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DSI 1 DSI* Dipole Shear Sonic Imager

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Page 1: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

DSI 1

DSI* DipoleShear SonicImager

Page 2: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

DSI 2

Lecture Plan

Wave Propagation - Monopole & Dipole

Hardware Waveform Processing Operations

Applications

Page 3: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

DSI 3

DSI* DipoleShear SonicImager

Wave Propagation

Page 4: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

DSI 4

• Compressional:– Particle vibration parallel to direction of wave propagation

• Shear:– Particle vibration perpendicular to direction of wave propagation

Wave Propagation Modes

Page 5: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 6: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 7: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 8: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 9: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 10: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 11: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 12: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 13: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 14: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 15: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 16: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 17: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 18: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

DSI 18

DSI* DipoleShear SonicImager

Hardware

Page 19: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

DSI 19

Monopole Compressional and

Dipole Shear measurements

provide Sonic data in hard and

soft formations

DSI-Dipole Shear Sonic Imager

Page 20: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 21: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 22: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 23: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 24: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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.

Page 25: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 26: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 27: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 28: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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.

Page 29: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 30: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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.

Page 31: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

DSI 31

DSI Operating Limits

Page 32: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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;

Page 33: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

DSI 33

DSI* DipoleShear SonicImager

Waveform Processing

Page 34: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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.

Page 35: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

DSI 35

STC Computation - 1 Array Waveforms

STC - Slowness-time-coherence processing

Page 36: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

DSI 36

STC Computation - 2 Contour Plot

Page 37: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 38: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 39: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 40: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 41: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

DSI 41

10250

Dipole Waveforms - Bias Correction

• Bias correction is small for fast formations and averages about 5 percent in slow formations

Page 42: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 43: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

DSI 44

DSI* DipoleShear SonicImager

Environment

Page 44: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 45: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 46: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

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

Page 47: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

DSI 48

DSI* DipoleShear SonicImager

Tool Maintenance

Page 48: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

DSI 49

Air Volume Check Procedure

Page 49: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä Applications

DSI 50

DSI* DipoleShear SonicImager

Applications

Page 50: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä 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

Page 51: DSI 1 DSI* Dipole Shear Sonic Imager. DSI 2 Lecture Plan ä Wave Propagation - Monopole & Dipole ä Hardware ä Waveform Processing ä Operations ä 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