Exploring the Subsalt - Schlumberger/media/Files/resources/oilfield_review/ors96/... · Exploring...
Transcript of Exploring the Subsalt - Schlumberger/media/Files/resources/oilfield_review/ors96/... · Exploring...
50 Oilfield Review
From the earliest days of exploration,prospectors associated salt with oil andgas—but not always for the right reasons. Inthe 1920s, so many successful wells weredrilled around salt domes that logging meth-ods were tuned to identify the high-salinitywater in formations overlying pay zones.1By 1923, gravity and seismic methodsbecame successful in spotting salt domes,and the industry was on its way to under-standing the structural role played by salt.Today, interpreters can view and tour saltstructures with the help of powerful graph-ics workstations (next page, top).
Salt is one of the most effective agents innature for trapping oil and gas: as a ductilematerial, it can move and deform surround-ing sediments, creating traps; salt is alsoimpermeable to hydrocarbons and acts as a
For help in preparation of this article, thanks to MarkBogaards, Cliff Kelly and Mark Puckett, Wireline & Test-ing, Houston, Texas, USA; Bob Godfrey, Colin Hulme,Tore Karlsson, Jane Lam, Dominique Pajot, John Ulloand Öz Yilmaz, Geco-Prakla, Gatwick, England; George Jamieson, Geco-Prakla, Houston, Texas; and Ron Roberts, Amoco, Denver, Colorado, USA.
Paul FarmerGatwick, England
Douglas MillerRidgefield, Connecticut, USA
Andy PieprzakJeff Rutledge Richard WoodsHouston, Texas, USA
Exploring the Subsalt
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30°
0°
30°
nDistribution of offshore salt sheets. [Adapted from Ward RW, MacKay S, Greenlee SMand Dengo CA: “Imaging Sediments Under Salt: Where are We?” The Leading Edge 13,no. 8 (August 1994): 834.]
Advances in seismic imaging have changed the way explorationists
view salt bodies. Once seen as impenetrable barriers to geophysical
probing with some flanking pay zones, many salt structures are now
proving to be thin blankets shielding rich reserves. Geophysicists are
developing new methods to see through salt, illuminating the reservoirs
below. This new vision of subsalt is impacting E&P decisions from well
planning and drilling to field delineation and development.
1. Allaud LA and Martin MH: Schlumberger The Historyof a Technique. New York, New York, USA: JohnWiley & Sons (1977): 68-69.
2. Western PG and Ball GJ: “3D Prestack Depth Migra-tion in the Gulf of Suez: A Case Study,” GeophysicalProspecting 40 (1992): 379-402.
Charisma seismic interpretation system, KUDOS 3Dvelocity modeling system, and SALTBOND cement sys-tem are marks of Schlumberger. CM-5 is a mark ofThinking Machines Corporation. GeoDepth is a mark ofParadigm Geophysical. InDepth is a mark of WesternGeophysical.
51Spring 1996
nFlying through a seismic interpretation. The top of a salt feature (yellow surface) has been interpreted on a seismic workstation. Alsoshown is a panel of seismic data (background), a reflector above the salt (brown surface), seismic velocities at vertical well locations(multicolored vertical logs) and deviated well trajectories (blue lines).
Passive—No Space Problem
Active—Diapir Creates Space
Reactive—Extension Creates Space
Thinning,arching
Radial orsubparallelfaults
Fan ofnormalfaults
nStyles of salt intru-sion. When the over-lying sediments offerlittle resistance (top),salt can rise, oftendragging flankinglayers up with it. Ifthe overburden doesresist, salt pressuredfrom below (middle)can still pushthrough, doming theoverburden and cre-ating radial faults inthe process. In thecase of regionalextension (bottom)faulting in the rigidoverburden can openthe way for salt torise. [Adapted fromJackson MPA, Vendev-ille BC and Schultz-ElaDD: “Salt-Related Struc-tures in the Gulf ofMexico: A Field Guidefor Geophysicists,” TheLeading Edge 13, no. 8(August 1994): 837.]
seal. Most of the hydrocarbons in NorthAmerica are trapped in salt-related struc-tures, as are significant amounts in other oilprovinces around the world (previous page).Many reservoirs in the North Sea are belowsalt, as are large fields in the Gulf of Suez.2
A product of seawater evaporation, saltaccumulation can reach thousands of feet inthickness. Salt retains a low density of2.1g/cm3 even after burial. However, the sur-rounding sediments compact and at somedepth become denser than the salt—anunstable situation. If the overlying sedimentsoffer little resistance, as is sometimes thecase in the Gulf of Mexico, the salt rises, cre-ating characteristic domes, pillows andwedges that truncate upturned sedimentarylayers (right). If the overburden does resist,salt can still push through, creating faults inthe process. If tectonic conditions are right,extensional faulting in the rigid overburdencan open the way for salt ascent. Much ofthe Zechstein salt pervasive in the North Seahas been mobilized this way.
In contrast to salt’s low density is its highseismic wave velocity—4400 m/sec (14,432ft/sec)—often more than twice that of sur-rounding sediments. The strong velocitycontrast at the sediment-salt interface actslike an irregularly shaped lens, refracting and
reflecting seismic energy. Early data process-ing techniques treated this contrast like amirror, resulting in images that portrayed saltfeatures as bottomless diapirs extending tothe deepest level of seismic data (left). In the1980s, seismic processing began to correctlyimage the steeply dipping and sometimesoverhanging faces of salt where hydrocar-bons could accumulate.
But in the last five years, a new image ofsalt has emerged. In some areas, not only isthe top of salt clearly visible, but the bottomalso. Geologists hypothesize that in theseareas of allocthonous salt—found awayfrom its original depositional position—con-ditions allow the salt, having reached verti-cal equilibrium, to begin flowing horizon-tally (above). In the Gulf of Mexico, thisoccurs mainly in deep water beyond thecontinental shelf, where sediment cover isnot as thick as it is near shore (bottom left).Wells drilled through thin salt sheets haveencountered oil-bearing sediments below.
However, knowledge of the existence ofhydrocarbons below salt is insufficient rea-son to start drilling. Drilling salt is risky (see“Drilling and Completions Through Salt,”page 54). The salt itself is weak and under-goes continuous deformation. Belowintruded salt, sediment layers are often dis-rupted and overpressured. And most impor-tant, unless seismic data have been pro-cessed to image through the salt, theposition of the target is unknown.
52 Oilfield Review
nEarly imaging results around salt. Seismic data processing resulted in images of bot-tomless salt diapirs (left). Enhancements in processing began to correctly image thesteeply dipping and sometimes overhanging faces of salt (right). [Reprinted with permis-sion from Ratcliff DW, Gray SH and Whitmore ND: “Seismic Imaging of Salt Structures in theGulf of Mexico,” The Leading Edge 11, no. 4 (April 1992): 15 and 22.]
Houston
Lake Charles
New Orleans
Enchilada
Mahogany
Teak Gemini
MickeyMouse
DiscoveryPlugged and abandonedSalt sheets
nSalt sheets mapped in the Gulf of Mexico. Recent exploration wells correspond to wells mentioned in table (next page).
1 2 3 4
Evolution of a Salt Wall
1 2 3 4
Evolution of a Salt Diapir
nEvolution of salt intrusions. Salt walls and diapirs are initiated at instabilities on extensive salt layers. As the salt rises and thenflows horizontally, the walls and diapirs change shape. Eventually some salt features become completely detached from the parentsalt layer.
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A few operators have announced signifi-cant oil discoveries beneath salt in the Gulfof Mexico, rekindling a spirit of explorationin the Gulf. Phillips Petroleum Company, inpartnership with Anadarko Petroleum Cor-poration and Amoco Production Company,announced the first commercial Gulf ofMexico subsalt discovery with theMahogany prospect in 1993, and attributedthe success to the imaging technique calledprestack depth migration.3 Drilled in 375 ft[114 m] of water to a depth of 16,500 ft[5030 m], the well produces from sedimentlayers beneath a salt sheet 3000 to 8000 ft[915 to 2439 m] thick.
Since the Mahogany find, many morewells have been drilled in the area, withother operators experiencing similar suc-cess (left). Before prestack depth migration,the success ratio in the subsalt play wasaround 5%. The new technique is increas-ing that to 25%. Depth migration is alsobringing first-time details to light in some ofthe many North Sea reservoirs that producefrom below salt, and operators plan explo-ration campaigns in the Red Sea using thesame method.4
What is this imaging technique and howdoes it help illuminate subsalt reservoirs? Theanswers are found in a review of the familyof imaging methods, including prestackdepth migration, that are bringing subsaltand other complex structures to light.5
53Spring 1996
3. Westcott ME, Leach MC, Wyatt KD, Valasek PA andBranham KL: “Mahogany: Seismic Technology Lead-ing to the First Economic Subsalt Field,” ExpandedAbstracts, 65th SEG International Meeting and Exposi-tion, Houston, Texas, USA (October 8-13, 1995):1161-1164.
4. Salpukas A: “Anadarko Planning to Drill in Red SeaUsing Computers,” New York Times, September 29,1995.
5. For more on subsalt imaging topics: The Leading Edge13, no. 8 (August 1994).
Subsalt Scorecard in January 1996
Mickey MouseMississippiCanyon 211
Prospect
MahoganyShip Shoal 349
Amoco 1South MarshIsland 169
MesquiteVermillion 349
Ship Shoal 250
TeakSouth TimbalierAddition 260
Ship Shoal 360
Ship Shoal 368
South Timbalier 289
Exxon andConoco
Operators/Partners
Phillips, Anadarkoand Amoco
Amoco
Phillipsand Anadarko
Japex and Vastar
Anadarko(originally withPhillips)
Unocaland Conoco
Amerada Hessand Shell
Consolidated Natural Gas andLouisiana Land & Exploration
Noncommercialdiscovery
Result
Commercialdiscovery
Dry hole
Dry hole
Dry hole
Potentiallycommercialdiscovery
Pluggedand abandoned
Dry hole
Dry hole
1991
Date
1993
1993
1994
1994
1994
1994
1994
1994
EnchiladaGarden Bank 128
South AnaVermillion 308
Garden Banks 119
AlexandriteShip Shoal 337
MonaziteVermillion 375
AgateShip Shoal 361
South Timbalier 231
North LobsterSouth Timbalier 308
GeminiMississippiCanyon 292
No NameSouth MarshIsland 97
Bald PateGarden Banks 260
Shell Offshore Inc.,Amerada Hessand Pennzoil
Amocoand Vastar
Oryx
Phillips, Anadarkoand Amoco
Anadarko
Phillipsand Anadarko
Louisiana Land & Exploration,Anadarko and Agip
Marathon
Texacoand Chevron
Pennzoil, OXYand Total
Commercialdiscovery
Dry hole
Dry hole
Dry hole
Drilling in 1996
Drilling in 1996
Drilling started in 1995
Potentiallycommercialdiscovery
Drilling in 1996
Developmentunder way
1994
1994
1995
1995
Spuddedin 1995
1995Oryx andAmerada
Commercialdiscovery
1996
1996
1995
Hydrocarbons present
nSubsalt drilling scorecard in the Gulf of Mexico. Since the successful well drilled byPhillips and partners in 1993, subsalt exploration in the Gulf of Mexico has blossomed.[From Taylor G: “Subsalt Returns to the Top,” AAPG EXPLORER 17, no. 2 (February 1996): 8.]
(continued on page 56)
54 Oilfield Review
Properties of salt—pseudoplastic flow under sub-
surface temperatures and pressures, and low per-
meability—that make salt bodies effective hydro-
carbon traps also present unique challenges for oil
and gas operators (above). Special considerations,
from selecting drilling fluids and bits to imple-
menting casing programs and cementing proce-
dures, are required to produce long-lasting wells.
Methods developed on the US Gulf Coast and in
the Gulf of Suez, Egypt have improved the effi-
ciency and reliability of drilling and completion
operations in thick salt sections.1
Unlike typical sediment sequences in which hor-
izontal stresses are less than vertical stresses
from overburden, salt is like a fluid, with stresses
in all directions approximately equal to the over-
burden. Therefore, if borehole fluid pressure is
less than in-situ salt strength, stress relaxation
may significantly reduce openhole diameters. In
some cases, relaxation and salt creep can cause
borehole restrictions even before drilling and com-
pletion operations are finished. Undergauge bore-
holes can lead to stuck drillpipe, problems running
casing and ultimately casing failures—ovaling,
bending or collapse.
To maintain near-gauge boreholes, drilling flu-
ids must minimize hole closure and washouts.
Water- and oil-base muds with saturated and
undersaturated salt concentrations, and synthetic
fluids have been used to drill salt, but no single
system works all the time. Water-base muds with
low salt concentrations try to balance salt erosion
and dissolution with creep rate to maintain hole
size. However, because salt creep and dissolution
change across thick salt sections, this can be
problematic and hole size may vary with depth.
High-salt-concentration, water-base muds dissolve
enough salt to offset creep, but can become under-
saturated at high temperatures and enlarge the
hole. Oil and synthetic muds prevent dissolution
and can be used effectively in salt, but are expen-
sive, can leach water, gas and other mineral inclu-
sions out of salt and may not offset creep.2 Eco-
nomic, easy to maintain and adaptable
salt-saturated, water-base muds are often used.
aaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaa aPotential Problems Casing Strings Wellbore Displacement
Salt
Radial stress relaxation
Salt creep ledgesimpinge on drillstring
Borehole wall weakenedby leaching water, gasand other mineralsout of salt
Wellbore enlargementresults from saltdissolution
Accumulated cuttingsjam drillstring
Salt
Salt
Caprock
Shear zone
Saltflow
150°F
200°F
Potentialoverpressure
Unconsolidatedzone
nSpectrum of challenges in subsalt drilling and completion. Drillers have to address factors that cause openhole instability and accompanying problems, includingborehole walls weakened by incompatible muds, restrictions and undergauge hole caused by salt creep, or enlargement due to dissolution (left). In rapidly moving salt,liners cemented inside cemented casing reduce radial pipe deformation and so increase wellbore resistance to nonuniform loads (center). During the life of a well, saltmovement can displace wellbore tubulars, possibly causing casing failure or restricted access (right).
Drilling and CompletionsThrough Salt
Salt is weak and soft, so polycrystalline dia-
mond and other mill-tooth insert cutters, which
make hole by scraping, are used. Stronger inserts
may be needed to penetrate caprock formed on the
top of some salt layers by groundwater leaching of
minerals. Side-cutting, eccentric or bicentered
reamers above bits have been proposed to open up
hole diameters that are larger than the bit and
allow for some salt creep before the borehole
becomes undergauge.3
After drilling into salt, heavier than expected
mud weights may be needed to control salt flow.
Drilling speeds vary among operators, but reason-
ably fast penetration rates—60 to 150 ft/hr [18 to
46 m/hr]—are required, so wells can be cased
quickly. Good hole cleaning and periodic back-
reaming, however, should not be sacrificed just to
make hole faster. Circulating a small volume of
fresh water can remove salt restrictions and free
stuck pipe, but care must be used to prevent
washouts. Enlarged or undergauge holes make
directional control difficult.
Thick salt bodies can affect temperature and
pressure in surrounding formations. Salt thermal
conductivity is high compared to other sediments,
so overlying formations are heated and underlying
formations are cooled. Because salt is a barrier to
basin fluids, if outward flow is insufficient to
achieve normal compaction, high pressure may
develop below salt.4 As disrupted sediments
below salt are penetrated, fluid losses or flow
can occur, depending on mud weight and forma-
tion pressures, unless drillers proceed slowly
and carefully.
Washouts, restrictions, ledges and moving salt
exert nonuniform loads on casing.5 Increasing wall
thickness offers better resistance to these loads
than higher yield strength steels, so heavy-wall
casing can be used if salt creep rates are low and
good cement jobs can be obtained. In more
extreme cases of rapidly moving salt, liners
55Spring 1996
cemented inside cemented casing increase
nonuniform load capacity by reducing casing
deformation. Collapse resistance of properly
cemented concentric strings can equal or exceed
the combined strengths of individual liners and
casings.6 Casing across salt zones is subjected to
tension, compression, burst and hydrostatic loads
combined with nonuniform forces, which must be
included in design calculations.7 Casing can be set
just below salt to save time or in deeper forma-
tions for better support, depending on the salt
interval.8 A diversion stage tool in the casing
string just below the salt may be needed to place
specialized cements across the salt, reduce hydro-
static pressure on weaker subsalt intervals or
ensure efficient slurry placement.
Effective cement fill in the annulus between the
outer casing and borehole minimizes nonuniform
load effects. Long slurry thickening times may
allow salt to encroach on casing before a complete
set occurs, and inadequate displacement across
washouts may cause unequal loading or localized
bending. Adequate fluid-loss control is needed to
prevent excessive loss of slurry mix water that can
dissolve or weaken salt, adversely affect cement
properties or cause annular bridging, loss of
hydrostatic pressure and gas migration (see “Get-
ting to the Root of Gas Migration,” page 36).
Salt-saturated cements prevent salt dissolution,
but are more difficult to mix on surface and extend
slurry set times (over-retardation). Freshwater and
low-salt concentration slurries avoid retardation
problems and are easier to handle, but long-term
exposure to salt may lead to cement failures.
Additives introduced in the late 1980s helped solve
over-retardation and strength development prob-
lems in salt-rich slurries.9 This led to development
of proprietary slurries for cementing across salt
zones like the Dowell SALTBOND cement system,
which provides controllable thickening times,
good early compressive strengths, effective place-
ment rheology, excellent fluid-loss control and
resistance to aggressive brine attack. –MET
1. Barker JW, Feland KW and Tsao YH: “Drilling Long Salt Sec-tions Along the U.S. Gulf Coast,” paper SPE 24605, pre-sented at the 67th SPE Annual Technical Conference andExhibition, Washington, DC, USA, October 4-7, 1992.
Pattillo PD and Rankin TE: “How Amoco Solved CasingDesign Problems in The Gulf of Suez,” Petroleum EngineerInternational 53, no. 11 (November 1981): 86-112.
2. Leyendecker EA and Murray SC: “Properly Prepared OilMuds Aid Massive Salt Drilling,” World Oil 180, no. 4 (April 1975): 93-95.
3. Warren TM, Sinor LA and Dykstra MW: “SimultaneousDrilling and Reaming with Fixed Blade Reamers,” paper SPE30474, presented at the 71st SPE Annual Technical Confer-ence and Exhibition, Dallas, Texas, October 22-25, 1996.
4. O’Brien J and Lerche I: “Understanding SubsaltOverpressure May Reduce Drilling Risks,” Oil & Gas Jour-nal 2, no. 4 (January 24, 1994): 28-34.
5. Cheatham JB and McEver JW: “Behavior of Casing Sub-jected to Salt Loading,” Journal of Petroleum Technology 16(September 1964): 1069-1075.
6. Burkowsky M, Ott H and Schillinger H: “Cemented Pipe-in-Pipe Casing Strings Solve Field Problems,” World Oil 193,no. 5 (October 1981): 143-147.
El-Sayed AAH and Khalaf F: “Resistance of Cemented Con-centric Casing Strings Under Nonuniform Loading,” SPEDrilling Engineering 7, no. 1 (March 1992): 59-64.
7. Recent methods use common Von Mises calculations fornormal loads along with the addition of stresses to accountfor nonuniform collapse. For more on these methods: Hack-ney RM: “A New Approach to Casing Design for Salt Forma-tions,” paper SPE/IADC 13431, presented at the 1985SPE/IADC Drilling Conference, New Orleans, Louisiana,USA, March 6-8, 1985.
8. An article in three parts: LeBlanc L: “Drilling, Completion,Workover Challenges in Subsalt Formations,” Offshore(June 1994): 21-22, 49 (part I); (July 1994): 42-44, 59 (partII); (August 1994): 38-40 (part III).
9. Yearwood J, Drecq P and Rae P: “Cementing Across Mas-sive Salt Formations,” paper 88-39-104, presented at the39th Annual Technical Meeting of the Petroleum Society ofCIM, Calgary, Alberta, Canada, June 12-16, 1988.
ImagingImaging describes the two seismic data pro-cessing steps, stacking and migration, thatbring seismic reflections into focus. Stackingattempts to increase signal-to-noise ratio bysumming records obtained from severalseismic shots reflecting at the same point(above). Energy arrives on each trace at adifferent time, depending on the source-receiver separation, or offset. For a uniform-velocity layer overlying the reflector, seismicrays are straight, and the arrival times definea hyperbola. The set of traces is called acommon midpoint (CMP) gather. Before theCMP gather can be stacked, the traces mustbe shifted to align arrivals. The offset versustime parameter that describes the shiftsdefines the stacking velocity of that layer.Shifting is performed for all reflections visi-ble in the traces. The result of stacking is asingle trace, taken to represent the signalthat would have been recorded in a normal-incidence experiment at the midpoint of thesource-receiver pairs. The basic assumptionin stacking is that velocity does not varyhorizontally over the extent of the gather.
The second component of imaging,migration, redistributes reflected seismicenergy from its recorded position to its trueposition using a velocity model (right ).There are many classes of migration, vary-ing in environment of applicability fromsimple structures and smooth velocity varia-tions to complex structures and rapidlyvarying velocities.6
The main distinctions, for the purpose ofthis article, are the imaging domain—either
time or depth—and the order of migrationin the work flow—poststack or prestack. Toprocess any one survey, combinations ofmigration techniques may be used. Thetrend today, as complex reservoirs comeunder scrutiny, is to use depth rather thantime and prestack instead of poststack.
In time migration, the velocity model,sometimes called the velocity field, may varyonly smoothly (next page, bottom). Velocityshould increase with depth, and any varia-tions in the horizontal direction should begradual. The output of the process is a seis-
mic volume with time as the vertical axis.Time migration is most successful whenvelocities are laterally invariant or smoothlyvarying. It is often applicable and, hencechosen in most parts of the world.
In depth migration, the velocity modelmay have strong velocity contrasts verticallyor horizontally. Depth migration is suited forenvironments in which velocities changeabruptly, often the case with complex struc-tures such as steep dips, faults, folds, saltintrusions and truncated layers. The outputvolume has depth as the vertical axis. Depthmigration, though often appropriate, is stillrarely done because of the difficulty in con-structing an accurate velocity model.
Poststack migration is migration appliedafter the seismic traces have been stacked.Stacking enhances the seismic signal, andalso reduces by an order of magnitude thenumber of traces that comprise the stackedseismic volume, so migration poststack isroughly 100 times faster than prestack. Forpoststack migration to be effective, theassumptions made in stacking must bevalid. The amplitude of the stacked tracemust represent that of the normal-incidencetrace and reflected arrivals must be approxi-mately hyperbolic (next page, top). Theseassumptions are valid only when the struc-ture is simple. Otherwise prestack migrationis more suitable.
Prestack migration is run before stacking,and can handle the most complex structures
56 Oilfield Review
6. For a review: Farmer P, Gray S, Hodgkiss G, PieprzakA, Ratcliff D, Whitcombe D and Whitmore D: “Struc-tural Imaging: Toward a Sharper Subsurface View,”Oilfield Review 5, no. 1 (January 1993): 28-41.
nStacking to enhance and focus seismic signals by summing traces reflected midway between several source-receiver pairs. Energyarrives on each seismic record at a different time, depending on the source-receiver separation, or offset. The arrival times define ahyperbola. Before the traces can be stacked, they must be shifted to align arrivals. The offset versus time relationship that describesthe shifts defines the stacking velocity of that layer.
aaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaa0 offset
Offset 1
Offset 2
Offset 3
Offset 4
Common midpoint(CMP)
1 2 3 4
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Hyperboliccurve
Stackingvelocity
+ =
Offset
Corrected CMP gather StackedCMP
+ + + =aaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaaa a aaaaaaaaMigratedtrace
Midpointtrace Receiver
MIG
Source
Salt
Originaldata
nRedistribution of reflected seismic energyby migration. In this simple 2D rendition,migration (MIG) repositions a reflectedtrace from its recorded position to its trueposition using a velocity model. In morecomplex and 3D cases, reflections may beredistributed to positions outside the planecontaining the source and receivers.Energy may also be distributed amongmultiple locations.
57
nThe effects of velocity variations on raytracing and common midpoint (CMP) assumptions. In a flat model with simplestructures and velocities (top left), raypaths are straight and wavefronts are spherical. Arrival times on seismic records canbe fit with a hyperbola (bottom left). In such a case, the CMP and reflection point would be coincident. Inserting a salt wedgeover the flat reflector (top right) gives rise to bent raypaths. The arrivals do not have a hyperbolic shape on seismic records(bottom right). In this case, the CMP would not be coincident with the reflection point. Also visible in the salt case are multi-ples—arrivals from multiply reflected waves—that present additional processing problems. These waveforms and traceswere created with 2D acoustic finite-difference modeling.
Simple velocities + simplestructure = poststack time migration
Complex velocities + simplestructure = poststack depth migration
Simple velocities + complexstructure = prestack time migration
Complex velocities + complexstructure = prestack depth migration
Incr
easi
ng v
eloc
ity
nVelocity models for four migrationclasses: time, depth, poststack andprestack. Poststack models are on the left,prestack on the right. Time-based modelsare on the top, depth-based on the bot-tom. In time migration, the velocitymodel may vary only smoothly or mono-tonically—always increasing with depth.Depth migration is required for more com-plex velocity models. Poststack migrationworks with models of low complexity,while prestack migration can handle themost complex models.
Dep
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Spring 1996
and velocity fields. With the amount of datain modern 3D surveys, the main constraintson this method are the time and skillneeded to construct velocity models and thecomputing power required for reasonableprocessing turnaround time.
Imaging a seismic volume containing asalt body is unlike traditional processing, inwhich thousands of tapes are sent off to aprocessing group that sends back a finishedproduct, ready for interpretation. Subsaltimaging requires several iterations of migra-tion and interpretation. The process is acomplex interplay of many steps (left ).7
Some of the steps, such as the migrations,are run as batch input to mainframe or mas-sively parallel processor (MPP) computers.Others, such as velocity modeling and layerboundary interpretation, require interactiveworkstations.
Different operators and service companiesmay have variants of these methods, but thegeneral processing flow is the same. Thefirst step is to build an initial model of thevelocity in the overburden—the velocities oflayers overlying the salt. In the North Sea,several major velocity contrasts may overliethe salt. Velocity estimates can come fromray-tracing-based velocity analysis on CMPgathers. If the common midpoint geometryis not suitable, such as when velocities varyhorizontally, a CMP gather cannot be used.Instead, a common image point (CIP) gatheris created using a prestack migration tech-nique to assemble all the traces that imagethe depths below a given surface location.8
In the Gulf of Mexico, sediments are typi-cally sand-shale sequences with smallvelocity contrasts between layers. Withoutstrong velocity contrast, CMP-based velocityanalysis is not necessary, so initial velocitiesare taken from stacking velocities. In bothcases, velocities are checked for trends withwell data such as sonic logs or boreholeseismic data.
The second step uses this early velocitymodel to predict reflection arrival times onCMP or CIP gathers at control points. Theshape of the arrival times of the shallowestmajor reflector is analyzed for the velocitythat best flattens the times, and the velocitymodel is updated. This is the most time-intensive step, and requires the interventionof an expert and the versatility of an interac-tive velocity modeling workstation. (For atour of the Geco-Prakla KUDOS 3D veloc-ity model building workstation, see “Foun-dations in Velocity,” page 60.)
58 Oilfield Review
Model validation
Current layer = maximum
Current layer < maximum
3D poststackdepth migration
volume
Prestack depthmigration of
selected offsets
AnalyzeCIP gathers
3D CMP gathers
3D prestack travel-timeinversion from ray-based
velocity analysis
Compute and outputvelocity nodes
Update velocitycomponent of model
3D poststackdepth migration
Delineate geometryof base of layerin depth domain
Update depthcomponent of model
3D prestackdepth migration
Interpretation ofcurrent layer
in time domain
Velocity modelin depth
3D prestackdepth migration
volume
Inputs
3D stackvolume
nSubsalt prestack depth migration flow chart.Some of the steps, such as velocity modeling andlayer boundary interpretation, require interactiveworkstations. The migrations are run on powerfulmainframe or MPP computers.
With the updated velocity model, post-stack or prestack depth migration is applied,and the gathers are recomputed andchecked for arrival flatness. If necessary,these few steps are iterated to obtain anaccurate velocity of the topmost layer. Thenthe process is repeated for as many layers asare identified above the salt.
If the top of salt appears to be structurallysimple based on preliminary time migration,the velocities of the overburden can be usedin a poststack depth migration to image thetop of salt with good precision. An exampleof this is the imaging of the Cavendish 3Dsurvey in the North Sea. The velocity modelindicates a smooth top of the Zechstein salt(bottom left). Encased within the Zechsteinis a thin, complexly folded dolomite, calledPlattendolomit, that causes strong distortionof seismic ray paths before they reach theSilverpit target. An important step in theconstruction of an accurate depth-velocitymodel was characterizing the shape of thePlattendolomit (below right). The complex-ity of the velocity model—high-velocity saltoverlying lower-velocity sediments—sug-gests that depth migration is better suited forimaging than is time migration. Applyingdepth migration makes a dramatic differ-ence in subsalt structure: the dip of subsaltlayers, and so the locations of potentialtraps, changes significantly compared to thetime migration results (left).
59Spring 1996
7. Modified from: Godfrey B, Pieprzak A, Berg K and Yilmaz Ö: “3-D Salt and Sub-Salt Imaging Strategy: A Case History from the Gulf of Mexico,” TechnicalProgram and Abstracts SEG Summer Research Work-shop on 3-D Seismology: Integrated Comprehensionof Large Data Volumes, Rancho Mirage, California,USA, (August 1-6, 1993): 128-134.
8. Common image point gathers are assembled by amethod that has been likened to looking for a needlein a haystack. Every possible source-receiver pair inthe 3D volume of interest is checked to see whether itcontributes to the signal generated by the reflection ata test point in the volume.
nComparing poststack time (top) to poststack depth migration (bottom) on theCavendish survey. The complex velocity model requires depth migration toaccurately image subsalt structures. Without depth migration, the dips on sub-salt layers may be incorrectly imaged.
nSurface of the complexly folded Plattendolomit.
nVelocity model for the North SeaCavendish survey. The Zechstein salttop is relatively smooth, allowing post-stack migration. Within the salt layerthe lower-velocity Plattendolomit canbe seen. The target layer is the Silver-pit formation.
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Amoco Survey Velocity Section
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50001500 3250Velocity, m/sec
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(continued on page 63)
Before the arrival of massively parallel processor
computers, migration was the stumbling block in
prestack depth imaging. Now that MPPs can han-
dle migration in reasonably short order, the con-
struction of an accurate 3D velocity model is the
most time-consuming task. The Geco-Prakla
KUDOS 3D velocity model building system allows
specialists in interpretive processing to construct
and visualize velocity models interactively.
Velocity modeling systems developed by other
service companies, such as InDepth by Western
Geophysical and GeoDepth by Paradigm Geo-
physical, contain similar features.
A velocity model is defined by two sets of
parameters—layer velocities and reflector
geometries. Such models can have either time or
depth as their vertical axis. Models with time as
the vertical axis are relatively easy to derive from
conventional time-domain processing, and are
generally smooth: rays can be traced through the
models with moderate bending at interfaces, so
processing steps such as computing travel times
through the model can be executed rapidly and
nearly automatically.
In contrast, earth models in depth usually have
strong horizontal and vertical velocity variations.
Rays can bend sharply at interfaces and so the
reflector geometry must be known very accu-
rately. Processing must take an interpretive pause
after each layer is built, precluding automation.
Efficient construction of depth-based models is
the aim of the KUDOS velocity modeler.
Traditional velocity modeling programs con-
strain models to be simple—unlike the real earth
—with no abrupt terminations, pinchouts or multi-
ple vertical values. Layers must be continuous
and extend across the entire survey. The KUDOS
system, by contrast, allows models to be built
with any structural complexity. Graphic elements
are rendered on a high-performance workstation,
allowing immediate visualization—a key ability in
velocity model construction and validation.
In the KUDOS system, a modeling volume is
defined that has its vertical dimension in depth.
Surfaces corresponding to the main geological
horizons are inserted into this volume, subdivid-
ing it. Interval velocity fields are derived and
assigned to each subvolume, forming a spatially
variant velocity-depth model.
Layers are added to the model in an iterative
sequence. At each stage the model consists of a
series of layers, each with its own velocity field,
and a halfspace of unknown velocity below the
bottom layer. This halfspace contains the next
horizon to be imaged. The velocity that will cor-
rectly image the next horizon is derived through
ray-based velocity analysis (below). The velocity
of the layer is mapped by interpolating velocities
determined at control points (next page, bottom).
The halfspace is then “flooded” with the velocity
field derived for that next horizon.
The subvolume model is then exported from
the KUDOS workstation as either a tessellation or
60 Oilfield Review
nInteractive ray-based velocity analysis. For a chosen gather (lower left panel) traces can be shifted interactively to test different interval veloci-ties. A plot of semblance—the coherence achieved between traces shifted with a given velocity—shows the best choices for velocities (upperleft). The higher the semblance, the better that velocity flattens the traces. Velocities that are too high leave arrival times drooping at long offsets(upper right). Velocities that are too low produce corrected gathers that swing up at long offsets (middle right). The correct velocities flattenarrival times across the gather (lower right).
Foundations in Velocity
a 3D grid, and sent with the seismic data to the
computer for post- or prestack depth migration.
Tessellation involves dividing the layered
velocity model into tetrahedra (above, left and
right). Interval velocities are stored at each cor-
ner of every tetrahedron, and the topographies of
the depth surfaces are represented by tetrahedral
facets. Tessellated volumes have special proper-
ties; they are especially efficient for modeling
arrival times by raytracing—for generating travel
times for prestack depth migration—and they can
represent realistic geologic models with struc-
tural complexity at all scales (left). The KUDOS
61Spring 1996
nLayered model before (left) and after (right) tessellation. Tessellation divides layer volumes into tetrahedra and assigns a velocity to each corner of every tetrahedron.
nVelocity control pointsfor a chalk reflectorabove the salt. Velocitiesfor the layer immediatelyabove the reflector areinterpolated betweencontrol points (smallcubes) which are colorcoded by interval veloc-ity—blue is faster thangreen. The spatial posi-tion of each control pointis dictated by rays tracedthrough the velocityfields of the overlyinglayers. A 2D slicethrough the seismic vol-ume is displayed withrays contributing toselected control points.
nTessellation of salt volume with structural complexity at many scales.
Velocity Control Points
Layered Model Before Tessellation Layered Model After Tessellation
Tessellated Salt Body
system can also express the velocity model as an
array of evenly spaced 3D grid points. This creates
a volume that may not look as complex as the tes-
sellated volume, but has a velocity representation
more suited for some migration algorithms.
Following migration, the seismic data are
loaded to the interpretation workstation, where
the newly imaged horizon is delineated in depth.
This surface is then incorporated into the KUDOS
model, forming a new base layer. The velocity
field below this layer now needs to be determined,
so the next iteration of velocity analysis begins.
In some areas, such as the Gulf of Mexico, the
background velocity is slowly varying and layer
boundaries are difficult to identify (next page, top).
Instead of proceeding in steps, layer by layer, the
background velocity model is built in just a few
steps, each handling several layers. At selected
locations, CIP gathers are analyzed for the overall
velocity function that best flattens all the arrivals
simultaneously. In the KUDOS system, this
method is called image-based velocity analysis.
The velocity function can be modified interactively
and a corrected gather can be viewed (right).
62 Oilfield Review
nFinding the velocity function that flattens all arrivals simultaneously. Common image point (CIP) gathers(top) obtained from prestack depth migration are converted from depth to time using the current velocitymodel and displayed twice (left and center). The interval (green) and root mean square (RMS) velocity func-tions (red) for this model are shown as a pair of curves on a semblance display (right). Interval velocities canbe modified interactively, automatically adjusting the corresponding RMS velocity function. A new gather isthen computed, and the arrival curvature can be compared to that on the reference gather (left) which remainsunchanged. Other velocities can be tested (bottom). In this example, velocities higher than the referencemodel have been picked (green dots) and applied to the gather (center panel). The new velocities are too high,causing downward curvature to the arrivals. The original velocities remain as black dots on the screen.
Correct Velocities
High Velocities
If the top of salt is rough, prestack depthmigration must be applied (right). Geolo-gists surmise that such complex topogra-phies indicate instabilities where theupward movement of the salt, once halted,has been reactivated.
Once the top of salt has been imaged, aninterpreter must delineate the top of salt onan interactive seismic interpretation worksta-tion. Then the velocity model is updated byfilling the volume below the top of salt withsalt velocity, assumed to be uniform. Withthis new model, another prestack—or post-stack if overburden velocities are smoothenough—depth migration is performed, andthe bottom of salt comes into focus.
An interpreter then maps the bottom ofsalt. Next, and similar to the first step, veloc-ities of the sedimentary layers below the saltare estimated. These are first approximatedby the velocities of layers at the same depthbut outside the canopy of salt. Then aprestack depth migration is run and sets ofgathers are checked for flat arrivals. Thevelocity model is updated at these controlpoints until all control points show flat
arrivals on CIP gathers. Then the velocitiesare interpolated between control points andthe full-volume velocity model is complete.
The final step is to run a prestack depthmigration using the full-volume velocitymodel. Then individual cuts through themigrated data volume can be displayed forfurther interpretation. With the vertical axisin depth, locations of interpreted featurescan be communicated directly to engineersto guide drilling and well location decisions.
This set of techniques was used to imagethe salt and subsalt layers in a survey forAmoco in the southern North Sea gas basin.Layers were interpreted on the Charismaseismic interpretation system, and theirvelocities were modeled on the KUDOSworkstation. The target layers were theRotleigendes and Westphalian sands below
63Spring 1996
nGulf of Mexico salt sheet with associated velocity functions at controlpoints. The background velocity increases gradually with depth (yellow togreen) making layer boundaries above the salt difficult to pick. The strongcontrast and constant velocity of the salt are depicted by the dark blueband in the velocity functions.
nA structurallycomplex salt fea-ture requiringprestack depthmigration to imageits top and bottom.The top surface iswhite, the bottomis gold. Imagingoverlapping saltbodies, such asthose shown in thisfigure, requiresadditional itera-tions in processing.
50001500 3250Velocity, m/sec
Overlapping Salt Bodies
the Zechstein salt. Comparison of poststackand prestack depth migration shows thegreater clarity of the prestack method infocusing the top and bottom salt reflections(above ). The prestack depth migrationshows a more sharply focused reflection offthe base of salt and more coherently imagedsubsalt strata than does the poststack migra-tion, paving the way for more confidentinterpretation of subsalt layers.
Algorithms for carrying out these classesof migration have been known for sometime.9 But only in the past few years hascomputer power grown sufficiently to allowcommercially acceptable turnaround forprestack depth migration. Massively parallelprocessors have brought the elapsed timerequired to process a “typical” prestackdepth migration down to one month—a ten-fold improvement.10 In this case, typicalmeans an output volume of two to three off-shore US blocks at 9 sq mile [23 km2] each.Specialists estimate that creating an accu-
rate velocity model takes about a week foreach layer in the model. Velocities must beaccurate to within a couple percent to beuseful for guiding subsalt drilling.
Much work remains if subsalt reservoirsare to be understood as fully as other, moreaccessible fields. In general, even the mostcarefully migrated subsalt images fail toexhibit the same signal quality as sectionsimaged in the absence of salt. Up to now,nearly all subsalt features drilled andlabeled commercial successes have beenidentified by structure rather than by ampli-tude or other waveform attributes routinelytracked by interpreters exploring above salt.
Another seismic technique, the boreholeseismic survey, offers subsalt informationunobtainable by other means.11 These sur-veys, with receivers in the borehole, canmeasure subsalt layer velocities with highaccuracy, map reflector locations and mea-sure reflection amplitudes at the subsaltreflectors. Some operators are using bore-hole seismic survey results to update veloc-ity models for reprocessing prestack depthmigrations.
An advance anticipated in the future is themeasurement of sonic velocities whiledrilling, which can be related to seismiclayer velocities. Operators may be willing toupdate seismic velocity models and repro-cess 3D surveys to get a clearer imagebefore drilling deeper.
The future of subsalt exploration anddevelopment promises as many technicalchallenges as in the past. And beyond salt,the same techniques hold the power toimage other complex features such as over-thrust faults, reefs, recumbent folds and sed-iments below high-velocity carbonates.
—LS
64 Oilfield Review
nComparison of poststack (left) and prestack (right) depth migration of the Amoco survey in the North Sea. Poststack migrationproduces a broken image of the top and bottom of the Zechstein salt. Prestack migration better images reflections from thesalt boundaries, and brings subsalt layering into focus.
9. Western PG and Ball GJ, reference 2.10. The Geco-Prakla processing megacenter in Houston,
Texas, USA relies on a Connection Machine CM-5with a 400-Gbyte disk and 512 processing nodes,providing 64 Gigaflops of peak processing power.
11. For a review of borehole seismic applications:Christie P, Dodds K, Ireson D, Johnston L, RutherfordJ, Schaffner J and Smith N: “Borehole Seismic DataSharpen the Reservoir Image,” Oilfield Review 7,no. 4 (Winter 1995): 18-31.
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