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Reduced-Time Reduced-Time Migration of Migration of Converted Converted Waves Waves David Sheley David Sheley University of University of Utah Utah
36

Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Dec 20, 2015

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Page 1: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Reduced-Time Reduced-Time Migration of Migration of

Converted WavesConverted Waves

David SheleyDavid SheleyUniversity of UtahUniversity of Utah

Page 2: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

OutlineOutline• MotivationMotivation• Migration TheoryMigration Theory• Error AnalysisError Analysis• Synthetic Data Results Synthetic Data Results • Field Data ResultField Data Result• Conclusions & Future WorkConclusions & Future Work

Page 3: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

PP vs PS Transmission MigrationPP vs PS Transmission MigrationD

epth

Dep

th

OffsetOffset

00

ZZ

Rec

eive

r W

ell

Sou

rce

Wel

l

XX00

Page 4: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

PP Reflection MigrationPP Reflection Migration

XX

Sou

rce

Wel

l

Rec

eive

r W

ell

PP

P = ?P = ?

PP

=?=?

00

Dep

thD

epth

ZZ00 OffsetOffset

Page 5: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Rec

eive

r W

ell

Converted Wave MigrationConverted Wave MigrationS

ourc

e W

ell

XX

PP

PP PSPS

PSPS

VVpp,V,Vss = ? = ?

=?=?

00

Dep

thD

epth

ZZ00 OffsetOffset

Page 6: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

OutlineOutline• MotivationMotivation• Migration TheoryMigration Theory• Error AnalysisError Analysis• Synthetic Data Results Synthetic Data Results • Field Data ResultField Data Result• Conclusions & Future WorkConclusions & Future Work

Page 7: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Conventional MigrationConventional Migration

m(r) = S(zm(r) = S(zgg, , sr sr ++ rgrg))

srsr rgrgss

rr

gg

Page 8: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

PS Transmission MigrationPS Transmission Migration

m(r) = S(zm(r) = S(zgg, d, dsrsr/V/Vp p ++ ddrgrg/V/Vss))

ddsrsr/V/Vpp ddrgrg/V/Vssss gg

rr

Page 9: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

km/seckm/sec

6.06.0

5.05.0

7.07.0

ProblemProblem

WellWell

00

2020

4040

6060

505000

ReceiverReceiverWellWell

SourceSource

Dep

th (

m)

Dep

th (

m)

Offset (m)Offset (m)

Page 10: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Reduced-Time MigrationReduced-Time Migration• Data time shiftData time shift

S’(g, t) = S(zS’(g, t) = S(zgg, t + , t + sg sg sgsgObserved direct-P timeObserved direct-P time

obsobs

obsobs

Page 11: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Dep

th (

m)

Dep

th (

m)

00

1141142020 3535Time (ms)Time (ms)

Original DataOriginal Data

Dep

th (

m)

Dep

th (

m)

00

1141148822 Time (s)Time (s)

Shifted Muted DataShifted Muted Data

SPSPPSPS

PP

PSPS SS

SPSP

Data ShiftData Shift

Page 12: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Reduced-Time MigrationReduced-Time Migration• Data time shiftData time shift

S’(zS’(zgg, t) = S(z, t) = S(zgg, t + , t + sg sg

sgsgObserved direct-P timeObserved direct-P time

obsobs

obsobs

• Modify the migration equationModify the migration equation

m(r) = S(zm(r) = S(zgg, , sr sr ++ rg rg - - sg sg ++ sg sg ))obsobscalccalc

calccalcm(r) = S’(zm(r) = S’(zgg, , sr sr ++ rg rg –– sg sg ))

Page 13: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

OutlineOutline• MotivationMotivation• Migration TheoryMigration Theory• Error AnalysisError Analysis• Synthetic Data Results Synthetic Data Results • Field Data ResultField Data Result• Conclusions & Future WorkConclusions & Future Work

Page 14: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Error Analysis -- CWMError Analysis -- CWM

• Single traceSingle trace• Homogeneous mediaHomogeneous media• True velocity = True velocity = cc

• Migration velocityMigration velocity

c’ = c + c’ = c + cc• VVpp/V/Vss = = psrpsr

Assumptions:Assumptions:

m(r) = S(zm(r) = S(zgg, , sr sr ++ rg rg psrpsr))

m(r) = S(zm(r) = S(zgg, (d, (dsr sr ++ ddrg rg psrpsr)/)/c’c’ ))

Page 15: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Error Analysis Error Analysis Conventional MigrationConventional Migration

(d(dsr sr ++ ddrg rg psrpsr)/)/c’c’ (d(dsr sr ++ ddrg rg psrpsr)/()/(c + c + c)c)==

~~ (d(dsr sr ++ ddrg rg psrpsr)()(s – s s – s c)c)22~~

(d(dsr sr ++ ddrg rg psrpsr) ) s s cc

22

cmcm

Page 16: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

m(r) = S(g,m(r) = S(g,

Error Analysis Error Analysis Reduced-Time MigrationReduced-Time Migration

))obsobscalccalcsr sr ++ rg rg - - sg sg ++ sgsg

Page 17: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Error Analysis Error Analysis Reduced-Time MigrationReduced-Time Migration

obsobscalccalcsr sr ++ rg rg - - sg sg ++ sgsg

==(d(dsr sr ++ ddrg rg psr psr -- ddsgsg)()(s s –– s s c) + c) + ddsg sg ss

22

(d(dsr sr ++ ddrg rg psr psr -- ddsgsg) ) s s cc

rtmrtm22

Page 18: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Error FunctionsError FunctionsCWM vs. RTM CWM vs. RTM

rtmrtm(d(dsr sr ++ ddrg rg psr psr -- ddsgsg) ) s s cc

22

cmcm(d(dsr sr ++ ddrg rg psrpsr) ) s s cc

22

Page 19: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

rtmrtm

cmcm

00

0000

00250250

250250

500500

500500

Dep

th (

m)

Dep

th (

m)

Offset (m)Offset (m)

Dep

th (

m)

Dep

th (

m)

Offset (m)Offset (m)

00

1212

88

44

1616

Imaging-Time ErrorImaging-Time Error

ImagingImaging ErrorError (ms)(ms)

Page 20: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

OutlineOutline• MotivationMotivation• Migration TheoryMigration Theory• Error AnalysisError Analysis• Synthetic Data ResultsSynthetic Data Results • Field Data ResultField Data Result• Conclusions & Future WorkConclusions & Future Work

Page 21: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Crosswell ModelCrosswell Model

Dep

th (

m)

Dep

th (

m)

Offset (m)Offset (m) 11411400114114

00

VV22

VV11

V = 5500 m/sV = 5500 m/s22

V = 5000 m/sV = 5000 m/s11

VVpp /V /Vss = 1.5 = 1.5

Well Separation Well Separation = 100 m= 100 m

Source = 1500 HzSource = 1500 Hzds = 2 mds = 2 mdg = 2 mdg = 2 m

Page 22: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Synthetic DataSynthetic DataD

epth

(m

)D

epth

(m

)

00

1141142020 3535Time (ms)Time (ms)

Original DataOriginal Data

Dep

th (

m)

Dep

th (

m)

00

1141148822 Time (s)Time (s)

Shifted Muted DataShifted Muted Data

SPSPPSPS

PP

PSPS SS

SPSP

Page 23: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

PS Transmission Migration PS Transmission Migration True VelocityTrue Velocity

Dep

th (

m)

Dep

th (

m)

Offset (m)Offset (m)00114114

00

114114

Page 24: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Conventional PS MigrationConventional PS Migration+ 10 % Velocity+ 10 % Velocity

Dep

th (

m)

Dep

th (

m)

Offset (m)Offset (m)00114114

00

114114

Page 25: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Reduced-Time PS MigrationReduced-Time PS Migration+ 10% Velocity+ 10% Velocity

Dep

th (

m)

Dep

th (

m)

Offset (m)Offset (m)00114114

00

114114

Page 26: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

OutlineOutline• MotivationMotivation• Migration TheoryMigration Theory• Error AnalysisError Analysis• Synthetic Data ResultsSynthetic Data Results • Field Data ResultField Data Result• Conclusions & Future WorkConclusions & Future Work

Page 27: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

• Time Delay = 3 ms ?Time Delay = 3 ms ?

• Well locationWell location

• Velocity ModelVelocity Model

Data ProblemsData Problems

Page 28: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

km/seckm/sec

6.06.0

5.05.0

7.07.0

Kidd CreekKidd Creek

WellWell

00

2020

4040

6060

505000

ReceiverReceiverWellWell

SourceSource

Dep

th (

m)

Dep

th (

m)

Offset (m)Offset (m)

Page 29: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

66Time (ms)Time (ms)

00

2020

4040

6060

Dep

th (

m)

Dep

th (

m)

00

Time Shifted CRGTime Shifted CRG

Page 30: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Conventional PS MigrationConventional PS Migration00

2020

4040

6060

505000

Dep

th (

m)

Dep

th (

m)

Offset (m)Offset (m)

Page 31: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Reduced-Time PS MigrationReduced-Time PS Migration00

2020

4040

6060

505000

Dep

th (

m)

Dep

th (

m)

Offset (m)Offset (m)

Page 32: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

RTM-PS CRG #8RTM-PS CRG #800

2020

4040

6060

505000

Dep

th (

m)

Dep

th (

m)

Offset (m)Offset (m)

Page 33: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Kidd CreekKidd Creek00

2020

4040

6060

505000 Offset (m)Offset (m) 505000 Offset (m)Offset (m)

Page 34: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

OutlineOutline• MotivationMotivation• Migration TheoryMigration Theory• Error AnalysisError Analysis• Synthetic Data ResultsSynthetic Data Results • Field Data ResultField Data Result• Conclusions & Future WorkConclusions & Future Work

Page 35: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Discussion & ConclusionsDiscussion & Conclusions

• PS migration can image structure PS migration can image structure invisible to reflection migration.invisible to reflection migration.

• Reduced-time migraton decreases the Reduced-time migraton decreases the error of an incorrect velocity model. error of an incorrect velocity model.

• Converted wave reduced-time Converted wave reduced-time migration can successfully image a migration can successfully image a transmitting boundary.transmitting boundary.

Page 36: Reduced-Time Migration of Converted Waves David Sheley University of Utah.

Future WorkFuture Work• Model and migrate salt proximity Model and migrate salt proximity

VSP data with converted wave VSP data with converted wave RTM. RTM.

• Model and test PP RTM.Model and test PP RTM.• Search for other applications of Search for other applications of

RTM.RTM.• Graduate.Graduate.