dsi 1 dsi* dipole shear sonic imager. dsi 2 lecture plan ä wave propagation - monopole & dipole...
TRANSCRIPT
DSI 1
DSI* DipoleShear SonicImager
DSI 2
Lecture Plan
Wave Propagation - Monopole & Dipole
Hardware Waveform Processing Operations
Applications
DSI 3
DSI* DipoleShear SonicImager
Wave Propagation
DSI 4
• Compressional:– Particle vibration parallel to direction of wave propagation
• Shear:– Particle vibration perpendicular to direction of wave propagation
Wave Propagation Modes
DSI 5
Wave Propagation Modes
• Slowness depends on rock mechanical properties:
– rock density– elastic dynamic constants
• Shear slowness:– stiffness of the rock
• Compressional slowness:– stiffness of the rock– compressibility
DSI 6
Wave Propagation Modes
• Fluid-saturated rocks, slowness depends on:
– amount and type of fluid– the makeup of the rock grains– degree of intergrain cementation
• Soft, loosely consolidated rocks:– generally less stiff and more compressible than hard rocks– sound waves travel slower in soft
rocks than in hard ones
• Fluids (completely unconsolidated rocks):
– have no stiffness at all– will not support shear wave propagation
DSI 7
• Stoneley:– Surface wave guided by the borehole– Travels slower than mud– Does not penetrate the formation– It’s energy concentrates on the bore-
hole surface– It’s amplitude exceeds that of other
waveforms– At low frequency there is little energy
decay by comparison to high frequency
Wave Propagation Modes
DSI 8
• Non-directional pressure source
• Pulse created in bore-hole & propagates into the formation
• Excites both P & S waveforms in the formation
• Head-waves are created in the mud & detected by the receivers
• Operates in the 10 Khz to 20 Khz range (Not suitable for Stoneley)
Monopole Source
DSI 9
Hard (Fast) Formation — Monopole
• Formation shear slowness less than mud compressional slowness
Vmud < Vshear
• Both the compressional and shear formation waves propagate along the borehole
• Energy leaks back into the borehole as headwaves, which are detected
Head waves
Fluid waveOmnidirectional source
Formation
Compressionalwave
Shearwave
Compressionalwave
Shearwave
Stoneleywave
Compressionalwave
Wellbore
DSI 10
Soft (Slow) Formation — Monopole
• Formation shear slowness greater than mud compressive slowness
Vmud > Vshear
• Snell’s Law predicts in slow formations the shear wave transmitted into the formation travels away from the borehole
•The shear headwave in the borehole is only marginally detectable or absent
• Shear curve is discontinuous when ‘slow’ zones are present, log is of limited value
Head wave
Fluid waveOmnidirectional source
Compressionalwave
Shearwave
Compressionalwave
Stoneleywave
Wellbore Formation
DSI 11
• Directional pressure source
• Pulse created on one side of the bore-hole causing a small amount of flexing. (Flexural Wave)
• Excites both P & S waveforms in the formation
• Flexural waves travel up the bore-hole & are detected by the directional receivers.
• Operates at low frequencies (~2.2 Khz)
Dipole Source
DSI 12
DSI Transducer - Dipole
• A dipole tool utilises a directional source and receivers
• The dipole source creates a pressure increase on one side of the hole and a decrease on the other
• This causes a small flexing of the borehole wall which directly excites compressional and shear waves in the formation
DSI 13
DSI Transducer - Dipole
• Propagation of this flexural wave is coaxial with the borehole
• Displacement is at right angles to the borehole axis and in line with the transducer
• Dipole has low operating frequencies, below 4 kHz where excitation of these waves is optimum
DSI 14
Soft (Slow) Formation - Dipole
• Compressional and shear waves radiate straight out into the formation
• An additional shear/flexural wave propagating up the borehole. It creates a "dipole-type” pressure disturbance in the borehole fluid
It is this pressure disturbance that the directional receivers detect
Wellbore
Flexural waveDirectional source
Formation Compressional
wave
Shearwave
Compressionalwave
Flexuralwave
Shearwave
DSI 15
Soft (Slow) Formation - Dipole
• The shear/flexural wave, initiated by the flexing action of the borehole, is dispersive
• At low frequencies it travels at the same speed as the shear wave; at higher frequencies it travels at a slower speed
• Unlike monopole-only tools, the dipole tool can record a shear/flexural wave even in slow formations
Wellbore
Flexural waveDirectional source
Formation Compressional
wave
Shearwave
Compressionalwave
Flexuralwave
Shearwave
DSI 16
• Shear/flexural wave is:– short in duration– concentrated at lower frequencies
• Additional higher-frequency compressional arrival
• In this typical slow formation example, there is a clear flexural wave from which the shear slowness is inferred
Compressionalwave
Flexuralwave
Shearwave
Dipole Waveforms - Slow Formation
DSI 17
Dipole Waveforms - Fast Formation
• Shear/flexural wave is:– long in duration– very dispersive
• Low frequency components, traveling near the shear slowness, become fairly well separated from the slower, higher frequency components
• Shear can often be detected and the formation shear slowness estimated directly from the waveforms
Shear Flexural Mode
DSI 18
DSI* DipoleShear SonicImager
Hardware
DSI 19
Monopole Compressional and
Dipole Shear measurements
provide Sonic data in hard and
soft formations
DSI-Dipole Shear Sonic Imager
DSI 20
• The borehole physics limitation of a
Monopole Sonic to acquire DT shear in
formations where DT shear > DT mud.
• Dipole Sonic acquisition overcomes this
limitation & DT formation >> DT mud
are acquired.
DSI vs DSLT
DSI 21
DSI Hardware
SPAC (Sonic Parallel Acquisition Cartridge)
Microprocessor controls:
• Digitizing• Stacking• Transmitting signals up-hole• Sending commands to the other tool
components via a dedicated serial link
DSI 22
SMDR• 8x receiver stations
• Each station has 2x hydrophone pairs:
– 1x oriented in line with the upper dipole transmitter (odd pair)– 1x oriented in line with the lower dipole transmitter (even pair)
• The outputs from each pair are:– Differenced for dipole reception– Summed for monopole reception
• Receivers are carefully matched during manufacture . Selectable filters and programmable amplifiers are also in the SMDR sonde.
DSI Hardware
DSI 23
DSI Hardware
SSIJ (Sonic Sonde Isolation Joint)
• Mechanical shock absorber to prevent:
– Direct acoustical tool arrivals from the transmitters– Reduces noises coming from below the receiver section
• Do not log with more than 900-
lbs.of weight below the SSIJ
• Do not log without the SSIJ
DSI 24
DSI HardwareSMDX• 3x transmitter elements:
– 1x omni-directional monopole, ceramic transducer– 2x unidirectional dipole transducers oriented perpendicular to each other
• Monopole transducer:– Low frequency pulse for Stoneley– High or low frequency pulse for compressional and shear
• Dipole transducers:– Standard frequency– Low frequency (for large borehole and very slow formations)
• All transducers can be fired at a rate of up to 15 Hz.
DSI 25
DSI Specifications
Temperature rating 350°F [175°C]
Pressure rating 20,000 psi [138 MPa]
Tool diameter 35/8 in. [92 cm]
Minimum hole size 51/2 in. [13.9 cm]
Maximum hole size 21 in. [53.3 cm]
Tool length 51 ft [15.5 m]
Maximum logging speed
One eight-waveform set 3600 ft/hr(single mode)
All six modes simultaneously 900 ft/hr(without BCR)
Digitizer precision 12 bits
Digitizer sampling interval limits Variable from 10 to 32,700 µsec per sample
Digitized waveform duration limits Up to 15,000 samples/ all waveforms
Acoustic bandwidth
Dipole and Stonely 80 Hz to 5 kHz
High-frequency monopole 8 to 30 kHz
Combinability All MAXIS tools, any resistivity tool
DSI 26
• Depths of investigation for sonic devices is a function of:
– formation type– shear and compressional slowness– transmitter-to-receiver – source frequency (wavelength)– etc
Depth of Investigation
DSI 27
DSI Hardware Versions: DSI-A
• CTS telemetry , TCC ( DTC/DTA ) +SPAC-A+SMDR-
A+SSIJ-B+SMDX-A
• DSST-A is obsolete; its production started in August 1990 and
stopped in July 1995. There will be no support for DSST-A in OP
9.2 and later OP versions. SKK recommends that you upgrade all
your current SPAC-A tools to the SPAC-B version
DSI 28
DSI Hardware Versions: DSI-B
• DTS telemetry , DTC-A/H +SPAC-B+SMDR-A+SSIJ-
B+SMDX-A
• DSST-B production started in July 1995. The SMDR-AA
receiver sonde is also going to become obsolete soon. SKK
recommends that you upgrade all your current SMDR-A sondes
to the SMDR-BD/BE version.
DSI 29
DSI Hardware Versions: DSI-II (DSI-Plus)
• Enhances the measurement quality & improves
tool reliability. • Enhances shear slowness measurement by
improving waveform amplitude• The SMDR receiver array has been redesigned
to achieve these improvements • To implement the upgrade of DSI to DSI-II,
SMDR-AA MR-2 & SSIJ-BA MR-2 is needed.• These are mandatory modifications that must
be implemented only by trained and qualified
personnel• The SMDR-AA becomes SMDR-BD
DSI 30
DSI Hardware Versions: S-DSI
• DSI logs run in slow formations with the standard DSI
sleeve result in a strong sleeve arrival in the data.
• Do not run the standard SMDR slotted sleeve in
formations slower than 500 us/ft.
• When in doubt about DTs & when logging surface
formations, use S-DSI and not DSI-II (DSI Plus).
• S-DSI uses a slow-formation sleeve that replaces the
standard SMDR sleeve to extend the range of DSI-II dipole
slowness measurement from 500 usec/ft to 1200 usec/ft.
• To implement the upgrade of DSI-II to S-DSI a Slotted
Sleeve is required, which is SMDR-BD MR-3 (optional).
• The slotted sleeve is intended for use only with DSI-II
tools.
DSI 31
DSI Operating Limits
DSI 32
DSI Hardware Versions: BARS
• DSST-C ( BARS )
• DTS telemetry , DTC-A/H +SPAC-B+SMDR-C+SSIJ-
B+SMDX-A
• DSST-C is available in OP 9.1 and later version as an experimental
tool for BARS (Borehole Acoustic Reflection Survey) operations.
SMDR-C is identical in every aspect to the SMDR-B with the exception
of its PGA board;
DSI 33
DSI* DipoleShear SonicImager
Waveform Processing
DSI 34
DSI Acquisition & Processing
• Acquisition: Waveforms of the acquired modes, one for the Rx & one (optionally) for the Tx are built into sets.
• STC (Slowness Time Coherence): Rx & Tx waveform sets are processed to identify coherent arrivals.
• Labelling: Detects the desired arrival from among the peaks identified by STC.
DSI 35
STC Computation - 1 Array Waveforms
STC - Slowness-time-coherence processing
DSI 36
STC Computation - 2 Contour Plot
DSI 37
Poisson's Ratio
.25 .50Gamma Ray
Caliper
6 16
0 100
Delta-T Comp.
100 200Delta-T Shear
0 1. 1. 0
100 500Dtc Coherence Dts
10200
10250
10300
10350
Slowness Time PlaneProjection
Labeling
DSI 38
Dipole Waveforms - Bias Correction
• Bias correction is small for fast formations and averages about 5 percent in slow formations
Shear Flexural Mode
Flexural ModeShear
Flexureslowness
Shearslowness
BiasCorrection
DSI 39
10250
Dipole Waveforms - Bias Correction
• One of the coherence peaks will correspond to the dispersive flexural mode
• The slowness of this peak is always greater (slower) than the true shear slowness
• In fast formations a low-frequency band pass filter usually produces a coherence peak very close to the true shear slowness
• In slow formations the formation shear must be estimated from the flexural data
DSI 40
10250
Dipole Waveforms - Bias Correction• Low-frequency source tends to minimize the dispersion
• Some correction is still needed to obtain the true formation shear
• A precomputed correction, derived using data generated from numerical modeling, is included in the processing to correct for the bias caused by flexural wave dispersion
• Amount of correction depends on:– the acoustic response signature of the source– the STC filter characteristics– the borehole size– shear slowness
DSI 41
10250
Dipole Waveforms - Bias Correction
• Bias correction is small for fast formations and averages about 5 percent in slow formations
DSI 42
DFMD - Digital First Motion Detection
• Amplitude threshold-crossing
times derived in the cartridge for
each receiver waveform
• Input into Identification and
tracking algorithm
• Algorithm selects crossing time
the one on each waveform that
corresponds to first motion, and
tracks it over depth
DSI 44
DSI* DipoleShear SonicImager
Environment
DSI 45
DDBHC = average (RA & TA)
RA - Receiver array– derived from one tool position
TA - pseudo-transmitter array– derived from several tool positions
DSI Borehole Compensation
DSI 46
SAM 1 & 2 (Dipole) - RA only
SAM 3 (Stoneley) - RA only
SAM 4 (P&S) - DDBHC
SAM 5 (DFMD) - N/A
SAM X (Expert) - N/A
Note:There is no theoretical basis for borehole compensation for the Stoneley mode or for the dipole modes
DSI Borehole Compensation
DSI 47
Road Noise
• Cause: contact between centralisers / standoffs and borehole wall
• Use correct method and placement of centralisation
• Reduce OD of CME-Z close to BS to reduce road noise
• New LCME-A (CME-Y) shows similar order of noise as CME-Z’s
MST - Monopole Stoneley
LDP - Lower Dipole
CME-Y new centralizer
LCME-A
DSI 48
DSI* DipoleShear SonicImager
Tool Maintenance
DSI 49
Air Volume Check Procedure
DSI 50
DSI* DipoleShear SonicImager
Applications
DSI 51
• Mechanical property analysis
— sanding analysis
— fracture height
— wellbore stability
• Formation evaluation
— gas detection
— fractures
— permeability
• Geophysical interpretation
— synthetic seismograms
— VSP
— AVO
• Formation Shear Anisotropy
Applications
DSI 67
Summary
• The DSST tool has advantages over the previous sonic tools like SDT
• It utilises both Dipole and Monopole transducers
• The dipole capability allows the tool to measure the shear slowness in
typical slow or unconsolidated formations to overcome the limitation of
monopole
Remember:– Always use DSI job planner and understand why the job is being run– Always run the tool well-centred and under the recommended logging speed limit– Never run the tool without SSIJ– Run DSST with GPIT for BCR mode