1 Direct Estimation of Porosity from Seismic Data using Rock and Wave Physics Informed Neural Networks RW -PINN

2025-04-28 0 0 1.47MB 20 页 10玖币
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Direct Estimation of Porosity from Seismic Data using Rock and Wave Physics Informed
Neural Networks (RW-PINN)
Divakar Vashisth*¹ and Tapan Mukerji2
1Department of Energy Science and Engineering, Stanford University, USA, 2Department of Energy
Science and Engineering, Stanford University, USA; Department of Geological Sciences, Stanford
University, USA; and Department of Geophysics, Stanford University, USA.
email: 1divakar.vashisth98@gmail.com, 2mukerji@stanford.edu
Abstract
Petrophysical inversion is an important aspect of reservoir modeling. However due to the lack of a unique
and straightforward relationship between seismic traces and rock properties, predicting petrophysical
properties directly from seismic data is a complex task. Many studies have attempted to identify the direct
end-to-end link using supervised machine learning techniques, but face different challenges such as a lack
of large petrophysical training dataset or estimates that may not conform with physics or depositional
history of the rocks. We present a rock and wave physics informed neural network (RW-PINN) model
that can estimate porosity directly from seismic image traces with no or limited number of wells, with
predictions that are consistent with rock physics and geologic knowledge of deposition. As an example,
we use the uncemented sand rock physics model and normal-incidence wave physics to guide the learning
of RW-PINN to eventually get good estimates of porosities from normal-incidence seismic traces and
limited well data. Training RW-PINN with few wells (weakly supervised) helps in tackling the problem
of non-uniqueness as different porosity logs can give similar seismic traces. We use weighted normalized
root mean square error loss function to train the weakly supervised network and demonstrate the impact
of different weights on porosity predictions. The RW-PINN estimated porosities and seismic traces are
compared to predictions from a completely supervised model, which gives slightly better porosity
estimates but poorly matches the seismic traces, in addition to requiring a large amount of labeled training
data. In this paper, we demonstrate the complete workflow for executing petrophysical inversion of
seismic data using self-supervised or weakly supervised rock physics informed neural networks.
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Introduction
Seismic data is widely used in exploration and exploitation industry to infer subsurface geophysical and
geological properties to eventually delineate an underlying reservoir. The conventional approach for
reservoir characterization involves geophysical inversion of seismic data to obtain elastic properties like
seismic velocities and densities (Tarantola, 2005; Sen, 2006; Sen and Stoffa, 2013; Biswas et al., 2019;
Das et al., 2019) followed by petrophysical inversion with the help of rock physics models obtained from
core and well log data to retrieve petrophysical properties like porosities and water saturation (Avseth et
al., 2005; Bachrach, 2006; Mavko et al., 2009, Aleardi, 2018; Grana et al., 2021). Several researchers
have attempted petrophysical inversion of seismic data using deterministic methods (Angeleri and Carpi,
1982; Dolberg et al., 2000; Bosch, 2004), stochastic methods (Ma, 2002; Eidsvik et al., 2004; Saltzer et
al., 2005; Bachrach, 2006) and geostatistical methods (Gonzalez et al., 2008; Bosch et al.,
2009a, 2009b; Azevedo and Soares, 2017; Grana et al., 2021). Avseth et al. (2005) and Grana et al.
(2021) have provided a detailed review on different methods and workflows to perform seismic inversion
for reservoir characterization.
There is no direct relationship between seismic data and petrophysical properties hence many studies have
made use of machine learning methods to approximate the complex nonlinear functional mapping
between input (seismic trace) and output (petrophysical properties) without specifying any explicit
physical relationships. Some examples include the use of support vector regressor and artificial neural
networks (Wong et al., 2002; Gholami and Ansari, 2017; Chaki et al., 2018; Singh et al.,
2021). However, these studies are based on supervised learning that requires a large labeled training
dataset that is geologically consistent with the target reservoir, which can hinder the use of supervised
methods. Das and Mukerji (2020) used convolutional neural networks (CNN) to estimate petrophysical
properties directly from seismic data and used very few wells to augment the training data. Jo et al.
(2021) used ResUNet++ to estimate porosity from spectral decomposed seismic data.
Another shortcoming of solving the inverse problem using purely supervised learning techniques is that
the estimates are not guaranteed to be physically or geologically consistent, honoring the different
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velocity-porosity relations in different depositional environments. To overcome these limitations, we
propose a rock and wave physics informed machine learning model inspired by the autoencoder
architecture (Goodfellow et al., 2016). This machine learning model learns on its own by maximizing the
match between the input and the output. Calderon-Macias et al. (1998) used wave physics informed fully
connected neural network for automatic normal moveout correction and velocity estimation. Biswas et al.
(2019) used wave physics guided CNN for seismic impedance inversion while Dhara and Sen (2022) used
physics guided autoencoder to perform full waveform inversion. Feng et al. (2020) used unsupervised
CNN to estimate porosity from poststack seismic data but required a low-frequency prior porosity along
with the source wavelet to correctly predict the absolute value of porosity.
In this paper, we estimate porosity directly from normal-incidence seismic image trace using rock and
wave physics informed neural network (RW-PINN). We begin with a brief description of our RW-PINN
architecture for both self-supervised and weakly supervised cases. Then, in order to demonstrate the
efficacy of our proposed architecture, we provide insights into the synthetic data we generated using
uncemented sand rock physics model and normal-incidence wave physics model. This is followed by a
comparison between results from completely self-supervised and weakly supervised RW-PINN model
trained using a few wells with a discussion on the impact of number of wells and weights on normalized
root mean square error loss function. Finally, we compare the RW-PINN results with a completely
supervised model and discuss the pros and cons of the different approaches.
Rock and Wave Physics Informed Neural Network (RW-PINN)
The RW-PINN architecture can be sub-divided into two parts: an encoder and a decoder (Figure 1). The
encoder is a deep CNN that takes the seismic trace as input and gives a latent vector as output. Then, this
output vector acts as input for the decoder where it passes through the rock physics block encapsulating
the porosity to velocity relationship, followed by the wave physics block to give normal-incidence
reflectivities that are convolved with the source wavelet to output a predicted seismic trace from the
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decoder. The network learns on its own by minimizing the misfit between the input seismic trace and
predicted seismic trace. Once the training is complete, the encoder output vector gets a meaning in the
form of petrophysical porosity and the encoder is separated and used to predict porosity directly from the
seismic trace. For the completely self-supervised case, root mean square (RMS) misfit is minimized
between the input seismic trace and the predicted seismic trace from the decoder.
Figure 1. Self-supervised RW-PINN architecture, where NT is number of time samples and ND is
number of depth samples. Encoder is a deep CNN that is trained to output porosity from a given input
seismic trace while decoder has all the physics required to guide the learning of the encoder.
We use He initialization method (He et al., 2015) for weights while bias terms of all the convolution
layers are initialized to 0 in the encoder. We use dropout regularization (randomly sets 30% of the input
units of a layer to zero at each epoch) only in the last convolution layer to avoid overfitting during
training (Srivastava et al., 2014). Rectified linear units (ReLU) activation function (Nair and Hinton,
2010) is used to introduce non-linearity in the CNN network while hyperbolic tangent (tanh) activation
function is applied to the CNN output vector to scale the output between -1 to 1 before passing it as input
摘要:

1DirectEstimationofPorosityfromSeismicDatausingRockandWavePhysicsInformedNeuralNetworks(RW-PINN)DivakarVashisth*¹andTapanMukerji21DepartmentofEnergyScienceandEngineering,StanfordUniversity,USA,2DepartmentofEnergyScienceandEngineering,StanfordUniversity,USA;DepartmentofGeologicalSciences,StanfordUniv...

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