclination data show scattered but positive values, clustering around the
expected Geocentric Axial Dipole (GAD) inclination. Expected inclination for
the site is 27.2° during normal polarity and -27.2° during reversed polarity
assuming a GAD. Declination shows some scatter but coupled with the positive
inclination data suggests all sediments were deposited under normal polarity
conditions. Using the geomagnetic polarity timescale of Cande
and Kent (1995) these sediments were deposited in the Brunhes
Chron and are younger than 780 ka.
Different from the previous sites, the magnetic susceptibility data obtained from the cored material at Site U1399 show not clear variation with the material recovered.
Only two strong peaks correlating to thicker layers of coarse-grained volcaniclastic material have been observed throughout both
holes. Bulk density data scatter around an average value of 1.7 g/cm3
and generally increase with depth. Reduction of the bulk density data using a
moving average, extending over 20 m, shows that significant difference in
density exist between the two holes, consistent with difference in
sedimentation rate. The analysis of the smoothed data implies large swings in
density between the hemipelagic and volcaniclastic
zones. Bulk density obtained from the measurement of discrete hemipelagic
samples ranges between 1.5 and 1.8 g/cm3, displaying a weak positive
correlation with depth. Sandy samples have bulk densities as high as 2.05 g/cm3.
As in all previous sites, porosity and bulk density display a clear negative
correlation. Grain density varies between 2.65 and 2.8 g/cm3. The
volcanic sands have a similar grain density compared to the hemipelagic samples.
Porosity obtained from the measurement of discrete hemipelagic samples ranges
between 53% and 73%. In contrast to the previous sites, Site U1399 shows a weak
negative porosity-depth correlation from ~70% at mud line to ~60% at 270 mbsf. Porosity
in volcanic sand samples ranges between 40% and 50%. The porosity of the loose
sands may be underestimated up to 20% due to draining of pore-water during
coring, splitting and sampling. The natural gamma radiation data show the
differences expected measuring hemipelagic sediment and volcanic material.
Count rates in the hemipelagic material vary between 15 and 50 counts per
second, whereas the count rates in the volcanic material are below 15 counts
per second. P-wave velocities obtained from hemipelagic sediment shallower than
140 mbsf range from 1500 to 1550 m/s, whereas the volcaniclastic
material shows velocity values between 1650 and 1800 m/s. Between the depth
interval of 140 to 180 mbsf P-wave velocities increase gradually from 1550 and
1650 m/s to 1650 and 1900 m/s in the hemipelagic and volcaniclastic
sediment, respectively. Shear strength of the studied material generally increases
downhole in both holes. Downhole formation temperature was measured by APCT-3
at the bottom of Cores U1399A-3H, -4H, -5H, and -6H (24, 34, 43, and 53 mbsf,
respectively) and the bottom of Cores U1399B-3, -6H, and -9H (25, 53, and 81 mbsf,
respectively). The geothermal gradient calculated based on the obtained
temperatures is 65.4±0.9°C/km. Using the thermal conductivity of 1.045±0.080 W/mK obtained from the cored material, the implied heat flow,
if conductive, is 68.3±5.8 mW/m2. This
estimate probably needs to be corrected, based on the high sedimentation rate observed
at this site. Despite a separation of 410 m between the two holes cored at this
site, all temperature measurements lie on a single line. This suggests that
fluid flow is not disturbing the temperature gradient.
The in
situ measurements of physical properties obtained by the downhole logging
operations on Hole U1399C are generally of good quality. Four different logging
units have been identified based on specific characteristics observed across
the physical properties measured, especially gamma ray, resistivity and
magnetic susceptibility obtained by the tools in the triple combo tool
string. Logging Unit 1 (80-106
mbsf) is characterized by an overall increase in gamma ray with depth from ~25
to ~50 gAPI. The magnetic susceptibility and electrical resistivity profiles are similar in character with a small net decrease with depth. At 106 mbsf, the transition from Unit 1 to Unit 2 (106-150 mbsf) is marked by a sharp decrease in gamma ray that coincides with sharp increases in resistivity and magnetic
susceptibility. Similar to Unit 1,
Logging Unit 2 shows a net increase with depth in gamma ray. Between 140 and
150 mbsf there is an interval of increased gamma ray values, this is reflected
in both the total gamma ray and spectral gamma ray measurements. Interestingly
this increase is not shown in the corresponding NGR data from cores recovered
in Hole U1399A. Resistivity
generally decreases with depth through this logging unit with localized high
resistivity features. This trend is repeated in the magnetic susceptibility
curve. Logging Unit 3 (150-181 mbsf) is characterized by higher amplitude
variability in gamma ray, resistivity and magnetic susceptibility. Similar to
the transition between Logging Units 1 and 2, the transition from logging Unit 2
to Unit 3 is marked by a step-wise decrease in gamma ray and increases in
resistivity and magnetic susceptibility. Generally lower values of gamma ray
coincide with higher values of both resistivity and magnetic susceptibility. Logging
Unit 4 (181 mbsf to total hole depth) is characterized by more regular gamma
ray variations, of the order ~15 gAPI, continuing
through the upper 25 m of this unit, after which variations decrease in
amplitude. In addition this unit exhibits the most variable magnetic
susceptibility profile in Hole U1399C, including some significant peaks, the
largest of which (~205-208 mbsf) corresponds to similarly elevated values of
resistivity. Check-shot travel times obtained by the seismic experiments range
from 0.128 seconds two-way time at 87.8 mbsf to 0.279 seconds at the bottom of
the hole (225.7 mbsf).
Twenty-eight
samples for headspace analyses were taken throughout the hole. Methane
concentrations were only a few ppm in all but the
deepest sample. The deepest sample (276 mbsf in Hole U1399A) yielded a methane
concentration of 690 ppm. This is slightly deeper than the zone of high methane
concentrations observed at Site U1398. The major ion pore water profiles are characteristic of a deep-sea diagenetic sequence. Sulphate concentrations gradually decrease over the same
interval over which alkalinity and ammonia shows steady increases. Calcium
concentrations show a steady decrease with depth, reflecting precipitation of
secondary carbonate. Magnesium concentrations also show a decrease with depth being
most likely caused by alteration of volcanic material. The slight increase in
chloride concentrations also reflects uptake of water into secondary mineral
phases at depth. The shape of the pore water profiles suggests that the main oxidation of organic carbon takes place in the upper 60 m of the sediment column. Generally organic carbon concentrations decrease with depth. The upper 115 m of the interval cored contain several samples with organic carbon concentrations close to 1 wt.%,
whereas the maximum concentration observed in the lower 155 m is about 0.7 wt.%.
The change in organic carbon concentrations between the upper 115 m and the
lower 155 m of the sediment column may reflect a change in the input of organic
carbon to the system rather than changes in preservation. There is, however, a
strong caveat to this hypothesis as the percentage of volcanic material can
also vary with depth, and this may act to cause variable dilution of a constant
input flux of organic carbon to the sediments.
References
Cande, S.C., and Kent, D.V. (1995) Revised calibration of the geomagnetic polarity timescale for the late Cretaceous and Cenozoic. Journal of Geophysical Research, 100: 6093-6095.
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