3.5kHz Profiling with Vertically Separated Source and Receiver

"making a mini reflection survey around a deep-water drill hole"


Bolmer, S.T., Hoskins, H., Stephen, R.A.,
and the ODP Leg 200 Scientific Party


Woods Hole Oceanographic Institution,
360 Woods Hole Road, Woods Hole, MA 02543-1542 USA




ABSTRACT


     The spatial resolution of hull mounted 3.5kHz echo sounding systems is often limited in deep water by the large footptint (Fresnel zone) of the insonifying energy on the seafloor. On ODP Leg 200 at Site 1224, we tested a system that could be used from the drillship while on station to improve resolution. In 4970 m water depth, a 3.5 kHz pinger was mounted on the video camera frame and lowered down the drill string to a few meters above the seafloor. The ship's 3.5 kHz receiver recorded the returns. Having the source and receiver at differing distances above the seafloor provides two advantages: 1) the area returning reflections is greatly reduced, 2) the amplitudes of the sub-seafloor reflections are less affected by the spreading effect. Reflections were observed to 40 ms beneath the seafloor on lowerings at three closely spaced holes. The heave of the ship and camera frame shifted the travel times of the reflection sequences. A level-discriminator and correlation MatLab routine was used to align the traces and to stack them to enhance signal. The reflections showed good correlation with the limited geotechnical data obtained from the sediment cores. Although tested from the drill ship this system could be used to provide a low cost, shallow penetration profiling system from ROV's and AUV's. This work was supported by a grant from JOI-USSAC.

Figure 1. Hole 1224 is near the H2O observatory between Hawaii and California.

Figure 2. This 3.5-kHz echo sounder recording shows that the seafloor dips smoothly ~6 m from the H2O junction box to the drill site, 1224. One subbottom horizon at ~9 m is fairly uniform throughout the area. Based on drilling results, this is a mid-sediment reflector. A second reflector at ~30 m below the junction box can be associated with basaltic basement although it appears only occasionally in the record. One objective of lowering the 3.5 kHz source to the seafloor was to improve the resolution of the basement reflection. PDR = precision depth recorder.

Figure 3. This shows a schematic of the 3.5 kHz Experiment. The 3.5kHz source was on the VIT frame. The ship's hull mounted 3.5kHz Transducer was used to receive the signals. (This figure was adapted from the Leg 203 Intial Reports volume.)

 

EXPERIMENTAL SETUP


     The area of the seafloor insonified (within the first Fresnel zone) can be greatly reduced by lowering a broadbeam source to a few meters above the seafloor. By comparing the echo sequences observed at three holes at Site 1224, and at four elevations above the seafloor, inferences as to the lateral character of drilled interfaces can be made. In these data, there was little difference in spreading loss as the direct and reflected returns were recorded on the ship’s 3.5 kHz receiver nearly 5 km above the source and seafloor.
     The 0.25 sec data window, digitized at 24 kHz, was triggered by the direct water arrival from the back lobe of the transducer. A MatLab travel time alignment program was written to align the returns from the free-running source. Ten groups of aligned traces were stacked to reduce noise, and are shown in figure 7.

Figure 4. On the VIT frame, the 4.252-kHz transducer (a nominal 3.5 kHz source) is the squat cylinder in the middle under the frame's horizontal member. The pinger batteries and electronics are in the yellow cylinder to the upper left marked "Pinger."

Figure 5. (TOP) Installation of the reentry cone and steel casing in Hole 1224D as observed on deep-source records. This figure is excerpted from the EPC graphic recording on 2 January. The traveltime interval shown is ~410 ms; the light horizontal traces are spaced at 100 ms. The heavier vertical traces are 5-min marks. The 14-ms fluctuation with an amplitude of up to 4 ms in the traveltime of the direct water wave is primarily due to the heave of the ship pulling and slackening the vibration isolated television (VIT) cable. The 1- to 2-ms fluctuations in the traveltime for the reentry cone is a measure of the VIT heave plus the uncompensated heave of the drill string because the cone is rigidly linked to the ship’s heave compensator by the drill string. (BOTTOM) This shows the same data plotted using MatLab to show the match between the analog PDR recording and the digital data acquirred.

Figure 6. This figure contains part of the data shown in Figure 5. (TOP) A quarter (1/4) second window of data is shown with time 0 starting at the direct water wave arrival. The data at about .035 sconds is the seafloor arrival. Note the roughness due to ship's heave. (BOTTOM) The data here have been lined up at the first motion of the waveform representing the seafloor. Only 60 milleseconds (0.060 seconds) of data are shown below the seafloor. Note how the subbottom reflectors line up very coherantly in this figure. Both of the figures are a result of the MatLab code used to process the data.

RESULTS shown in figure 7

Reflector
Comment
Approximate
Travel time
Depth (Meters)
11 ms
Consistent between lowerings and differing source elevation;
appears to be an extensive interface
9.4
14 ms
Varies between lowerings and with differing source elevation;
probably a less planar interface
11.9
27 ms
Weak return which varies between lowering and source
elevation; perhaps a prominence in basement
24.5
32 ms
Strength varies with elevation; perhaps indicating a concave
surface which focusses and defocusses
29.5
36 ms
Strong basement reflector; change of echo envelope between
lowerings suggests irregular topography
33.5
39 ms
Big changes between lowerings and with source elevation;
perhaps represents a small hollow in basement surface
36.5

Taken together, the 32, 36 and 39 ms reflections suggest basement relief of up to 7 m in the vicinity of Site 1224.

 

Figure 7. This shows the stacks from 10 different windows at this site. There is good agreement of the data irregardless of the height of the source off of the seafloor. The different horizontal lines are referred to in the box above and to the left discusing results.

 

Conclusions


     Two subseafloor reflecting interfaces were identified that were drilled. Based on the changes in acoustic impedance indicated by the two reflections, the following stratigraphic spacing is suggested:
  • A. The 11-ms interval between the seafloor and the first subsurface reflection corresponds to the 9 m of unconsolidated yellow to brown clay cored, assuming that the sound velocity of this material is near that of water.
  • B. The 25-ms interval between the first and second subseafloor reflectors corresponds to a somewhat more consolidated sedimentary sequence ~19 m thick. There was little core retrieved from this interval.
  • C. Basaltic basement is an irregular surface at a depth of ~28 m bsf. Using the 3.5-kHz hull-mounted source, the basement reflector could be identified at the H2O junction box but not at the drill site. At the drill site, the basement reflector was only identified with the deep source.



          Contact us for further logistic details. These measurements do not take rig time. We would like to make further measurements and would welcome the opportunity to join future drilling legs.
    hhoskins@whoi.edu
    rstephen@whoi.edu
    tbolmer@whoi.edu


    This was created on December 12, 2003 by Tom Bolmer

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