NeuralPDE

NeuralPDE.jl is a solver package which consists of neural network solvers for
partial differential equations using physics-informed neural networks (PINNs). This package utilizes
neural stochastic differential equations to solve PDEs at a greatly increased generality
compared with classical methods.

Installation

Assuming that you already have Julia correctly installed, it suffices to install NeuralPDE.jl in the standard way, that is, by typing ] add NeuralPDE. Note:
to exit the Pkg REPL-mode, just press Backspace or Ctrl + C.

Tutorials and Documentation

For information on using the package,
see the stable documentation. Use the
in-development documentation for the version of
the documentation, which contains the unreleased features.

Features

• Physics-Informed Neural Networks for ODE, SDE, RODE, and PDE solving
• Ability to define extra loss functions to mix xDE solving with data fitting (scientific machine learning)
• Automated construction of Physics-Informed loss functions from a high level symbolic interface
• Sophisticated techniques like quadrature training strategies, adaptive loss functions, and neural adapters
  to accelerate training
• Integrated logging suite for handling connections to TensorBoard
• Handling of (partial) integro-differential equations and various stochastic equations
• Specialized forms for solving ODEProblems with neural networks
• Compatibility with Flux.jl and Lux.jl
  for all of the GPU-powered machine learning layers available from those libraries.
• Compatibility with NeuralOperators.jl for
  mixing DeepONets and other neural operators (Fourier Neural Operators, Graph Neural Operators,
  etc.) with physics-informed loss functions

Example: Solving 2D Poisson Equation via Physics-Informed Neural Networks

using NeuralPDE, Lux, ModelingToolkit, Optimization, OptimizationOptimisers
import DomainSets: Interval, infimum, supremum

@parameters x y
@variables u(..)
Dxx = Differential(x)^2
Dyy = Differential(y)^2
2D PDE
eq = Dxx(u(x, y)) + Dyy(u(x, y)) ~ -sin(pi * x) * sin(pi * y)
Boundary conditions
bcs = [u(0, y) ~ 0.0, u(1, y) ~ 0,
    u(x, 0) ~ 0.0, u(x, 1) ~ 0]
Space and time domains
domains = [x ∈ Interval(0.0, 1.0),
    y ∈ Interval(0.0, 1.0)]
Discretization
dx = 0.1
Neural network
dim = 2 # number of dimensions
chain = Lux.Chain(Dense(dim, 16, Lux.σ), Dense(16, 16, Lux.σ), Dense(16, 1))
discretization = PhysicsInformedNN(chain, QuadratureTraining())
@named pde_system = PDESystem(eq, bcs, domains, [x, y], [u(x, y)])
prob = discretize(pde_system, discretization)
callback = function (p, l)
    println("Current loss is: $l")
    return false
end
res = Optimization.solve(prob, ADAM(0.1); callback = callback, maxiters = 4000)
prob = remake(prob, u0 = res.minimizer)
res = Optimization.solve(prob, ADAM(0.01); callback = callback, maxiters = 2000)
phi = discretization.phi

And some analysis:

xs, ys = [infimum(d.domain):(dx / 10):supremum(d.domain) for d in domains]
analytic_sol_func(x, y) = (sin(pi * x) * sin(pi * y)) / (2pi^2)

u_predict = reshape([first(phi([x, y], res.minimizer)) for x in xs for y in ys],
    (length(xs), length(ys)))
u_real = reshape([analytic_sol_func(x, y) for x in xs for y in ys],
    (length(xs), length(ys)))
diff_u = abs.(u_predict .- u_real)
using Plots
p1 = plot(xs, ys, u_real, linetype = :contourf, title = "analytic");
p2 = plot(xs, ys, u_predict, linetype = :contourf, title = "predict");
p3 = plot(xs, ys, diff_u, linetype = :contourf, title = "error");
plot(p1, p2, p3)

Citation

If you use NeuralPDE.jl in your research, please cite this paper:

@article{zubov2021neuralpde,
  title={NeuralPDE: Automating Physics-Informed Neural Networks (PINNs) with Error Approximations},
  author={Zubov, Kirill and McCarthy, Zoe and Ma, Yingbo and Calisto, Francesco and Pagliarino, Valerio and Azeglio, Simone and Bottero, Luca and Luj{\'a}n, Emmanuel and Sulzer, Valentin and Bharambe, Ashutosh and others},
  journal={arXiv preprint arXiv:2107.09443},
  year={2021}
}