Standard Wireline Data Processing
DSDP operator
and logging contractor:
Scripps Institution of Oceanography
Hole: 550B
Leg: 80
Location: Goban Spur (central N Atlantic)
Latitude: 48° 30.96' N
Longitude: 13° 26.37' W
Logging date: June 1981
Sea floor
depth (punch core
mudline in Hole 550): 4432 mbrf
Sea floor
depth (drillerŐs depth
used): 4432 mbrf.
Total
penetration: 720.5 mbsf
Total core
recovered: 177.91 m
(67.3 % of cored section)
Oldest
sediment cored: Late
Albian
Lithologies: nannofossil ooze and chalk and
mudstone, basalt (basement, 685 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. LSS/GR/MCD |
main |
0 |
698 |
89 |
|
repeat |
617 |
698 |
|||
2. DLL/GR |
main |
85 |
694 |
90 |
|
repeat |
641 |
703 |
|||
3. FDC/CNL/GR |
main |
0 |
694 |
120 |
Reference |
repeat | 563.5 |
691 |
All three tool
strings reached basement near of the bottom of the hole, and no problems were
reported. The LSS sonic tool appears to have been run on a single transmitter,
because the transit-time logs have the same symptoms as the LSS run at Hole
548B.
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 (-4432 m). The
FDC/CNL/GR main pass was chosen as the reference run because it had long 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.
There was no clear
step in the step in gamma ray values at the sea floor, so the sea-floor depth
given by the drillers, 4432 mbrf, was used. Using this depth also puts the
sediment-basement contact in the DLL logs at 685 mbsf, the same as in the
cores).
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 550B it appears that only one of the two transmitters was used
(similarly to Hole 548B). 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 FDC caliper gave a flat 7 inch
reading for the hole and is therefore invalid. The MDC caliper originally read
between 14-15 inches, and 10.5 inches inside the pipe. The pipe reading
indicates that the calibration of the caliper was wrong, so 4 inches has been
subtracted from the MCD caliper logs so that they more closely approach the
actual hole diameter. 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