Velocity calibration and wavefield Overview decomposition for - - PowerPoint PPT Presentation

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Velocity calibration and wavefield Overview decomposition for - - PowerPoint PPT Presentation

Velocity calibration and wavefield decomposition M. von Steht & J. Mann Velocity calibration and wavefield Overview decomposition for walkover VSP data Theory CRS stack for VSP FO CRS-Operator Calibration method Markus von Steht and


slide-1
SLIDE 1

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Velocity calibration and wavefield decomposition for walkover VSP data

Markus von Steht and Jürgen Mann

Wave Inversion Technology Consortium Geophysical Institute, University of Karlsruhe (TH) June 12, 2008

slide-2
SLIDE 2

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Overview Theory CRS approach for VSP geometry FO CRS traveltime approximation Calibration method Data example Survey description Velocity calibration Wavefield decomposition Conclusions & outlook

slide-3
SLIDE 3

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS approach for VSP geometry

slide-4
SLIDE 4

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS approach for VSP geometry

Finite-offset (FO) 2D CRS stack theory initially introduced for surface seismic (Zhang et al., 2001)

slide-5
SLIDE 5

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS approach for VSP geometry

Finite-offset (FO) 2D CRS stack theory initially introduced for surface seismic (Zhang et al., 2001)

◮ second order approximation based on paraxial

ray-theory

slide-6
SLIDE 6

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS approach for VSP geometry

Finite-offset (FO) 2D CRS stack theory initially introduced for surface seismic (Zhang et al., 2001)

◮ second order approximation based on paraxial

ray-theory

◮ central ray is non-zero offset

slide-7
SLIDE 7

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS approach for VSP geometry

Finite-offset (FO) 2D CRS stack theory initially introduced for surface seismic (Zhang et al., 2001)

◮ second order approximation based on paraxial

ray-theory

◮ central ray is non-zero offset

➥ expansion points ( xS, xG) for each simulated source and receiver pair

slide-8
SLIDE 8

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS approach for VSP geometry

Finite-offset (FO) 2D CRS stack theory initially introduced for surface seismic (Zhang et al., 2001)

◮ second order approximation based on paraxial

ray-theory

◮ central ray is non-zero offset

➥ expansion points ( xS, xG) for each simulated source and receiver pair

◮ FO CRS operator depends on five parameters

slide-9
SLIDE 9

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS approach for VSP geometry

Finite-offset (FO) 2D CRS stack theory initially introduced for surface seismic (Zhang et al., 2001)

◮ second order approximation based on paraxial

ray-theory

◮ central ray is non-zero offset

➥ expansion points ( xS, xG) for each simulated source and receiver pair

◮ FO CRS operator depends on five parameters

➥ multi-dimensional optimization problem

slide-10
SLIDE 10

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS approach for VSP geometry

Finite-offset (FO) 2D CRS stack theory initially introduced for surface seismic (Zhang et al., 2001)

◮ second order approximation based on paraxial

ray-theory

◮ central ray is non-zero offset

➥ expansion points ( xS, xG) for each simulated source and receiver pair

◮ FO CRS operator depends on five parameters

➥ multi-dimensional optimization problem

◮ geometrical explanation of stacking parameters

slide-11
SLIDE 11

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS approach for VSP geometry

Finite-offset (FO) 2D CRS stack theory initially introduced for surface seismic (Zhang et al., 2001)

◮ second order approximation based on paraxial

ray-theory

◮ central ray is non-zero offset

➥ expansion points ( xS, xG) for each simulated source and receiver pair

◮ FO CRS operator depends on five parameters

➥ multi-dimensional optimization problem

◮ geometrical explanation of stacking parameters

➥ hypothetical wavefronts, in vicinity of sources and receivers assuming:

slide-12
SLIDE 12

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS approach for VSP geometry

Finite-offset (FO) 2D CRS stack theory initially introduced for surface seismic (Zhang et al., 2001)

◮ second order approximation based on paraxial

ray-theory

◮ central ray is non-zero offset

➥ expansion points ( xS, xG) for each simulated source and receiver pair

◮ FO CRS operator depends on five parameters

➥ multi-dimensional optimization problem

◮ geometrical explanation of stacking parameters

➥ hypothetical wavefronts, in vicinity of sources and receivers assuming:

◮ local isotropy

slide-13
SLIDE 13

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS approach for VSP geometry

Finite-offset (FO) 2D CRS stack theory initially introduced for surface seismic (Zhang et al., 2001)

◮ second order approximation based on paraxial

ray-theory

◮ central ray is non-zero offset

➥ expansion points ( xS, xG) for each simulated source and receiver pair

◮ FO CRS operator depends on five parameters

➥ multi-dimensional optimization problem

◮ geometrical explanation of stacking parameters

➥ hypothetical wavefronts, in vicinity of sources and receivers assuming:

◮ local isotropy ◮ local homogeneity

slide-14
SLIDE 14

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS approach for VSP geometry

Finite-offset (FO) 2D CRS stack theory initially introduced for surface seismic (Zhang et al., 2001)

◮ second order approximation based on paraxial

ray-theory

◮ central ray is non-zero offset

➥ expansion points ( xS, xG) for each simulated source and receiver pair

◮ FO CRS operator depends on five parameters

➥ multi-dimensional optimization problem

◮ geometrical explanation of stacking parameters

➥ hypothetical wavefronts, in vicinity of sources and receivers assuming:

◮ local isotropy ◮ local homogeneity ◮ known velocities

slide-15
SLIDE 15

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS approach for VSP geometry

Finite-offset (FO) 2D CRS stack theory initially introduced for surface seismic (Zhang et al., 2001)

◮ second order approximation based on paraxial

ray-theory

◮ central ray is non-zero offset

➥ expansion points ( xS, xG) for each simulated source and receiver pair

◮ FO CRS operator depends on five parameters

➥ multi-dimensional optimization problem

◮ geometrical explanation of stacking parameters

➥ hypothetical wavefronts, in vicinity of sources and receivers assuming:

◮ local isotropy ◮ local homogeneity ◮ known velocities ➥ calibration required

slide-16
SLIDE 16

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

VSP measurement configuration

S and G are the positions of xS and xG, respectively

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SLIDE 17

CRS Operator for arbitrary geometry

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SLIDE 18

CRS Operator for arbitrary geometry

τ2

hyp

=

  • τ0 + sinβS

vS ∆xS − cosβS vS ∆zS + sinβG vG ∆xG − cosβG vG ∆zG 2 + τ0 AB−1 (∆xS −∆zS tanβS)2 + τ0 DB−1 (∆xG −∆zG tanβG)2 − 2 τ0 B−1 (∆xS −∆zS tanβS) (∆xG −∆zG tanβG).

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SLIDE 19

CRS Operator for arbitrary geometry

τ2

hyp

=

  • τ0 + sinβS

vS ∆xS − cosβS vS ∆zS + sinβG vG ∆xG − cosβG vG ∆zG 2 + τ0 AB−1 (∆xS −∆zS tanβS)2 + τ0 DB−1 (∆xG −∆zG tanβG)2 − 2 τ0 B−1 (∆xS −∆zS tanβS) (∆xG −∆zG tanβG).

◮ τ0 : traveltime of central FO ray

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SLIDE 20

CRS Operator for arbitrary geometry

τ2

hyp

=

  • τ0 + sinβS

vS ∆xS − cosβS vS ∆zS + sinβG vG ∆xG − cosβG vG ∆zG 2 + τ0 AB−1 (∆xS −∆zS tanβS)2 + τ0 DB−1 (∆xG −∆zG tanβG)2 − 2 τ0 B−1 (∆xS −∆zS tanβS) (∆xG −∆zG tanβG).

◮ τ0 : traveltime of central FO ray ◮ ∆xS, ∆zS, ∆xG, ∆zG : horizontal and vertical offsets

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SLIDE 21

CRS Operator for arbitrary geometry

τ2

hyp

=

  • τ0 + sinβS

vS ∆xS − cosβS vS ∆zS + sinβG vG ∆xG − cosβG vG ∆zG 2 + τ0 AB−1 (∆xS −∆zS tanβS)2 + τ0 DB−1 (∆xG −∆zG tanβG)2 − 2 τ0 B−1 (∆xS −∆zS tanβS) (∆xG −∆zG tanβG).

◮ τ0 : traveltime of central FO ray ◮ ∆xS, ∆zS, ∆xG, ∆zG : horizontal and vertical offsets ◮ vS, vG : velocities in the vicinity of

xS and xG

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SLIDE 22

CRS Operator for arbitrary geometry

τ2

hyp

=

  • τ0 + sinβS

vS ∆xS − cosβS vS ∆zS + sinβG vG ∆xG − cosβG vG ∆zG 2 + τ0 AB−1 (∆xS −∆zS tanβS)2 + τ0 DB−1 (∆xG −∆zG tanβG)2 − 2 τ0 B−1 (∆xS −∆zS tanβS) (∆xG −∆zG tanβG).

◮ τ0 : traveltime of central FO ray ◮ ∆xS, ∆zS, ∆xG, ∆zG : horizontal and vertical offsets ◮ vS, vG : velocities in the vicinity of

xS and xG

◮ βS, βG : emergence angles of central ray

slide-23
SLIDE 23

CRS Operator for arbitrary geometry

τ2

hyp

=

  • τ0 + sinβS

vS ∆xS − cosβS vS ∆zS + sinβG vG ∆xG − cosβG vG ∆zG 2 + τ0 AB−1 (∆xS −∆zS tanβS)2 + τ0 DB−1 (∆xG −∆zG tanβG)2 − 2 τ0 B−1 (∆xS −∆zS tanβS) (∆xG −∆zG tanβG).

◮ τ0 : traveltime of central FO ray ◮ ∆xS, ∆zS, ∆xG, ∆zG : horizontal and vertical offsets ◮ vS, vG : velocities in the vicinity of

xS and xG

◮ βS, βG : emergence angles of central ray ◮ DB−1, AB−1, B−1 : composites of elements of

ray-propagator matrix

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SLIDE 24

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

A look at multi-coverage walkover data

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SLIDE 25

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

A look at multi-coverage walkover data *

CR CS qCO

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SLIDE 26

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration of CRS attributes

slide-27
SLIDE 27

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration of CRS attributes

Stacking parameters are converted to wavefield attributes by using tuned velocities.

slide-28
SLIDE 28

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration of CRS attributes

Stacking parameters are converted to wavefield attributes by using tuned velocities.

◮ inaccurate velocities ⇔ incorrect attributes

slide-29
SLIDE 29

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration of CRS attributes

Stacking parameters are converted to wavefield attributes by using tuned velocities.

◮ inaccurate velocities ⇔ incorrect attributes ◮ conventional way: checkshot inversion

slide-30
SLIDE 30

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration of CRS attributes

Stacking parameters are converted to wavefield attributes by using tuned velocities.

◮ inaccurate velocities ⇔ incorrect attributes ◮ conventional way: checkshot inversion

  • ften too inaccurate!
slide-31
SLIDE 31

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration of CRS attributes

Stacking parameters are converted to wavefield attributes by using tuned velocities.

◮ inaccurate velocities ⇔ incorrect attributes ◮ conventional way: checkshot inversion

  • ften too inaccurate!

◮ alternatively: CRS analysis of downgoing waves

slide-32
SLIDE 32

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration of CRS attributes

Stacking parameters are converted to wavefield attributes by using tuned velocities.

◮ inaccurate velocities ⇔ incorrect attributes ◮ conventional way: checkshot inversion

  • ften too inaccurate!

◮ alternatively: CRS analysis of downgoing waves

Assumption:

slide-33
SLIDE 33

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration of CRS attributes

Stacking parameters are converted to wavefield attributes by using tuned velocities.

◮ inaccurate velocities ⇔ incorrect attributes ◮ conventional way: checkshot inversion

  • ften too inaccurate!

◮ alternatively: CRS analysis of downgoing waves

Assumption:

◮ velocities virtually constant within paraxial vicinity

slide-34
SLIDE 34

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration of CRS attributes

Stacking parameters are converted to wavefield attributes by using tuned velocities.

◮ inaccurate velocities ⇔ incorrect attributes ◮ conventional way: checkshot inversion

  • ften too inaccurate!

◮ alternatively: CRS analysis of downgoing waves

Assumption:

◮ velocities virtually constant within paraxial vicinity

(already inherent assumption of CRS method)

slide-35
SLIDE 35

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration of CRS attributes

Stacking parameters are converted to wavefield attributes by using tuned velocities.

◮ inaccurate velocities ⇔ incorrect attributes ◮ conventional way: checkshot inversion

  • ften too inaccurate!

◮ alternatively: CRS analysis of downgoing waves

Assumption:

◮ velocities virtually constant within paraxial vicinity

(already inherent assumption of CRS method) ➥ length of slowness vector

  • p
  • independent of

incidence angle

slide-36
SLIDE 36

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration strategy

slide-37
SLIDE 37

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration strategy

◮ VSP data provides only one slowness component:

slide-38
SLIDE 38

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration strategy

◮ VSP data provides only one slowness component:

slowness component pt tangent to well

slide-39
SLIDE 39

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration strategy

◮ VSP data provides only one slowness component:

slowness component pt tangent to well ➥ in general insufficient to determine

  • p
slide-40
SLIDE 40

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration strategy

◮ VSP data provides only one slowness component:

slowness component pt tangent to well ➥ in general insufficient to determine

  • p
  • ◮ special case: walkover VSP
slide-41
SLIDE 41

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration strategy

◮ VSP data provides only one slowness component:

slowness component pt tangent to well ➥ in general insufficient to determine

  • p
  • ◮ special case: walkover VSP

◮ pt of downgoing rays varies with source position

xS

slide-42
SLIDE 42

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration strategy

◮ VSP data provides only one slowness component:

slowness component pt tangent to well ➥ in general insufficient to determine

  • p
  • ◮ special case: walkover VSP

◮ pt of downgoing rays varies with source position

xS

◮ a ray tangent to well at receiver

xG is very likely

slide-43
SLIDE 43

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration strategy

◮ VSP data provides only one slowness component:

slowness component pt tangent to well ➥ in general insufficient to determine

  • p
  • ◮ special case: walkover VSP

◮ pt of downgoing rays varies with source position

xS

◮ a ray tangent to well at receiver

xG is very likely there: naturally pt ≡

  • p
slide-44
SLIDE 44

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration strategy

◮ VSP data provides only one slowness component:

slowness component pt tangent to well ➥ in general insufficient to determine

  • p
  • ◮ special case: walkover VSP

◮ pt of downgoing rays varies with source position

xS

◮ a ray tangent to well at receiver

xG is very likely there: naturally pt ≡

  • p
  • ◮ Strategy
slide-45
SLIDE 45

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration strategy

◮ VSP data provides only one slowness component:

slowness component pt tangent to well ➥ in general insufficient to determine

  • p
  • ◮ special case: walkover VSP

◮ pt of downgoing rays varies with source position

xS

◮ a ray tangent to well at receiver

xG is very likely there: naturally pt ≡

  • p
  • ◮ Strategy

◮ identify downgoing direct P and/or S arrivals

slide-46
SLIDE 46

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration strategy

◮ VSP data provides only one slowness component:

slowness component pt tangent to well ➥ in general insufficient to determine

  • p
  • ◮ special case: walkover VSP

◮ pt of downgoing rays varies with source position

xS

◮ a ray tangent to well at receiver

xG is very likely there: naturally pt ≡

  • p
  • ◮ Strategy

◮ identify downgoing direct P and/or S arrivals ◮ calculate pt

  • xS,

xG

  • ∀ sources S and receivers G
slide-47
SLIDE 47

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration strategy

◮ VSP data provides only one slowness component:

slowness component pt tangent to well ➥ in general insufficient to determine

  • p
  • ◮ special case: walkover VSP

◮ pt of downgoing rays varies with source position

xS

◮ a ray tangent to well at receiver

xG is very likely there: naturally pt ≡

  • p
  • ◮ Strategy

◮ identify downgoing direct P and/or S arrivals ◮ calculate pt

  • xS,

xG

  • ∀ sources S and receivers G

◮ for each G, search maximum of pt

  • xS,

xG = const

slide-48
SLIDE 48

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration strategy

◮ VSP data provides only one slowness component:

slowness component pt tangent to well ➥ in general insufficient to determine

  • p
  • ◮ special case: walkover VSP

◮ pt of downgoing rays varies with source position

xS

◮ a ray tangent to well at receiver

xG is very likely there: naturally pt ≡

  • p
  • ◮ Strategy

◮ identify downgoing direct P and/or S arrivals ◮ calculate pt

  • xS,

xG

  • ∀ sources S and receivers G

◮ for each G, search maximum of pt

  • xS,

xG = const

searched-for velocity v

  • xG
  • = max
  • pt
  • xS;

xG −1

slide-49
SLIDE 49

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

surface well

slide-50
SLIDE 50

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

surface well downgoing ray

slide-51
SLIDE 51

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

surface well downgoing ray

  • bservable:

tangent slowness component searched−for slowness vector

{

?

slide-52
SLIDE 52

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

surface well

slide-53
SLIDE 53

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

surface well

slide-54
SLIDE 54

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

surface well tangent slowness component length of slowness vector

=

slide-55
SLIDE 55

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

surface well

slide-56
SLIDE 56

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Application of tuned velocities

slide-57
SLIDE 57

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Application of tuned velocities

◮ separate calibration for P- and S-waves

slide-58
SLIDE 58

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Application of tuned velocities

◮ separate calibration for P- and S-waves ◮ velocity vG is property of receiver position

slide-59
SLIDE 59

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Application of tuned velocities

◮ separate calibration for P- and S-waves ◮ velocity vG is property of receiver position

➥ applicable to also calibrate reflected waves

slide-60
SLIDE 60

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Application of tuned velocities

◮ separate calibration for P- and S-waves ◮ velocity vG is property of receiver position

➥ applicable to also calibrate reflected waves

◮ Geometric interpretation provides

slide-61
SLIDE 61

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Application of tuned velocities

◮ separate calibration for P- and S-waves ◮ velocity vG is property of receiver position

➥ applicable to also calibrate reflected waves

◮ Geometric interpretation provides

◮ emergence angles

slide-62
SLIDE 62

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Application of tuned velocities

◮ separate calibration for P- and S-waves ◮ velocity vG is property of receiver position

➥ applicable to also calibrate reflected waves

◮ Geometric interpretation provides

◮ emergence angles ◮ wavefront curvatures

slide-63
SLIDE 63

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Application of tuned velocities

◮ separate calibration for P- and S-waves ◮ velocity vG is property of receiver position

➥ applicable to also calibrate reflected waves

◮ Geometric interpretation provides

◮ emergence angles ◮ wavefront curvatures

◮ suited for

slide-64
SLIDE 64

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Application of tuned velocities

◮ separate calibration for P- and S-waves ◮ velocity vG is property of receiver position

➥ applicable to also calibrate reflected waves

◮ Geometric interpretation provides

◮ emergence angles ◮ wavefront curvatures

◮ suited for

◮ wavefield decomposition

slide-65
SLIDE 65

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Application of tuned velocities

◮ separate calibration for P- and S-waves ◮ velocity vG is property of receiver position

➥ applicable to also calibrate reflected waves

◮ Geometric interpretation provides

◮ emergence angles ◮ wavefront curvatures

◮ suited for

◮ wavefield decomposition ➥ data example

slide-66
SLIDE 66

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Application of tuned velocities

◮ separate calibration for P- and S-waves ◮ velocity vG is property of receiver position

➥ applicable to also calibrate reflected waves

◮ Geometric interpretation provides

◮ emergence angles ◮ wavefront curvatures

◮ suited for

◮ wavefield decomposition ➥ data example ◮ redatuming

slide-67
SLIDE 67

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Application of tuned velocities

◮ separate calibration for P- and S-waves ◮ velocity vG is property of receiver position

➥ applicable to also calibrate reflected waves

◮ Geometric interpretation provides

◮ emergence angles ◮ wavefront curvatures

◮ suited for

◮ wavefield decomposition ➥ data example ◮ redatuming ◮ inversion

slide-68
SLIDE 68

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Application of tuned velocities

◮ separate calibration for P- and S-waves ◮ velocity vG is property of receiver position

➥ applicable to also calibrate reflected waves

◮ Geometric interpretation provides

◮ emergence angles ◮ wavefront curvatures

◮ suited for

◮ wavefield decomposition ➥ data example ◮ redatuming ◮ inversion

◮ strategy also suited for deviated wells

slide-69
SLIDE 69

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

slide-70
SLIDE 70

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

P-wave velocity [km/s]

slide-71
SLIDE 71

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

Modeling:

slide-72
SLIDE 72

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

Modeling:

◮ wavefront construction method

slide-73
SLIDE 73

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

Modeling:

◮ wavefront construction method ◮ direct P

, reflected PP & SS, converted PS

slide-74
SLIDE 74

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

Modeling:

◮ wavefront construction method ◮ direct P

, reflected PP & SS, converted PS

◮ 3D wave propagation

slide-75
SLIDE 75

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

Modeling:

◮ wavefront construction method ◮ direct P

, reflected PP & SS, converted PS

◮ 3D wave propagation ◮ two walkover lines, 100 shots each

slide-76
SLIDE 76

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

Modeling:

◮ wavefront construction method ◮ direct P

, reflected PP & SS, converted PS

◮ 3D wave propagation ◮ two walkover lines, 100 shots each ◮ 40 three-component receiver levels

slide-77
SLIDE 77

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

Modeling:

◮ wavefront construction method ◮ direct P

, reflected PP & SS, converted PS

◮ 3D wave propagation ◮ two walkover lines, 100 shots each ◮ 40 three-component receiver levels ◮ 2D approach sufficiently accurate for calibration

slide-78
SLIDE 78

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

slide-79
SLIDE 79

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

convenient CRS parameter: emergence angle

slide-80
SLIDE 80

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

convenient CRS parameter: emergence angle ➥ tangency ≡ zero angle

slide-81
SLIDE 81

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

convenient CRS parameter: emergence angle ➥ tangency ≡ zero angle Expected behavior:

slide-82
SLIDE 82

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

convenient CRS parameter: emergence angle ➥ tangency ≡ zero angle Expected behavior:

◮ over-estimated velocity

slide-83
SLIDE 83

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

convenient CRS parameter: emergence angle ➥ tangency ≡ zero angle Expected behavior:

◮ over-estimated velocity

zero angle smeared over large offset range

slide-84
SLIDE 84

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

convenient CRS parameter: emergence angle ➥ tangency ≡ zero angle Expected behavior:

◮ over-estimated velocity

zero angle smeared over large offset range

◮ under-estimated velocity

slide-85
SLIDE 85

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

convenient CRS parameter: emergence angle ➥ tangency ≡ zero angle Expected behavior:

◮ over-estimated velocity

zero angle smeared over large offset range

◮ under-estimated velocity

zero angle never occurs

slide-86
SLIDE 86

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

convenient CRS parameter: emergence angle ➥ tangency ≡ zero angle Expected behavior:

◮ over-estimated velocity

zero angle smeared over large offset range

◮ under-estimated velocity

zero angle never occurs

◮ correct velocity

slide-87
SLIDE 87

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Model and survey geometry

convenient CRS parameter: emergence angle ➥ tangency ≡ zero angle Expected behavior:

◮ over-estimated velocity

zero angle smeared over large offset range

◮ under-estimated velocity

zero angle never occurs

◮ correct velocity

well-localized minimum at zero angle

slide-88
SLIDE 88

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration using checkshot inversion

slide-89
SLIDE 89

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration using checkshot inversion

7 7 7 7 7 7 15 15 15 15 15 30 60 60 5 10 15 20 25 30 35 40 receiver index 20 40 60 80 100 shot index

isoclines of emergence angle [◦]

slide-90
SLIDE 90

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration with initial model

7 7 7 15 15 30 30 60 60 5 10 15 20 25 30 35 40 receiver index 20 40 60 80 100 shot index

isoclines of emergence angle [◦]

slide-91
SLIDE 91

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Calibration with corrected model

7 7 15 15 30 30 60 60 5 10 15 20 25 30 35 40 receiver index 20 40 60 80 100 shot index

isoclines of emergence angle [◦]

slide-92
SLIDE 92

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Forward-modeled angles

7 15 15 30 30 60 60 5 10 15 20 25 30 35 40 receiver index 20 40 60 80 100 shot index

isoclines of emergence angle [◦]

slide-93
SLIDE 93

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

1D velocity curves along well

slide-94
SLIDE 94

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

1D velocity curves along well

1400 1600 1800 2000 2200 2400 2600 2800 3000 200 300 400 500 600 700 800 900 P-wave velocity [m/s] depth [m] Inverted Model Initial Model Calibrated Model

slide-95
SLIDE 95

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS-based wavefield decomposition

slide-96
SLIDE 96

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS-based wavefield decomposition

Components (V,H) prior to rotation

slide-97
SLIDE 97

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS-based wavefield decomposition

Components (R,T) after rotation by β P

G – R is strong

slide-98
SLIDE 98

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

CRS-based wavefield decomposition

Components (R,T) after rotation by β S

G – T is strong

slide-99
SLIDE 99

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Five CS gathers prior to rotation

vertical component

slide-100
SLIDE 100

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Five CS gathers prior to rotation

horizontal component

slide-101
SLIDE 101

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Five CS gathers after decomposition

radial orientation using β P

G

slide-102
SLIDE 102

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Five CS gathers after decomposition

transverse orientation using β S

G

slide-103
SLIDE 103

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Conclusions & outlook

slide-104
SLIDE 104

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Conclusions & outlook

Calibration of CRS attributes

slide-105
SLIDE 105

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Conclusions & outlook

Calibration of CRS attributes

◮ high sensitivity to inaccurate velocity

slide-106
SLIDE 106

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Conclusions & outlook

Calibration of CRS attributes

◮ high sensitivity to inaccurate velocity ◮ simple criterion to determine tuned velocities

slide-107
SLIDE 107

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Conclusions & outlook

Calibration of CRS attributes

◮ high sensitivity to inaccurate velocity ◮ simple criterion to determine tuned velocities ◮ readily applicable to 3D data and deviated wells

slide-108
SLIDE 108

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Conclusions & outlook

Calibration of CRS attributes

◮ high sensitivity to inaccurate velocity ◮ simple criterion to determine tuned velocities ◮ readily applicable to 3D data and deviated wells ◮ reliable geometrical CRS attributes for

slide-109
SLIDE 109

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Conclusions & outlook

Calibration of CRS attributes

◮ high sensitivity to inaccurate velocity ◮ simple criterion to determine tuned velocities ◮ readily applicable to 3D data and deviated wells ◮ reliable geometrical CRS attributes for

◮ wavefield decomposition

slide-110
SLIDE 110

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Conclusions & outlook

Calibration of CRS attributes

◮ high sensitivity to inaccurate velocity ◮ simple criterion to determine tuned velocities ◮ readily applicable to 3D data and deviated wells ◮ reliable geometrical CRS attributes for

◮ wavefield decomposition ◮ redatuming

slide-111
SLIDE 111

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Conclusions & outlook

Calibration of CRS attributes

◮ high sensitivity to inaccurate velocity ◮ simple criterion to determine tuned velocities ◮ readily applicable to 3D data and deviated wells ◮ reliable geometrical CRS attributes for

◮ wavefield decomposition ◮ redatuming ◮ inversion, e. g. stereo tomography

slide-112
SLIDE 112

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Conclusions & outlook

Calibration of CRS attributes

◮ high sensitivity to inaccurate velocity ◮ simple criterion to determine tuned velocities ◮ readily applicable to 3D data and deviated wells ◮ reliable geometrical CRS attributes for

◮ wavefield decomposition ◮ redatuming ◮ inversion, e. g. stereo tomography ◮ . . .

slide-113
SLIDE 113

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Conclusions & outlook

Calibration of CRS attributes

◮ high sensitivity to inaccurate velocity ◮ simple criterion to determine tuned velocities ◮ readily applicable to 3D data and deviated wells ◮ reliable geometrical CRS attributes for

◮ wavefield decomposition ◮ redatuming ◮ inversion, e. g. stereo tomography ◮ . . .

◮ possible combination with hodogram analysis

slide-114
SLIDE 114

Velocity calibration and wavefield decomposition

  • M. von Steht & J. Mann

Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

Acknowledgments

This work was kindly supported by. . .

◮ the sponsors of the Wave Inversion Technology

(WIT) Consortium

◮ Paulsson Geophysical Services Inc. for providing

synthetic data and tremendous assistance in questions of VSP imaging

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Velocity calibration and wavefield decomposition

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Overview Theory CRS stack for VSP FO CRS-Operator Calibration method Data example Survey description Velocity calibration Decomposition Conclusions & outlook

W I T

.