The name of this book, Physics-Based Deep Learning, denotes combinations of physical modeling and numerical simulations with methods based on artificial neural networks. The general direction of Physics-Based Deep Learning represents a very active, quickly growing and exciting field of research. The following chapter will give a more thorough introduction to the topic and establish the basics for following chapters.
From weather and climate forecasts [Sto14] (see the picture above), over quantum physics [OMalleyBK+16], to the control of plasma fusion [MLA+19], using numerical analysis to obtain solutions for physical models has become an integral part of science.
In recent years, machine learning technologies and deep neural networks in particular, have led to impressive achievements in a variety of fields: from image classification [KSH12] over natural language processing [RWC+19], and more recently also for protein folding [Qur19]. The field is very vibrant and quickly developing, with the promise of vast possibilities.
Replacing traditional simulations?¶
These success stories of deep learning (DL) approaches have given rise to concerns that this technology has the potential to replace the traditional, simulation-driven approach to science. E.g., recent works show that NN-based surrogate models achieve accuracies required for real-world, industrial applications such as airfoil flows [CT21], while at the same time outperforming traditional solvers by orders of magnitude in terms of runtime.
Instead of relying on models that are carefully crafted from first principles, can data collections of sufficient size be processed to provide the correct answers? As we’ll show in the next chapters, this concern is unfounded. Rather, it is crucial for the next generation of simulation systems to bridge both worlds: to combine classical numerical techniques with deep learning methods.
One central reason for the importance of this combination is that DL approaches are powerful, but at the same time strongly profit from domain knowledge in the form of physical models. DL techniques and NNs are novel, sometimes difficult to apply, and it is admittedly often non-trivial to properly integrate our understanding of physical processes into the learning algorithms.
Over the last decades, highly specialized and accurate discretization schemes have been developed to solve fundamental model equations such as the Navier-Stokes, Maxwell’s, or Schroedinger’s equations. Seemingly trivial changes to the discretization can determine whether key phenomena are visible in the solutions or not. Rather than discarding the powerful methods that have been developed in the field of numerical mathematics, this book will show that it is highly beneficial to use them as much as possible when applying DL.
Black boxes and magic?¶
People who are unfamiliar with DL methods often associate neural networks with black boxes, and see the training processes as something that is beyond the grasp of human understanding. However, these viewpoints typically stem from relying on hearsay and not dealing with the topic enough.
Rather, the situation is a very common one in science: we are facing a new class of methods, and “all the gritty details” are not yet fully worked out. However, this is pretty common for scientific advances. Numerical methods themselves are a good example. Around 1950, numerical approximations and solvers had a tough standing. E.g., to cite H. Goldstine, numerical instabilities were considered to be a “constant source of anxiety in the future” [Gol90]. By now we have a pretty good grasp of these instabilities, and numerical methods are ubiquitous and well established.
Thus, it is important to be aware of the fact that – in a way – there is nothing magical or otherworldly to deep learning methods. They’re simply another set of numerical tools. That being said, they’re clearly fairly new, and right now definitely the most powerful set of tools we have for non-linear problems. Just because all the details aren’t fully worked out and nicely written up, that shouldn’t stop us from including these powerful methods in our numerical toolbox.
Reconciling DL and simulations¶
Taking a step back, the aim of this book is to build on all the powerful techniques that we have at our disposal for numerical simulations, and use them wherever we can in conjunction with deep learning. As such, a central goal is to reconcile the data-centered viewpoint with physical simulations.
Goals of this document
The key aspects that we will address in the following are:
explain how to use deep learning techniques to solve PDE problems,
how to combine them with existing knowledge of physics,
without discarding our knowledge about numerical methods.
The resulting methods have a huge potential to improve what can be done with numerical methods: in scenarios where a solver targets cases from a certain well-defined problem domain repeatedly, it can for instance make a lot of sense to once invest significant resources to train a neural network that supports the repeated solves. Based on the domain-specific specialization of this network, such a hybrid could vastly outperform traditional, generic solvers. And despite the many open questions, first publications have demonstrated that this goal is not overly far away [KSA+21, UBH+20].
Another way to look at it is that all mathematical models of our nature are idealized approximations and contain errors. A lot of effort has been made to obtain very good model equations, but to make the next big step forward, DL methods offer a very powerful tool to close the remaining gap towards reality [AAC+19].
Within the area of physics-based deep learning, we can distinguish a variety of different approaches, from targeting constraints, combined methods, and optimizations to applications. More specifically, all approaches either target forward simulations (predicting state or temporal evolution) or inverse problems (e.g., obtaining a parametrization for a physical system from observations).
No matter whether we’re considering forward or inverse problems, the most crucial differentiation for the following topics lies in the nature of the integration between DL techniques and the domain knowledge, typically in the form of model equations via partial differential equations (PDEs). The following three categories can be identified to roughly categorize physics-based deep learning (PBDL) techniques:
Supervised: the data is produced by a physical system (real or simulated), but no further interaction exists. This is the classic machine learning approach.
Loss-terms: the physical dynamics (or parts thereof) are encoded in the loss function, typically in the form of differentiable operations. The learning process can repeatedly evaluate the loss, and usually receives gradients from a PDE-based formulation. These soft-constraints sometimes also go under the name “physics-informed” training.
Interleaved: the full physical simulation is interleaved and combined with an output from a deep neural network; this requires a fully differentiable simulator and represents the tightest coupling between the physical system and the learning process. Interleaved differentiable physics approaches are especially important for temporal evolutions, where they can yield an estimate of the future behavior of the dynamics.
Thus, methods can be categorized in terms of forward versus inverse solve, and how tightly the physical model is integrated into the optimization loop that trains the deep neural network. Here, especially interleaved approaches that leverage differentiable physics allow for very tight integration of deep learning and numerical simulation methods.
Physical simulations are a huge field, and we won’t be able to cover all possible types of physical models and simulations.
Rather, the focus of this book lies on:
Field-based simulations (no Lagrangian methods)
Combinations with deep learning (plenty of other interesting ML techniques exist, but won’t be discussed here)
Experiments are left as an outlook (i.e., replacing synthetic data with real-world observations)
It’s also worth noting that we’re starting to build the methods from some very fundamental building blocks. Here are some considerations for skipping ahead to the later chapters.
Hint: You can skip ahead if…
you’re very familiar with numerical methods and PDE solvers, and want to get started with DL topics right away. The Supervised Training chapter is a good starting point then.
On the other hand, if you’re already deep into NNs&Co, and you’d like to skip ahead to the research related topics, we recommend starting in the Physical Loss Terms chapter, which lays the foundations for the next chapters.
A brief look at our notation in the Notation and Abbreviations chapter won’t hurt in both cases, though!
This text also represents an introduction to a wide range of deep learning and simulation APIs. We’ll use popular deep learning APIs such as pytorch https://pytorch.org and tensorflow https://www.tensorflow.org, and additionally give introductions into the differentiable simulation framework ΦFlow (phiflow) https://github.com/tum-pbs/PhiFlow. Some examples also use JAX https://github.com/google/jax. Thus after going through these examples, you should have a good overview of what’s available in current APIs, such that the best one can be selected for new tasks.
As we’re (in most Jupyter notebook examples) dealing with stochastic optimizations, many of the following code examples will produce slightly different results each time they’re run. This is fairly common with NN training, but it’s important to keep in mind when executing the code. It also means that the numbers discussed in the text might not exactly match the numbers you’ll see after re-running the examples.