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Dielectric ScannerMultifrequency dielectric dispersion service

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RA4

RA3

RA2

RA1

PA

PB

TA

TB

RB1

RB2

RB3

RB4

Measurements that speak volumes

Dielectric Scanner service is the first in the industry to employ

multifrequency dielectric dispersion science to accurately quantify

residual hydrocarbon volume, the Archie mn  exponent, and

formation CEC. Parameters available previously only through core

analysis or estimation are now delivered as continuous logs at the

wellsite. The dielectric dispersion measurement constructs an

accurate radial profile of the close-borehole region, providing new

and unique information on rock properties and fluid distribution for

advanced petrophysical interpretation. Used in conjunction with

 traditional logging measurements, Dielectric Scanner dielectric

dispersion measurement enables developing a more accurate

reservoir description for reservoir evaluation and management.

Multispacing Operation

The heart of Dielectric Scanner service lies in its short, multispac-

ing antenna array pad. Each of the cross-dipole antennas has

collocated magnetic dipoles. The transmitters (TA and TB) are in the

center and the receivers (RA1–4 and RB1–4) are placed symmetri-

cally around them for optimal measurement accuracy and borehole

compensation. To minimize environmental effects, the short, fully

articulated antenna pad is applied firmly against the borehole wall

by a hydraulically operated eccentering caliper to enable optimal

pad contact, even in rugose boreholes. Electromagnetic waves are

propagated into the formation at four frequencies and two polariza-

 tions for high-resolution, high-accuracy measurements of reservoir

properties at up to 4 in from the borehole wall.

The conventional approach to determining oil volumerequires weeks or months for laboratory core analysis or

accepting the uncertainty inherent in estimated Archie

parameters. With Dielectric Scanner* measurements

direct from your reservoir, the wait for accurate formation

evaluation answers is over.

APPLICATIONS■  Direct measurement of water volume

independent of water resistivity (R w ) at

a depth of investigation to 4 in [10 cm],

solving for

•  Residual hydrocarbon volume in

produced reservoirs

•  Hydrocarbon volume in low-resistivity

or low-contrast shaly and laminated

sand formations

•  Hydrocarbon volume and mobility in

heavy oil reservoirs

•  Water salinity

■  Continuous Archie mn  exponent log from

rock texture measurements in carbonates

for determining saturations beyond the

invaded zone

■  Cation exchange capacity (CEC) to account

for effect of clay volume in siliciclastics

■  High-resolution water-filled porosity for

 thin-bed analysis

Dielectric Scanner pad antenna con- figuration. The blue dipoles define thelongitudinal polarization and the redones are the transverse polarization.The two coaxial electrical probes(P A and P B ) are used for quality controlof pad application and for determiningthe mud and mudcake dielectric proper- ties at the frequencies of interest.

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One of the revolutionary advances provided by

 the Dielectric Scanner tool is the continuous

measurement of dielectric dispersion, which is

 the variation of formation dielectric properties

as a function of the frequency. High-resolution

measurements obtained with the different

array spacings, each with two polarizations

at four frequencies, are radially interpreted

 to obtain permittivity and conductivity at each

frequency. Conventional dielectric tools make

only a single-frequency measurement with

limited applications, and its interpretation can-

not account for textural effects, invasion, and

unknown or variable water salinities.

The Dielectric Scanner permittivity and con-

ductivity measurements at each frequency are

interpreted using a petrophysical model. The

output parameters of the model are water-filled porosity (hence water saturation if the

 total porosity is known), water salinity, and

 textural effects in carbonates or CEC in shaly

sands. Simultaneously fitting the permittivity

and conductivity dispersions frees the water-

filled porosity from salinity effects. Rather,

water salinity is an additional output of the

analysis. For a well drilled with oil-base mud

(OBM), the calculated water salinity is the

formation water salinity.

In carbonate reservoirs, the dielectric disper-

sion is driven mainly by the rock texture. In

 turn, Dielectric Scanner analysis provides a

continuous in situ measurement of rock tex-

 ture, presented as an mn  exponent log.

In shaly sand reservoirs, processing provides

a continuous log of the CEC. In heavy oil

reservoirs or in shallow-invasion situations,

Dielectric Scanner measurements are made

in both the invaded and non-invaded zones,

 to determine moveable hydrocarbon content.

Previous-generation single-frequency electromagnetic propa- gation tools, emulated in the log onthe left by single-frequency pro- cessing, cannot account for texturavariation, resulting in the overesti- mation of invaded zone resistivityRxo (Track 2). In the log on theright, Dielectric Scanner multifre- quency mixing analysis correctlymatches the water-filled porosityto the total porosity in this water- filled sand in Track 3, as confirmedby the matching Rxo values of theDielectric Scanner and resistivitytools in Track 2.

Dielectric dispersion science

Dispersion plots of the measured permittivity andconductivity at four frequencies and the fit to thepetrophysical model with the estimated parameters.

X,050

X,100

X,150

X,200

X,300

X,350

X,400

X,450

X,550

X,600

X,000

X,500

X,250

i i i

  I i

i i i

..

.

.

I i i i

.

i l iI i i i

.

i

l i

i l i

i ll i

..

li i

i l i

li i

Resistivity

2-ft Array Induction

Resistivity A90

ohm.m0.2 2,000

0.2 2,000

0.2 2,000

Invaded Zone Resistivity

ohm.m

Dielectric ScannerInvaded Zone Resistivity

ohm.m

Porosity

Hydrocarbon

Total Porosity

y.yx.x ft3 /ft3

Dielectric Scanner

Water-Filled Porosity

Salinity

Dielectric

Scanner

Salinity

ppt0 100..

y.yx.x ft3 /ft3

X,050

X,100

X,150

X,200

X,300

X,350

X,400

X,450

X,550

X,600

X,000

X,500

X,250

Resistivity

2-ft Array Induction

Resistivity A90

ohm.m0.2 2,000

0.2 2,000

0.2 2,000

Invaded Zone Resistivity

ohm.m

Dielectric ScannerInvaded Zone Resistivity

ohm.m

Porosity

Hydrocarbon

Total Porosity

Dielectric Scanner

Water-Filled Porosity

y.yx.x ft3 /ft3

Salinity

Dielectric

Scanner

Salinity

ppt0 100

i i i

  I i

i i i

..

.

.

I i i i

.

i l iI i i i

.

i

l i

..

i l i

i ll i

y.yx.x ft3 /ft3

..

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An operator in the Middle East wanted to

improve understanding of the fluid saturations

in a high-porosity carbonate reservoir where

variability in the Archie m  and n  exponents

increased the uncertainty in conventional log

interpretation. The measurements were also

ambiguous because the mud filtrate salinity

was approximately 180,000-ppm [-ug/g] NaCl.

The carbonate textural information provided by Dielectric Scanner service enabled accurate

mn  determination instead of relying on potentially incorrect estimations from conventional log

analysis or waiting for laboratory core analysis. Having accurate values of the Archie exponents

is important because they are the basis for calculating saturation values from resistivity.

As shown by the porosity curves in Track 5, the significant difference between Dielectric Scanner

water-filled porosity (blue curve) and the total porosity calculated from standard porosity

measurements indicates a large volume of residual hydrocarbon in the formation. In Track 2 the

Dielectric Scanner hydrocarbon saturation accounts for variation in the Archie exponents across

 the reservoir and confirms up to 95% residual hydrocarbon. Conventional saturation determination

using constant values of the Archie mn  exponents does not account for their variation, as shown by

 the difference shaded red where the conventional and Dielectric Scanner residual oil saturations do

not match. Confirmation of the high residual saturation is in Track 4, where the R xo  measurements

from Dielectric Scanner and conventional resistivity logging closely match each other.

Dielectric Scanner measurements confirm

95% residual hydrocarbon saturation

It Speaks Volumes about Carbonates

Accurate hydrocarbon volume in carbonates from salinity-insensitive

determination of water-filled porosity and rock texture factors

Case studies

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Confirmation of 95% residual hydrocarbonby Rxo match. The Rxo curve fromDielectric Scanner service in thecarbonate reservoir agrees closely withthe conventional Rxo measurement inTrack 4, supporting the determinationof 95% residual hydrocarbon saturation.

X10

X20

X30

X40

X50

Illite (dry)

Lithology

0 10

Epsilon Matrix

from Lithology

1 3.5

Archie mn 

0 ft3 /ft3 1

Dielectric

Scanner

Oil

Residual Oil

Saturation

1 m3 /m3

Depth, m

0

Porosity

0 ft3 /ft3 1

Archie

Difference

Bound Water

Oil

Water

0.2 ohm.m 2,000

HRLA* True Resistivity

0.5 m3 /m3 0

Dielectric Scanner Water-Filled Porosity

Freq. 0 –

Freq. 1

Freq. 2 –

Freq. 3

Freq. 2 –

Freq. 1

Freq. 1 –

Freq. 2

Freq. 3 –

Freq. 2

Freq. 0 –

Freq. 1

Permittivity

Dispersion Image

Conductivity

0.5 m3 /m3 0

ELAN* Total Porosity

Hydrocarbon

Porosity

0.2 ohm.m 2,000

Dielectric Scanner Invaded Zone Resistivity

0.2 ohm.m 2,000

Invaded Zone Resistivity

0.2 ohm.m 2,000

Array Laterolog Resistivity

Resistivity

6 in 16

Caliper

Calcite

Dolomite

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The production potential of a laminated reservoir in the Orinoco belt of Venezuela could not be

fully determined with conventional logs. Thinly bedded shale and sand layers decreased resistiv-

ity measurements, masking pay zones and resulting in pessimistic interpretations of hydrocarbon

volume. In this heavy oil reservoir, NMR logs measured a reduced apparent formation porosity,

which in turn adversely affected fluid saturation determinations.

An additional complication was the highly rugose borehole, as shown by the caliper in Track 1,

but the pad of the Dielectric Scanner tool maintained good contact with the formation, and the

measurements were not compromised. The high resistivity in Track 5 in the oil-bearing interval

from approximately X,430 to X,500 ft had been observed in other wells in the area. However, resis

 tivity values below this interval are uniformly low. Similarly, the NMR log in Track 7 has a strongoil signature in the upper interval, but the apparent porosity is reduced with increasing depth.

The Dielectric Scanner log dispelled uncertainty about the reservoir quality of the lower interval,

revealing moveable oil over a 150-ft section, from X,560 to X,650 ft and again from X,690 to X,720 ft

Sidewall samples confirmed the Dielectric Scanner measurements.

Thin Beds

It Speaks Volumes about Thin Beds

High-resolution water-filled porosity and radial profiling delivered by

multifrequency measurements without the errors introduced through

 the estimation of Archie formation factors

Additional 150 ft of pay revealed by

Dielectric Scanner dispersion measurements

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Because the formation water salinity and resistivity vary in heavy oil reservoirs with thin-beddedshaly sections, Canadian operators had to wait several months for the results of Dean Stark

core analysis. Without the analysis results to adjust conventional saturation calculations, using

a constant R w  value led to errors in the water saturation determined for uncored intervals.

With water-filled porosity calculated from Dielectric Scanner dispersion measurements, the

weight percent of bitumen is accurately determined months in advance of laboratory core

analysis turnaround. The operators can confidently consider a reduction in coring frequency

and number of analysis points in their multiwell projects.

Accurate answers quickly. Water saturation and hydrocarbon volume calculated from Dielectric Scanner dispersion measurements provide higher resolution, moreaccurate answers than those derived from the Archie equation or nuclear magnetic resonance (NMR) data.

Weight percent bitumen quickly, accurately

determined in Canadian oil sands

High-ResolutionGamma Ray

  0 gAPI

Caliper

  125 mm

Washout

m

Depth, 90-in AIT Resistivity

  0.2 ohm.m

Archie Water Saturation

  0 1

  0 1

Wt% Oil Dielectric Scanner

Core Wt% Oil

%

Wt% Oil Archie

NMR Water Saturation %

NMR Wt% Oil

Dielectric Scanner Wt% O

Core Wt% Oil

X75

Y00

Y25

ms

  0.3

Density Porosity (Sand)m3 /m30.5 0

0.5 0

0.5 0

0.5 0

Neutron Porosity (Sand)m3 /m3

Total Porositym3 /m3

Dielectric Scanner Water-Filled Porosity (Sand)

m3 /m3

Gas HydrocarbonHydrocarbon

Dielectric ScannerWater Saturation

m3 /m3

m3 /m3

m3 /m3

2,000

375

150

T 2 Distribution

m3 /m30 0.3

1

0

00

00

0

m3 /m3 10

0 0.2

0 0.2

0 0.2

T 2 Cutoff

ms 3000

Dielectric ScannerWater Saturation

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Heavy oil saturation and mobility from high-resolution measurements

insensitive to oil viscosity and formation water resistivity

It Speaks Volumes about Heavy Oil

High vertical resolution. The high-resolution weight percent bitumen calculated from Dielectric Scanner measurements shows excellent agreement to thesubsequent core analysis results in Track 4, even in the thin shale intervals identified in the core photograph by the lighter colors within the black bitumen-rich core. IHS = inclined heterolithic stratification.

Total Porosityv/v

X75

Y00

Y25

Core Wt% Oil

%

CorePhotograph

High-ResolutionStatic FMI*

Image

High-ResolutionGamma Ray

  0 gAPI

Caliper

  125 mm

Washout Depth,m

90-in AIT Resistivity

  0.2 ohm.m 2,000

375

150

Neutron Porositym3 /m3

Density Porosity (Sand)m3 /m3

Dielectric Scanner Water-Filled Porosity (Sand)

m3 /m3

m3 /m3

High-Resolution Wt% OilDielectric Scanner

High-Resolution

WaterSaturationDielectricScanner

High-Resolution

WaterSaturation

Image

0.5 0

0.5 0

0.5 0

0

  0 1

0.2

0 0.2

0.5 0

Dielectric ScannerWater Saturation

  1 1:20

Depth,

mFacies

X74

X75

X76

X77

X78

X79

X80

X81

X82

Fine

Sand

Muddy

IHS

IHS

Fine

Sand

Sandy

IHS

IHS

Medium

Sand

Core Photograph

0m3 /m3

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Washed-out borehole intervals in a heavy oil reservoir in Cymric field, California, USA, were

adversely affecting logging. Washouts caused separation in the resistivity curves that could

be confused with invasion, as shown at 700 and 745 ft in Track 2. Water-filled porosity measure-

ments made with a conventional, mandrel-type, single-frequency electromagnetic propagation

 tool were suspect because the tool would not have been able to maintain good contact in these

rugose conditions.

Porosity and saturation calculated from Dielectric Scanner measurements in Tracks 5 and 3,

respectively, correct the previous washout-impaired porosity, as confirmed by sidewall core

analysis (black dots). With accurate porosity values, the pessimistically high water saturation

value was corrected by 23%.

Overlooked pay found in washed-out

zones in heavy oil reservoir

Caliper

in

Resistivity

Standoff

Resistivity

Standoff

DensityStandoff

Density

Standoff

Depth, ft

500

600

700

800

8.5   18.5

2-ft Array Induction

Resistivity A90   Residual Hydrocarbon

Hydrocarbon

Residual Hydrocarbon Residual Hydrocarbon

Quartz

Clay

Carbonate

IrreducibleWater Volume

Clay-Bound

Water Volume

ohm.m0.5   5,000

Invaded Zone

Resistivity

ohm.m0.5   5,000

Core Water Saturation

ft3 /ft30   1

Dielectric Scanner

Water Saturation

ft3 /ft31   0

Total Porosity

ft3 /ft3

ft3 /ft3

0.5   0

Electromagnetic

Propagation Porosity

ft3 /ft30.5   0

Dielectric Scanner

Water-Filled Porosity

ft3 /ft30.5   0

Core Porosity

ft3 /ft30.5   0

Dielectric Scanner

Water-Filled Porosity

0.5   0   ft3 /ft3

Total Porosity

0.5   0

Dielectric Scanner

Water Saturation

ft3 /ft30   1

Dielectric Scanner

Invaded Zone Resistivity

ohm.m0.5   5,000

in

2.5

0

in

2.5

0

Accurate resistivity and porosity measurements ina washed-out borehole. The articulated pad of theDielectric Scanner tool is not affected by rugose holeconditions and obtained the actual Rxo measurement,proving that the difference between the other tworesistivity curves in Track 2 was not caused by inva- sion. Similarly, the Dielectric Scanner porosity inTrack 5 accurately measured water-filled porosityacross washed-out intervals, unlike the previous- generation mandrel tool.

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Dielectric Pro* software provides quality control and advanced

interpretation for Dielectric Scanner service. After preprocessing

and applying quality control to the raw data, Dielectric Pro software

performs a robust radial interpretation of the different spacing and

polarization measurements to provide the dielectric dispersion data.

A multimineral analysis for lithology and porosity that integrates

measurements from different tools is performed in the same applica-

 tion to determine the total porosity and formation matrix permittivity.

These outputs are used together with the dielectric dispersion in a

final interpretation step, in which petrophysical models determine

water-filled porosity, water salinity, and textural parameters.

Following a carefully engineered, efficient workflow, Dielectric Pro

software delivers reliable petrophysical answers for complex envi-

ronments in minimum time.

Pore-fluid analysis

■  High-resolution residual saturation and invaded zone water salinity

■  Hydrocarbon saturation profile in heavy oil reservoirs or shallow

invasion environmentsMatrix analysis

■  Carbonates: mn  log for cementation exponent estimation

■  Shaly sands: high-resolution CEC for clay content

Structural analysis

■  Thin-bed analysis

■  Structural anisotropy in very thin beds

Picture to come

Dielectric Scanner interpretation and quality control software

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www.slb.com/ds

*Mark of Schlumberger

Other company, product, and service names are the properties

of their respective owners.

Copyright © 2013 Schlumberger. All rights reserved. 13-FE-0010

Dielectric Scanner

Specifications

Output Relative dielectric permittivity and conductivity at four frequenci

Logging speed 3,600 ft/h [1,097 m/h]

Vertical resolution† 1 in [2.5 cm]

Depth of investigation 1 to 4 in [2.5 to 10 cm]

Accuracy at the highest frequency Corresponding to 0.002-ft3 /ft3 [0.002-m3 /m3] water-filled porositPermittivity: ±1% or ±0.1Conductivity: ±1% or ±5 mS

Range of measurements at the highest frequency Permittivity: 1 to 100Conductivity: 0.1 to 3,000 mS

Combinability Platform Express* integrated wireline logging toolMost openhole tools

Max. temperature 350 degF [177 degC]

Max. pressure 25,000 psi [172 MPa]

Outside diameter 4.77 in [12.12 cm]

Borehole size—min. 5.5 in [14 cm]

Borehole size—max. 22.0 in [55.9 cm]

Minimum restriction 5.25 in [13.3 cm]

Borehole fluid Both water- and oil-base muds‡

Length 11.27 ft [3.44 m]

Weight 262 lbm [119 kg]

Max. tension 50,000 lbf [222,411 N]

Max. compression§ 4,400 lbf [19,572 N]

Conveyance Wireline, TLC* tough logging conditions system, or tractor† 1 in depending on frequency‡

Oil-base mud under specific conditions; contact your Schlumberger representative§ 8,000 lbf [35,586 N] with TLC stiffener kit