FMS Image Data Processing
ODP logging
contractor: LDEO-BRG
Hole: 1011-B
Leg: 167
Location: Baja California Margin (tropical NE Pacific Ocean)
Latitude: 31° 16.817' N
Longitude: 117° 38.0080' W
Logging date: May, 1996
Bottom felt: 2032.5 mbrf (used for depth shift to sea floor)
Total penetration: 281.5 mbsf
Total core recovered: 271.1 m ( 96%)
FMS Pass: 97-257 mbsf
Magnetic declination: 12.99697°
Water depth: 493.5 mbrf
The basic principle of the FMS (Formation MicroScanner) is to map the conductivity of the borehole wall with a dense array of sensors. This provides a high resolution electrical image of the formation which can be displayed in either gray or color scale. The purpose of this report is to describe the images from Leg 167 and the different steps used to generate them from the raw FMS measurements
The FMS tool records 4 perpendicular electrical images, using four pads, which are pressed against the borehole wall. Each pad has 16 buttons and the tool provides approximately 25% coverage of the borehole wall. The tool string also contains a triaxial accelerometer and three flux-gate magnetometers (in the GPIT, General Purpose Inclinometry Tool) whose results are used to accurately orient and position the images. Measurements of hole size, cable speed, and natural gamma ray intensity also contribute to the processing.
The FMS images in Hole 1011B are of
moderate quality. Reliable data were recorded in the lower half of the logged
interval, below 185 mbsf. Above, the hole is very degraded, with the worst
conditions occurring from 97 to 138 mbsf. All along the logging interval,
conductive levels (dark) correspond to hole enlargements, for instance at 165,
175, 203, 222, 226, and 232 mbsf. Furthermore, numerous thin conductive
laminations are detected on the FMS images (for instance in the 150-152,
160-162, 199-201, and 204-206 mbsf intervals) and are clearly related to the
overprint on the borehole wall left by the rotation of the drill-bit during
drilling. As a consequence, lithological or structural interpretations from the
conductive features have to be made with caution.
Good quality FMS images were
obtained in the lower section from 138 to 257 mbsf. The transition between Unit
IIA and IIB is expressed by an increase of the resistivity at 130 mbsf, despite
the bad hole condition at this particular depth. The overall matrix resistivity
decreases below 246 mbsf, which marks the limit between Unit IIIA and IIIB. The
210-240 mbsf interval is characterized by the regular occurrences of conductive
bands (10 to 20 cm thick) within a more resistive matrix. These conductive
bands are regularly spaced, and show a cyclical pattern which vanishes above
210 mbsf (transition Units IIC and IIIA). Some highly resistive layers, 10 to
20 cm thick, are detected along the logging interval at 138, 143.8, 146, 149,
230.5, and 252.8 mbsf and do not correlate with obvious features observed on
cores.
Image Processing
Processing is required to convert the electrical current in the formation, emitted by the FMS button electrodes, into a gray or color-scale image representative of the conductivity changes. This is achieved through two main processing phases: data restoration and image display.
1) Data Restoration
Speed
Correction. The data from the z-axis accelerometer is used to correct the
vertical position of the data for variations in the speed of the tool (GPIT
speed correction), including stick and slip. In addition, image-based speed
correction is also applied to the data: the principle behind this is that if
the GPIT speed correction is successful, the readings from the two rows of
buttons on the pads will line up, and if not, they will be offset from each
other (a zigzag effect on the image).
Equalization: Equalization is the process whereby the average response
of all the buttons of the tool are rendered approximately the same over large
intervals, to correct for various tool and borehole effects which affect
individual buttons differently. These effects include differences in the gain
and offset of the pre-amplification circuits associated with each button, and
differences in contact with the borehole wall between buttons on a pad, and
between pads.
Button Correction. If the measurements from a button are unreasonably
different from its neighbors (e.g. dead buttons) over a particular interval,
they are declared faulty, and the defective trace is replaced by traces from
adjacent good buttons.
EMEX voltage correction. The button response (current) is controlled by the EMEX voltage, which is applied between the button electrode and the return electrode. The EMEX voltage is regulated to keep the current response within the operating range. The button response is divided by the EMEX voltage so that the response corresponds more closely to the conductivity of the formation.
Depth-shifting: Each of the logging runs are depth-matched to a common scale by means of lining up distinctive features of the natural gamma log from each of the tool strings. If the reference logging run is not the FMS tool string, the specified depth shifts are applied to the FMS images. The position of data located between picks is computed by linear interpolation.
2) Image Display:
In "static normalization", a histogram equalization technique is used to obtain the maximum quality image. In this technique, the resistivity range of the entire interval of good data is computed and partitioned into 256 color levels. This type of normalization is best suited for large-scale resistivity variations.
The image can be enhanced when it is desirable to highlight features in sections of the well where resistivity events are relatively subdued when compared with the overall resistivity range in the section. This enhancement is called "dynamic normalization". By rescaling the color intensity over a smaller interval, the contrast between adjacent resistivity levels is enhanced. It is important to note that with dynamic normalization, resistivities in two distant sections of the hole cannot be directly compared with each other. A 2-m normalization interval is used.
For further information or questions about the processing,
please contact:
Cristina Broglia
Phone: 845-365-8343
Fax: 845-365-3182
E-mail: Cristina Broglia