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From observed data on the
surface to the subsurface image
Kamal Aghazade
Reference: Seismic Inversion by Schuster, G.T
As a seismic explorer what are we looking for?
Look at this real Earth model from Angola
21
As a seismic explorer what are we looking for?
Look at this real Earth model from Angola
22
As a seismic explorer what are we looking for?
Look at this real Earth model from Angola
23
As a seismic explorer what are we looking for?
Look at this real Earth model from AngolaNow suppose this is our earth model
24
As a seismic explorer what are we looking for?
Look at this real Earth model from AngolaNow suppose this is our earth model
We have No idea about the
subsurface.
But we want to explore it!
25
As a seismic explorer what are we looking for?
Look at this real Earth model from AngolaNow suppose this is our earth model
We have No idea about the
subsurface.
But we want to explore it!
26
As a seismic explorer what are we looking for?
Look at this real Earth model from AngolaNow suppose this is our earth model
We have No idea about the
subsurface.
But we want to explore it!
27
As a seismic explorer what are we looking for?
Look at this real Earth model from AngolaNow suppose this is our earth model
We have No idea about the
subsurface.
But we want to explore it!
How?
28
As a seismic explorer what are we looking for?
Look at this real Earth model from AngolaNow suppose this is our earth model
We have No idea about the
subsurface.
But we want to explore it!
How?
29
As a seismic explorer what are we looking for?
Look at this real Earth model from AngolaNow suppose this is our earth model
We have No idea about the
subsurface.
But we want to explore it!
How?
30
As a seismic explorer what are we looking for?
Look at this real Earth model from AngolaNow suppose this is our earth model
We have No idea about the
subsurface.
But we want to explore it!
How?
31
As a seismic explorer what are we looking for?
Look at this real Earth model from AngolaNow suppose this is our earth model
We have No idea about the
subsurface.
But we want to explore it!
How?
32
As a seismic explorer what are we looking for?
Look at this real Earth model from AngolaNow suppose this is our earth model
We have No idea about the
subsurface.
But we want to explore it!
How?
33
We have data set.
What is the next step?
34
We have data set.
What is the next step?
After some
processing
35
We have data set.
What is the next step?
After some
processing
36
We have data set.
What is the next step?
After some
processing
Stacked section
37
We have data set.
What is the next step?
After some
processing
Stacked section
38
We have data set.
What is the next step?
After some
processing
Stacked section
39
We have data set.
What is the next step?
After some
processing
Stacked section
What is the solution?
40
41
What is migration?
42
What is migration?
Lets start from the first,
when we propagate
waves into subsurface.
• We want to image
subsurface.
• We want to
estimate
reflectivity model.
• How it can be
done?
43
What is migration?
Lets start from the first,
when we propagate
waves into subsurface.
• We want to image
subsurface.
• We want to
estimate
reflectivity model.
• How it can be
done?
44
What is migration?
Lets start from the first,
when we propagate
waves into subsurface.
• We want to image
subsurface.
• We want to
estimate
reflectivity model.
• How it can be
done?
45
What is migration?
Lets start from the first,
when we propagate
waves into subsurface.
• We want to image
subsurface.
• We want to
estimate
reflectivity model.
• How it can be
done?
46
What is migration?
Lets start from the first,
when we propagate
waves into subsurface.
• We want to image
subsurface.
• We want to
estimate
reflectivity model.
• How it can be
done?
Forward and Adjoint
modeling using Green’s
function, which direction?
47
What is migration?
Lets start from the first,
when we propagate
waves into subsurface.
• We want to image
subsurface.
• We want to
estimate
reflectivity model.
• How it can be
done?
Forward and Adjoint
modeling using Green’s
function, which direction?
48
What is migration?
Lets start from the first,
when we propagate
waves into subsurface.
• We want to image
subsurface.
• We want to
estimate
reflectivity model.
• How it can be
done?
Forward and Adjoint
modeling using Green’s
function, which direction?
Given s-x coordinates, the
source wavelet and velocity
model our goal with
forward modeling is to use
Green’s theorem to find
pressure field.
49
50
51
52
53
54
How can we use Green’s function?
What is its rule in forward
modeling?
55
How can we use Green’s function?
What is its rule in forward
modeling?
56
57
58
Now we have this, sounds cumbersome 
59
Now we have this, sounds cumbersome 
If only outgoing waves are considered and the surface S0 is infinity we
have:
60
Now we have this, sounds cumbersome 
If only outgoing waves are considered and the surface S0 is infinity we
have:
61
Now we have this, sounds cumbersome 
If only outgoing waves are considered and the surface S0 is infinity we
have:
62
Look at this relation:
63
Look at this relation:
64
Look at this relation:
65
Look at this relation:
So What?
66
Look at this relation:
So What?
applying the appropriate Green’s function to the Helmholtz equation and
integrating over the volume is the inverse operator to the Helmholtz
equation.
67
Look at this relation:
So What?
applying the appropriate Green’s function to the Helmholtz equation and
integrating over the volume is the inverse operator to the Helmholtz
equation.
Welcome to the Green’s function world 
68
I’m really sorry, this is not the end 
69
I’m really sorry, this is not the end 
70
I’m really sorry, this is not the end 
71
I’m really sorry, this is not the end 
Has cumbersome computation!!
72
 Lippmann-Schwinger solution
73
 Lippmann-Schwinger solution
This equation has cumbersome computation too!!
74
75
We have two methods for finding an
approximate solution:
 Neumann series solution
 Born approximation
76
We have two methods for finding an
approximate solution:
 Neumann series solution
 Born approximation
77
We have two methods for finding an
approximate solution:
 Neumann series solution
 Born approximation
78
We have two methods for finding an
approximate solution:
 Neumann series solution
 Born approximation
79
80
81
What is Born approximation?
82
The first Born approximation, or simply the Born
approximation, is obtained by approximating the scattered
field by the first-order term of the Neumann series
in Neumann solution:
(0)
P P
83
The first Born approximation, or simply the Born
approximation, is obtained by approximating the scattered
field by the first-order term of the Neumann series
in Neumann solution:
(0)
P P
84
The first Born approximation, or simply the Born
approximation, is obtained by approximating the scattered
field by the first-order term of the Neumann series
in Neumann solution:
(0)
P P
85
The first Born approximation, or simply the Born
approximation, is obtained by approximating the scattered
field by the first-order term of the Neumann series
in Neumann solution:
(0)
P P
86
The first Born approximation, or simply the Born
approximation, is obtained by approximating the scattered
field by the first-order term of the Neumann series
in Neumann solution:
(0)
P P
87
The first Born approximation, or simply the Born
approximation, is obtained by approximating the scattered
field by the first-order term of the Neumann series
in Neumann solution:
(0)
P P
Lets go on with linear algebra 
88
We now have this equation:
89
We now have this equation:
90
We now have this equation:
91
We now have this equation:
92
We now have this equation:
93
We now have this equation:
Least Squares solution
94
We now have this equation:
Least Squares solution
95
We now have this equation:
Least Squares solution
96
We now have this equation:
Least Squares solution
This is Least Squares Migration
97
General Imaging Algorithms
98
General Imaging Algorithms
The goals of seismic imaging and migration are to estimate
slowness and reflectivity distribution, respectively.
99
General Imaging Algorithms
The goals of seismic imaging and migration are to estimate
slowness and reflectivity distribution, respectively.
100
General Imaging Algorithms
The goals of seismic imaging and migration are to estimate
slowness and reflectivity distribution, respectively.
101
102
103
104
Slowness model in terms of Green’s function
105
Slowness model in terms of Green’s function
106
Please stay with me and look at this formulae
107
Please stay with me and look at this formulae
108
Please stay with me and look at this formulae
109
Please stay with me and look at this formulae
110
Please stay with me and look at this formulae
111
112
113
114
Next presentation is LSM
Have a best migrated day.
115

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Seismic Migration

  • 1. From observed data on the surface to the subsurface image Kamal Aghazade Reference: Seismic Inversion by Schuster, G.T
  • 2. As a seismic explorer what are we looking for? Look at this real Earth model from Angola 21
  • 3. As a seismic explorer what are we looking for? Look at this real Earth model from Angola 22
  • 4. As a seismic explorer what are we looking for? Look at this real Earth model from Angola 23
  • 5. As a seismic explorer what are we looking for? Look at this real Earth model from AngolaNow suppose this is our earth model 24
  • 6. As a seismic explorer what are we looking for? Look at this real Earth model from AngolaNow suppose this is our earth model We have No idea about the subsurface. But we want to explore it! 25
  • 7. As a seismic explorer what are we looking for? Look at this real Earth model from AngolaNow suppose this is our earth model We have No idea about the subsurface. But we want to explore it! 26
  • 8. As a seismic explorer what are we looking for? Look at this real Earth model from AngolaNow suppose this is our earth model We have No idea about the subsurface. But we want to explore it! 27
  • 9. As a seismic explorer what are we looking for? Look at this real Earth model from AngolaNow suppose this is our earth model We have No idea about the subsurface. But we want to explore it! How? 28
  • 10. As a seismic explorer what are we looking for? Look at this real Earth model from AngolaNow suppose this is our earth model We have No idea about the subsurface. But we want to explore it! How? 29
  • 11. As a seismic explorer what are we looking for? Look at this real Earth model from AngolaNow suppose this is our earth model We have No idea about the subsurface. But we want to explore it! How? 30
  • 12. As a seismic explorer what are we looking for? Look at this real Earth model from AngolaNow suppose this is our earth model We have No idea about the subsurface. But we want to explore it! How? 31
  • 13. As a seismic explorer what are we looking for? Look at this real Earth model from AngolaNow suppose this is our earth model We have No idea about the subsurface. But we want to explore it! How? 32
  • 14. As a seismic explorer what are we looking for? Look at this real Earth model from AngolaNow suppose this is our earth model We have No idea about the subsurface. But we want to explore it! How? 33
  • 15. We have data set. What is the next step? 34
  • 16. We have data set. What is the next step? After some processing 35
  • 17. We have data set. What is the next step? After some processing 36
  • 18. We have data set. What is the next step? After some processing Stacked section 37
  • 19. We have data set. What is the next step? After some processing Stacked section 38
  • 20. We have data set. What is the next step? After some processing Stacked section 39
  • 21. We have data set. What is the next step? After some processing Stacked section What is the solution? 40
  • 22. 41
  • 24. What is migration? Lets start from the first, when we propagate waves into subsurface. • We want to image subsurface. • We want to estimate reflectivity model. • How it can be done? 43
  • 25. What is migration? Lets start from the first, when we propagate waves into subsurface. • We want to image subsurface. • We want to estimate reflectivity model. • How it can be done? 44
  • 26. What is migration? Lets start from the first, when we propagate waves into subsurface. • We want to image subsurface. • We want to estimate reflectivity model. • How it can be done? 45
  • 27. What is migration? Lets start from the first, when we propagate waves into subsurface. • We want to image subsurface. • We want to estimate reflectivity model. • How it can be done? 46
  • 28. What is migration? Lets start from the first, when we propagate waves into subsurface. • We want to image subsurface. • We want to estimate reflectivity model. • How it can be done? Forward and Adjoint modeling using Green’s function, which direction? 47
  • 29. What is migration? Lets start from the first, when we propagate waves into subsurface. • We want to image subsurface. • We want to estimate reflectivity model. • How it can be done? Forward and Adjoint modeling using Green’s function, which direction? 48
  • 30. What is migration? Lets start from the first, when we propagate waves into subsurface. • We want to image subsurface. • We want to estimate reflectivity model. • How it can be done? Forward and Adjoint modeling using Green’s function, which direction? Given s-x coordinates, the source wavelet and velocity model our goal with forward modeling is to use Green’s theorem to find pressure field. 49
  • 31. 50
  • 32. 51
  • 33. 52
  • 34. 53
  • 35. 54
  • 36. How can we use Green’s function? What is its rule in forward modeling? 55
  • 37. How can we use Green’s function? What is its rule in forward modeling? 56
  • 38. 57
  • 39. 58
  • 40. Now we have this, sounds cumbersome  59
  • 41. Now we have this, sounds cumbersome  If only outgoing waves are considered and the surface S0 is infinity we have: 60
  • 42. Now we have this, sounds cumbersome  If only outgoing waves are considered and the surface S0 is infinity we have: 61
  • 43. Now we have this, sounds cumbersome  If only outgoing waves are considered and the surface S0 is infinity we have: 62
  • 44. Look at this relation: 63
  • 45. Look at this relation: 64
  • 46. Look at this relation: 65
  • 47. Look at this relation: So What? 66
  • 48. Look at this relation: So What? applying the appropriate Green’s function to the Helmholtz equation and integrating over the volume is the inverse operator to the Helmholtz equation. 67
  • 49. Look at this relation: So What? applying the appropriate Green’s function to the Helmholtz equation and integrating over the volume is the inverse operator to the Helmholtz equation. Welcome to the Green’s function world  68
  • 50. I’m really sorry, this is not the end  69
  • 51. I’m really sorry, this is not the end  70
  • 52. I’m really sorry, this is not the end  71
  • 53. I’m really sorry, this is not the end  Has cumbersome computation!! 72
  • 55.  Lippmann-Schwinger solution This equation has cumbersome computation too!! 74
  • 56. 75
  • 57. We have two methods for finding an approximate solution:  Neumann series solution  Born approximation 76
  • 58. We have two methods for finding an approximate solution:  Neumann series solution  Born approximation 77
  • 59. We have two methods for finding an approximate solution:  Neumann series solution  Born approximation 78
  • 60. We have two methods for finding an approximate solution:  Neumann series solution  Born approximation 79
  • 61. 80
  • 62. 81
  • 63. What is Born approximation? 82
  • 64. The first Born approximation, or simply the Born approximation, is obtained by approximating the scattered field by the first-order term of the Neumann series in Neumann solution: (0) P P 83
  • 65. The first Born approximation, or simply the Born approximation, is obtained by approximating the scattered field by the first-order term of the Neumann series in Neumann solution: (0) P P 84
  • 66. The first Born approximation, or simply the Born approximation, is obtained by approximating the scattered field by the first-order term of the Neumann series in Neumann solution: (0) P P 85
  • 67. The first Born approximation, or simply the Born approximation, is obtained by approximating the scattered field by the first-order term of the Neumann series in Neumann solution: (0) P P 86
  • 68. The first Born approximation, or simply the Born approximation, is obtained by approximating the scattered field by the first-order term of the Neumann series in Neumann solution: (0) P P 87
  • 69. The first Born approximation, or simply the Born approximation, is obtained by approximating the scattered field by the first-order term of the Neumann series in Neumann solution: (0) P P Lets go on with linear algebra  88
  • 70. We now have this equation: 89
  • 71. We now have this equation: 90
  • 72. We now have this equation: 91
  • 73. We now have this equation: 92
  • 74. We now have this equation: 93
  • 75. We now have this equation: Least Squares solution 94
  • 76. We now have this equation: Least Squares solution 95
  • 77. We now have this equation: Least Squares solution 96
  • 78. We now have this equation: Least Squares solution This is Least Squares Migration 97
  • 80. General Imaging Algorithms The goals of seismic imaging and migration are to estimate slowness and reflectivity distribution, respectively. 99
  • 81. General Imaging Algorithms The goals of seismic imaging and migration are to estimate slowness and reflectivity distribution, respectively. 100
  • 82. General Imaging Algorithms The goals of seismic imaging and migration are to estimate slowness and reflectivity distribution, respectively. 101
  • 83. 102
  • 84. 103
  • 85. 104
  • 86. Slowness model in terms of Green’s function 105
  • 87. Slowness model in terms of Green’s function 106
  • 88. Please stay with me and look at this formulae 107
  • 89. Please stay with me and look at this formulae 108
  • 90. Please stay with me and look at this formulae 109
  • 91. Please stay with me and look at this formulae 110
  • 92. Please stay with me and look at this formulae 111
  • 93. 112
  • 94. 113
  • 95. 114
  • 96. Next presentation is LSM Have a best migrated day. 115