Standard Wireline Data Processing

 

Operator and logging contractor: LDEO-BRG

Hole: 19B (proposed site MNGH Gap)

Expedition: NGHP-1

Location: Manahadi Basin, Eastern India (Bay of Bengal)

Latitude: 18° 58.6532' N

Longitude: 85° 39.5160' E

Logging date: August 8, 2006

Sea floor depth (drillers'): 1433 mbrf

Sea floor depth (loggers'): 1436 mbrf

Total penetration: 1713 mbrf (280 mbsf )

Total core recovered: 271.28 m (90.4 % of cored section, from Hole NGHP-19A)

Oldest sediment cored: n/a

Lithologies: Nanofossil-rich clay (from Hole NGHP-19A)

 

Data

 

The logging data was recorded by Schlumberger in DLIS format. Data were processed at the Borehole Research Group of the Lamont-Doherty Earth Observatory.

 

Logging Runs

 

Tool string Pass Top depth (mbsf) Bottom depth (mbsf) Bit depth (mbsf) Notes
1. DIT/HLDS/APS/HNGS  Main
0
280
50.5
2. VSI
6 good stations
3. FMS/DSI/GPIT/SGT Pass 1
 69
263.4
Pass 2
 46
265.4

 

Hole 19B was a logging-dedicated hole. Prior to logging the hole was conditioned with a 40 bbl sepiolite sweep and then displaced with 100 bbl of 10.5 ppg barite. The DIT/HLDS/APS/HNGS run went smoothly and reached the bottom of the hole. Due to daylight requirements, the next run was the VSI; after some initial difficulties in reaching the open-hole interval, the tool was finally deployed to about 17 m above TD. Of the 10 stations attempted, six delivered reasonable results. The FMS/DSI/GPIT/SGT string was run last. Again, after some difficulty in passing an obstruction, the string reached about 13 m above TD on both passes.

The LDEO Wireline Heave Compensator compensated ship heave throughout the logging operations.

 

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.

 

Processing

 

Depth match and depth shift to sea floor: The DIT/HLDS/APS/HNGS pass was used as the depth reference, and the other passes were matched to it using resistivity and acoustic logs. All passes were then shifted to the sea floor (-1436 m), based on the step in gamma radiation at the sea floor in the DIT/HLDS/APS/HNGS pass. The DIT/HLDS/APS/HNGS pass was chosen as the reference run because it was the only one to reach the sea floor and to cover most of the open hole interval.

 

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 in the DIT/HLDS/APS/HNGS pass at 1436 mbrf (after depth matching). This differs by 3 m from the sea floor depth given by the drillers (see above).

 

Environmental corrections: The HNGS and SGT data were corrected for hole size during recording. The APS and HLDS have been corrected for standoff and hole diameter respectively during the recording.

 

High-resolution data: Bulk density and neutron porosity data were recorded at a sampling rate of 2.54 and 5.08 cm, respectively. The enhanced bulk density curve is the result of Schlumberger enhanced processing technique performed on the MAXIS system onboard. While in normal processing short-spacing data is smoothed to match the long-spacing one, in enhanced processing this is reversed. In a situation where there is good contact between the HLDS pad and the borehole wall (low-density correction) the results are improved, because the short spacing has better vertical resolution. SGT gamma ray was recorded at 15.24 and 5.08 cm sampling rates.

 

Acoustic data: The dipole shear sonic imager (DSI) was run in the following modes:

Pass 1: Low frequency monopole, low frequency upper dipole, standard (high) frequency lower dipole, and Stoneley modes.

Pass 2: Medium frequency monopole, and cross dipole modes.

Because of the slow formation, the automatic picking of wave arrivals in the sonic waveforms did not provide reliable results. Reprocessing of the original waveforms was required to extract meaningful compressional and shear velocities. The most reliable shear velocity value is the one derived from the upper dipole (VS2) during the first pass, where the lower source frequency used  generated more coherent waveforms.

 

Quality Control

 

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 acoustic log).

The hole is rough and irregular, with most readings above 12 inches. Despite the poor hole conditions, most of the log data of Hole 19B is of acceptable quality; the gamma ray logs from the three passes, however, correlate poorly, and the SFLU reads about 0.2 ohmm lower than the deep and medium resistivity (with the exception of the uppermost 20 m). The cause of this discrepancy could not be determined.

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.

 

A null value of -999.25 may replace invalid log values.

 

For further questions about the processing, please contact:

 

Cristina Broglia

Phone: 845-365-8343

Fax: 845-365-3182

E-mail: Cristina Broglia