Standard Wireline Data Processing
DSDP operator
and logging contractor:
Scripps Institution of Oceanography
Hole: 548A
Leg: 80
Location: Goban Spur (central N Atlantic)
Latitude: 48° 54.93' N
Longitude: 12° 09.87' W
Logging date: June 1981
Sea floor
depth (piston core
mudline): 1256 mbrf
Sea floor
depth (step in GR log):
1256 mbrf
Total
penetration: 551.5 mbsf
Total core
recovered: 249.33 m (72
% of cored section)
Oldest
sediment cored: Devonian
quartzite (basement)
Lithologies: nannofossil ooze and chalk (to late
Cretaceous), quartzite (basement, 532 mbsf).
The logging data
was recorded by Schlumberger in LIS format. Data were processed at the Borehole
Research Group at the Lamont-Doherty Earth Observatory in March 2004.
Tool string | Pass | Top depth (mbsf) | Bottom depth (mbsf) | Bit depth (mbsf) | Notes |
1. DIT/LSS/GR/MCD |
main |
150 |
536 |
171 |
|
2. FDC/CNL/GR |
main |
0 |
530 |
172 |
reference |
repeat |
441.5 |
492 |
Both tool
strings reached close to the bottom of the hole, and the first penetrated the
basement. The LSS sonic tool was run on a single transmitter. A second sonic
tool was rigged up but a surface equipment failure aborted the run. There was a
constant value offset (+ 155 API units) in the gamma ray log from the
FDC/CNL/GR run. The hole was flushed with 50 barrels of mud prior to logging.
The depths in
the table are for the processed logs (after depth matching between passes and
depth shift to the sea floor). Generally, discrepancies may exist between the
sea floor depths determined from the downhole logs and those determined by the
drillers from the pipe length. Typical reasons for depth discrepancies are ship
heave, wireline and pipe stretch, tides, and the difficulty of getting an
accurate sea floor from the 'bottom felt' depth in soft sediment.
Depth match
and depth shift to sea floor:
The original logs were depth-matched to the GR log from the main pass of the
FDC/CNL/GR tool string, and were then shifted to the sea floor (-1256 m). The
FDC/CNL/GR main pass was chosen as the reference run because it had the longest
hole coverage, crossed the sea floor, and because the cable speed was held
relatively constant. The GR logs from the other passes were matched to the GR
log from the reference run.
Depth-matching
is typically done in the following way. One log is chosen as reference (base)
log (usually the total gamma ray log from the run with the greatest vertical
extent and no sudden changes in cable speed), and then the features in the
equivalent logs from the other runs are matched to it in turn. This matching is
performed manually. The depth adjustments that were required to bring the match
log in line with the base log are then applied to all the other logs from the
same tool string.
The sea floor depth
was determined by the step in gamma ray values at the sea floor at 1256 mbrf.
This is the same as the sea floor depth determined by the drillers from a
piston core of the mudline.
Sonic data: Typically, LSS sonic data is processed
in the following way. The transit time data were processed using an in-house
program that compares the slowness derived from the 8 different
transmitter-receiver combinations at each depth, and discards those times that
are significantly different from the majority as bad data. The 'points' column
in the LSS data files is a measure of confidence: it records the number of transmitter-receiver pairs retained
- a value of 8 means that no data was discarded. This processing leads to improved compressional wave
velocity logs that are free of the artifacts present in the velocities derived
directly from DT and DTL.
In the case of
the LSS in Hole 548A only one of the two transmitters was used (according to
the paper plot made at the time of logging). However, the transit times, TT1,
TT2, TT3, TT4, are present in the original Schlumberger LIS file, representing
transmitter-receiver spacings of 12, 10, 10, and 8 feet respectively. This is
in contrast to the normal transmitter-receiver spacings of 10, 8, 12, and 10
feet respectively, and impossible to achieve with only one transmitter. It is
unclear to us exactly how all the transit time data were generated. We
therefore present only the transit time data, with no velocity calculation,
with the caution that the data does not follow the normal LSS pattern.
The quality of
the data is assessed by checking against reasonable values for the logged
lithologies, by repeatability between different passes of the same tool, and by
correspondence between logs affected by the same formation property (e.g. the
resistivity log should show similar features to the sonic velocity log).
Gamma ray logs
recorded through bottom hole assembly (BHA) and drill pipe should be used only
qualitatively, because of the attenuation on the incoming signal. The
thick-walled BHA attenuates the signal more than the thinner-walled drill pipe.
(The CNL porosity can sometimes be used qualitatively through the BHA and pipe,
but most of the other logs will not give usable data.)
A wide
(>12") and/or irregular borehole affects most recordings, particularly
those that require eccentralization and a good contact with the borehole wall
(FDC, CNL). Hole diameter was recorded by the hydraulic caliper on the FDC tool
(CALI) and by the 3-arm MCD tool (CALI). The hole varies between 9-13 inches in
diameter according to the MCD caliper, while the FDC caliper read between 10-11
inches, which is less realistic than the MCD caliper data.
A null value of
-999.25 may replace invalid log values.
Additional
information about the drilling and logging operation can be found in the
Operations section of the Site Chapter in DSDP Initial Reports Volume 80. For
further questions about the logs, please contact:
Cristina Broglia
Phone: 845-365-8343
Fax: 845-365-3182
E-mail: Cristina Broglia