using computational heuristics to recover a variable surface ......27/10/2017 1 using computational...
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Using computational heuristics to recover a variable surface relaxivity from tomographic images for NMR loggingFrancisco J. Benavides Murillo
PhD Candidate. Computer Sciences. UFFLAR laboratory
Universidade Federal Fluminense
Advisors: Dr. Rodrigo Bagueira, Dr. Ricardo Leiderman
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Agenda
� NMR deliverables
� NMR simulation workflow
� Our problem
� Our proposal
� Software
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Formation evaluation by NMR
� Deliverables
� Mineralogy independent porosity
� Pore size distribution
� Irreducible water saturation
� Formation Permeability
� Advantages
� Does not need to wait for laboratory results
� Continuous record of formation’s rock properties
� Available in logging while drilling (LWD)
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http://accutech.metadot.com/index.pl?r=1
www.spe.org/jpt/article/10327-technology-update-24
NMR simulation to produce a PSD
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Pore size distribution
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��,�= ��
�
�
Digital rock
Random Walk
NMR decay
T2 Distribution
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Our problem� A mismatch between laboratory measurements and simulated results (RW
method)
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0,000
0,200
0,400
0,600
0,800
1,000
0,001 0,01 0,1 1 10
Bin magnitude
Time T2 (s)
Reference Constant
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��,�= ��
�
Petrographic thin section
Our proposal
� Surface relaxivity varies with pores size
� Pore size is associated to the collision rate ξ of the fluid molecules saturating the porous media
� ��(�) can be expressed as a combination of sigmoid functions
� Pore size can be recovered from the collision rate
� � =4�
Δ
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0
10
20
30
40
50
0 0,5 1
Relaxivity (µm/s)
ξ…
0
10
20
30
40
50
60
0 0,5 1
Relaxivity (µm/s)
ξ…
0
10
20
30
40
0 0,5 1
Relaxivity (µm/s)
ξ…
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Iterative computational heuristics� A genetic algorithm optimization
� A large set of RW simulations must be performed
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0,0000,2000,4000,6000,8001,000
0,001 0,1 10
Bin magnitude
Time (s)
Random Walk( )ξρ2
GA Same DSP
Experimental results (AC, DP)
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0
20
40
60
80
100
1 3 5 7 9 11 13 15Surface relaxivity (µm/s)
Pore radius (µm)A
0,0000
0,0050
0,0100
0,0150
0,0200
0,0250
0,0300
0,001 0,010 0,100 1,000 10,000
Bin magnitude
T2 (s)B
0
50
100
150
200
250
1 3 5 7 9 11 13 15Surface relaxivity (µm/s)
Pore radius (µm)A
0,0000
0,0100
0,0200
0,0300
0,0400
0,0500
0,001 0,010 0,100 1,000 10,000
Norm
alized bin magnitude
T2 (s)B
0,0000
0,0050
0,0100
0,0150
0,0200
0,0250
0,0300
0,0350
0,001 0,010 0,100 1,000 10,000
Bin magnitude
T2 (s)D
0,0000
0,0100
0,0200
0,0300
0,0400
0,0500
0,0600
0,0700
0,001 0,010 0,100 1,000 10,000
Bin magnitude
T2 (s)D
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Pore size distributions� Varying surface relaxivity � Constant surface relaxivity
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0,0000,0250,0500,0750,1000,1250,1500,1750,2000,2250,250
Volume fraction
Radius (µm)
0,0000,0250,0500,0750,1000,1250,1500,1750,2000,2250,250
Volume fraction
Radius (µm)
0,0000,0250,0500,0750,1000,1250,1500,1750,2000,2250,250
Volume fraction
Radius (µm)
Simulation software
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Collision rate distribution
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Computational heuristics
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Conclusions� A new varying surface relaxivity concept was introduced
� This approach produces a more precise PSD from a rock sample
� The oil industry can apply this approach on the formation evaluation by NMR
� A new Software Tool specialized in NMR: https://www.youtube.com/watch?v=kR7FmL6KSII
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Acknowledgements
� Advisors: Dr. Rodrigo Bagueira and Dr. Ricardo Leiderman
� Universidade Federal Fluminense
� Universidad Nacional de Costa Rica
� Sponsored by Shell, registered as ``Aplicação de técnicas avançadas deRessonância Magnética Nuclear (RMN) assistidas por ferramentascomputacionais na avaliação petrofísica de rochas carbonáticas`` (ANP18999-3) under the ANP R&D levy as “Compromisso de Investimentos comPesquisa e Desenvolvimento”
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