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Contents


Introduction

Bridging physics and deep learning is a topical challenge. While deep learning frameworks open avenues in physical science, the design of physically-consistent deep neural network architectures is an open issue. In the spirit of physics-informed NNs, PDE-NetGen package provides new means to automatically translate physical equations, given as PDEs, into neural network architectures. PDE-NetGen combines symbolic calculus and a neural network generator. The later exploits NN-based implementations of PDE solvers using Keras. With some knowledge of a problem, PDE-NetGen is a plug-and-play tool to generate physics-informed NN architectures. They provide computationally-efficient yet compact representations to address a variety of issues, including among others adjoint derivation, model calibration, forecasting, data assimilation as well as uncertainty quantification. As an illustration, the workflow is first presented for the 2D diffusion equation, then applied to the data-driven and physics-informed identification of uncertainty dynamics for the Burgers equation.

  • O. Pannekoucke and R. Fablet, “PDE-NetGen 1.0: from symbolic partial differential equation (PDE) representations of physical processes to trainable neural network representations,” Geoscientific Model Development, vol. 13, no. 7, pp. 3373–3382, Jul. 2020, doi: 10.5194/gmd-13-3373-2020.
This work has been supported by the French INSU-LEFE, grant KAPA
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Example

Implementation of a simple PDE: the 2D diffusion equation

A diffusion over a 2D domain can be implemented as

Implementation of a 2D diffusion equation

(see the notebook ./example/pdenetgen-diffusion2D.ipynb)

Estimation of an unknown physical term

As an example, we consider a situation that can be encountered in physics where the dynamics makes appear an unkown term to determine from a dataset. For the illustration, we consider the dynamics

pkf-system

where the term unknown term is unkown.

With PDE-NetGen, we can design a closure from the data. For the illustration we consider a candidate for the closure, given by

pkf-closure

where $(a,b,c)$ are unkowns.

Two implementations can be considered.

1. Implementation using TrainableScalar

This is implemented by using TrainableScalar as follows:

  1. the candidate for the closure is defined as a symbolic level
  2. a neural network that implement the full dynamics (including the closure) is then generated and ready for the training

Implementation of a closure

The use of TrainableScalar is the simplest way to try a closure designed from partial derivatives.

(see the notebook ./example/pdenetgen-NN-PKF_burgers_learn-TrainableScalar-closure.ipynb)

2. Implementation using an external neural network (the exogenous case)

Another implemention is possible that relies on the introduction of an external neural network, for instance a deep neural network of your choice that you have to build by yourself and that can be plugged to the neural network generated from Eq.(7) .

(see the notebook ./example/pdenetgen-NN-PKF_burgers_learn-exogenous-closure.ipynb where the closure is provided as the implementation of Eq.(8) -- you can try your own NN that can be different from the candidate Eq.(8))

Install

Using pip

PDE-NetGen is available from pip, and can be installed as pip install pdenetgen

From github

  1. Clone the repository git clone https://github.com/opannekoucke/pdenetgen.git
  2. Install the package make install (or python setup.py install)
  3. Examples are given as jupyter notebooks (see ./example/)

Remove pdenetgen

pip uninstall pdenetgen

Citation

Pannekoucke, O. and Fablet, R.: PDE-NetGen 1.0: from symbolic partial differential equation (PDE) representations of physical processes to trainable neural network representations, Geosci. Model Dev., 13, 3373–3382, https://doi.org/10.5194/gmd-13-3373-2020, 2020.

@Article{Pannekoucke2020GMD,
  author    = {Olivier Pannekoucke and Ronan Fablet},
  journal   = {Geoscientific Model Development},
  title     = {{PDE}-{NetGen} 1.0: from symbolic partial differential equation ({PDE}) representations of physical processes to trainable neural network representations},
  year      = {2020},
  month     = {jul},
  number    = {7},
  pages     = {3373--3382},
  volume    = {13},
  doi       = {10.5194/gmd-13-3373-2020},
  publisher = {Copernicus {GmbH}},  
}