multisource full waveform inversion of marine streamer data with frequency selection

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Multisource Full Waveform Inversion of Marine Streamer Data with Frequency Selection Yunsong Huang and Gerard Schuster KAUST

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Multisource Full Waveform Inversion of Marine Streamer Data with Frequency Selection. Yunsong Huang and Gerard Schuster KAUST. Goal of the study Multisource Mismatch solution with marine data Low-discrepancy frequency coding Numerical results Conclusions. Outline. - PowerPoint PPT Presentation

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Page 1: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

Multisource Full Waveform Inversion of Marine Streamer Data

with Frequency Selection

Yunsong Huang and Gerard SchusterKAUST

Page 2: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

• Goal of the study• Multisource

– Mismatch solution with marine data

• Low-discrepancy frequency coding• Numerical results • Conclusions

Outline

Page 3: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

Standard optimization

for FWI

Goal of the Study

Multisource optimization for marine

FWI

Speed and quality

comparison

Page 4: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

• Aim of the study• Multisource Migration

– Least Squares Multisource Migration

• Low-discrepancy frequency coding• Numerical results • Conclusions

Outline

Page 5: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

Standard Migration vs Multisource Migration

Benefit: Reduced computation and memory

Liability: Crosstalk noise …

Given: d1 and d2

Find: m

Soln: m=L1 d1 + L2 d2T T

Given: d1 + d2

Find: m

= L1 d1 + L2 d2T T

+ L1 d2 + L2 d1T T

Soln: m = (L1 + L2)(d1+d2)T

Romero, Ghiglia, Ober, & Morton, Geophysics, (2000)

Src. imaging cond. xtalk

Page 6: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

K=1K=10

Multisource LSM & FWI

Inverse problem:

|| d – L m ||2~~1

2J =arg min

m

Dd misfit

m(k+1) = m(k) + a L Dd~T

Iterative update:

+ L1 Dd2 + L2 Dd1T T

L1Dd1 + L2Dd2T T

Page 7: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

Brief Early History Multisource

Phase Encoded Imaging

Romero, Ghiglia, Ober, & Morton, Geophysics, (2000)

Krebs, Anderson, Hinkley, Neelamani, Lee, Baumstein, Lacasse, SEG Zhan+GTS, (2009)

Virieux and Operto, EAGE, (2009)

Dai, and GTS, SEG, (2009)

Migration

Waveform Inversion and Least Squares Migration

Biondi, SEG, (2009)

Page 8: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

• Aim of the study• Multisource Migration

– Mismatch solution with marine data

• Low-discrepancy frequency coding• Numerical results • Conclusions

Outline

Page 9: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

Land Multisource FWIFixed spread

Simulation geometry must be consistent with the acquisition geometry

Page 10: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

4 Hz 8 Hz

Marine Multisource FWI

Simulated land data

Observedmarine data

Mismatch solution with marine data

wrong misfit

Freq. encoding

8 Hz4 Hz

Blend

Decode & mutepurify

4 Hz 8 Hz

F.T.,freq. selec.

4 Hz 8 Hz

Page 11: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

Multisource FWI Freq. Sel. Workflow

m(k+1) = m(k) + a L Dd~T

For k=1:K

end

Filter and blend observed data: dd

d d

Purify predicted data: dpreddpred

dpred dpred

Data residual: Dd=dpred-d

Select unique frequency for each src

Page 12: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

• Aim of the study• Multisource

– Mismatch solution with marine data• Low-discrepancy frequency coding• Numerical results • Conclusions

Outline

Page 13: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

Low-discrepancy Frequency Encoding

Fre

qu

ency

ind

ex1

60

Source index1 60 Source index1 60

Low-discrepancyencodingencoding

Standard

Fre

qu

ency

ind

ex1

60

Fre

qu

ency

ind

ex1

60

Page 14: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

• Aim of the study• Multisource

– Mismatch solution with marine data

• Low-discrepancy frequency coding• Numerical results • Conclusions

Outline

Page 15: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

Frequency-selection FWI of 2D Marine Data

• Source freq: 8 Hz• Shots: 60• Receivers/shot: 84 • Cable length: 2.3 km

Z (

km

)0

1.5

0 6.8X (km)

4.5

1.5

(km/s)

Page 16: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

FWI images

Starting modelActual model

Z (

km

)0

1.5

Standard FWI(69 iterations)

Z (

km

)0

1.5

0 X (km) 6.8

Multisource FWI(262 iterations)

0 X (km) 6.8

Page 17: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

Convergence Rates

Waveform error

Log

nor

mal

ized

Log iteration number

10.

025

1 26269

by individual sources1 supergather, low-discrepancy encoding

3.8 x

1 supergather,

standard encoding

Same asymptotic convergence rate of the red and white curves

Faster initial convergence rate of the white curve

Page 18: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

Convergence Rates

Velocity error

Log

nor

mal

ized

Log iteration number

10.

35

1 26269

1 supergather,

standard encoding

by individual sources 3.8 x

Speedup60 / 2 / 2 / 3.8 = 4

Gain• 60: sourcesOverhead factors:• 2 x FDTD steps• 2 x domain size• 3.8 x iteration

number1 supergather, low-discrepancy encoding

Page 19: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

Convergence Rates

Velocity error (normalized)

10.

75

iteration number1

10

standard encoding

Low-discrepancy encoding is

12% to 3x faster initially than

Standard encoding

Page 20: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

• Frequency selection is implemented in FDTD– 2 x time steps per forward or backward

modeling

• Low-discrepancy frequency encoding – affects no asymptotic rate of convergence– helps to reduce model error in the beginning of

simulation

• 4x speedup for the multisource FWI on the synthetic marine model

Conclusions

Page 21: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

ThanksSponsors of the CSIM (csim.kaust.edu.sa)

consortium at KAUST & KAUST HPC

Page 22: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

Thank you!

Page 23: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

• At lower (say 1/2) frequencies, the frequency selection strategy sees fewer frequency resources, but Computation cost:– (Nx x Nz) x Ns x Nt is reduced by 1/16,– since each factor is halved.

This part does not degrade the overall speedup much.

In the case of multiscale

Page 24: Multisource Full Waveform Inversion of Marine  Streamer Data  with Frequency Selection

Convergence Rates

Velocity error (normalized)

10.

75

iteration number1 10

by individual sources

1 supergather,

standard encoding

H

LSlew rate = H/L

1 supergather, low-discrepancy encoding