L EARNING CONTINUOUS - TIME PDE S FROM SPARSE DATA WITH GRAPH NEURAL NETWORKS
Anonymous authors
Paper under double-blind review
A BSTRACT
The behavior of many dynamical systems follow complex, yet still unknown partial differential equations (PDEs).
While several machine learning methods have been proposed to learn PDEs directly from data, previous methods are limited to discretetime approximations or make the limiting assumption of the observations arriving at regular grids.
We propose a general continuous-time differential model for dynamical systems whose governing equations are parameterized by message passing graph neural networks.
The model admits arbitrary space and time discretizations, which removes constraints on the locations of observation points and time intervals between the observations.
The model is trained with continuous-time adjoint method enabling efﬁcient neural PDE inference.
We demonstrate the model’s ability to work with unstructured grids, arbitrary time steps, and noisy observations.
We compare our method with existing approaches on several well-known physical systems that involve ﬁrst and higher-order PDEs with state-of-the-art predictive performance.
I NTRODUCTION
We consider continuous dynamical systems with a state u ( x , t ) ∈
R that evolves over time t ∈ R + and spatial locations x ∈ Ω ⊂ R D of a bounded domain Ω .
We assume the system is governed by an unknown partial differential equation (PDE)
[Equation]
where the temporal evolution ˙ u of the system depends on the current state u and its spatial ﬁrst and higher-order partial derivatives w.r.t.
the coordinates x .
Such PDE models are the cornerstone of natural sciences, and are widely applicable to modelling of propagative systems, such as behavior of sound waves, ﬂuid dynamics, heat dissipation, weather patterns, disease progression or cellular kinetics (Courant & Hilbert, 2008).
Our objective is to learn the differential F from data.
There is a long history of manually deriving mechanistic PDE equations for speciﬁc systems (Cajori, 1928), such as the Navier-Stokes ﬂuid dynamics or the Schrödinger’s quantum equations, and approximating their solution forward in time numerically (Ames, 2014).
These efforts are complemented by data-driven approaches to infer any unknown or latent coefﬁcients in the otherwise known equations (Isakov, 2006; Berg & Nyström, 2017; Santo et al., 2019), or in partially known equations (Freund et al., 2019; Seo & Liu, 2019b; Seo et al., 2020).
A series of methods have studied neural proxies of known PDEs for solution acceleration (Lagaris et al., 1998; Raissi et al., 2017; Weinan & Yu, 2018;
Sirignano & Spiliopoulos, 2018) or for uncertainty quantiﬁcation (Khoo et al., 2017).
Related work.
Recently the pioneering work of Long et al.
(2017) proposed a fully non-mechanistic method PDE-Net, where the governing equation F is learned from system snapshot observations as a convolutional neural network (CNN) over the input domain discretised into a spatio-temporal grid.
Further works have extended the approach with residual CNNs (Ruthotto & Haber, 2019), symbolic neural networks (Long et al., 2019), high-order autoregressive networks (Geneva & Zabaras, 2020), and feed-forward networks (Xu et al., 2019).
These models are fundamentally limited to discretizing the input domain with a sample-inefﬁcient grid, while they also do not support continuous evolution over time, rendering them unable to handle temporally or spatially sparse or non-uniform observations commonly encountered in realistic applications.
Models such as (Battaglia et al., 2016;
Chang et al., 2016; Sanchez-Gonzalez et al., 2018) are related to the interaction networks where object’s state evolves as a function of its neighboring objects, which forms dynamic relational graphs instead of grids.
In contrast to the dense solution ﬁelds of PDEs, these models apply message-passing between small number of moving and interacting objects, which deviates from PDEs that are strictly differential functions.
In Poli et al.
(2019) graph neural ordinary differential equations (GNODE) were proposed as a framework for modeling continuous-time signals on graphs.
The main limitations of this framework in application to learning PDEs are the lack of spatial information about physical node locations and lack of motivation for why this type of model could be suitable.
Our work can be viewed as connecting graph-based continuous-time models with data-driven learning of PDEs in spatial domain through a classical PDE solution technique.
Contributions.
In this paper we propose to learn free-form, continuous-time, a priori fully unknown
PDE model F from sparse data measured on arbitrary timepoints and locations of the coordinate domain Ω with graph neural networks (GNN).
Our contributions are:
• We introduce continuous-time representation and learning of the dynamics of PDE-driven systems •
We propose efﬁcient graph representation of the domain structure using the method of lines with message passing neural networks •
We achieve state-of-the-art learning performance on realistic PDE systems with irregular data, and our model is highly robust to data sparsity
Source code will be available at anonymized url .
[Table]
M ETHODS
In this Section we consider the problem of learning the unknown function F from observations ( y ( t 0 ) , . . .
, y ( t M ))
∈ R N ×
( M +1) of the system’s state u ( t ) =
( u ( x 1 , t ) , . . .
, u ( x N , t ))
T at N arbitrary spatial locations ( x 1 , . . .
, x N ) and at M + 1 time points ( t 0 , . . .
, t M ) .
We introduce efﬁcient graph convolution neural networks surrogates operating over continuous-time to learn PDEs from sparse data.
We apply the method of lines (MOL) (Schiesser, 2012) to numerically solve Equation 1 .
The MOL consists of selecting N nodes in Ω and discretizing spatial derivatives in F at these nodes.
We place the nodes to the observation locations ( x 1 , . . .
, x N ) .
The discretization leads to F being approximated by ˆ F and produces the following system of ordinary differential equations (ODEs) whose solution asymptotically approximates the solution of Equation
[Equation]
x N ( N ) , u N , u N ( N ) ) 
 ∈ R N .
[Equation] [Equation]
As the discretized ˆ F inherits its unknown nature from the true PDE function F , we approximate ˆ F by a learnable neural surrogate function.
The system’s state at x i is deﬁned as u i , while N ( i ) is a set of indices of neighboring nodes other than i that are required to evaluate ˆ F at x i , and x N ( i ) with u N ( i ) are positions and states of nodes
N ( i ) .
This shows that the temporal derivative ˙ u i of u i depends not only on the location and state at the node i , but also on locations and states of neighboring nodes, resulting in a locally coupled system of ODEs.
Each ODE in the system follows the solution at a ﬁxed location x i .
Numerous ODE solvers have been proposed (such as Euler and Runge-Kutta solvers) to solve the full system
[Equation]
where 0 ≤ τ ≤ t is a cumulative intermediate time variable.
Solving equation 3 forward in time scales linearly both with respect to the number of nodes N and the number of evaluated time points
M , while saturating the input space Ω requires a large number of nodes.
In practice, PDEs are often applied for two- and three-dimensional spatial systems where the method is efﬁcient.
2. P OSITION - INVARIANT GRAPH NEURAL NETWORK DIFFERENTIAL
After introducing Equation 2 , we transition from learning F to learning ˆ F .
The value of ˆ F at a node i must depend only on the nodes i and N ( i ) .
Furthermore, the number of arguments and their order in ˆ F is not known in advance and might be different for each node.
This means that our model
ˆ F must be able to work with an arbitrary number of arguments and must be invariant to permutations of their order.
Graph neural networks (GNNs) (Wu et al., 2020) satisfy these requirements.
In a more restricted setting, where the number of neighbors and their order is known, (e.g. if the grid is uniform) other types of models such as multilayer perceptrons and convolutional neural networks can be used as well.
We consider a type of GNNs called message passing neural networks (MPNNs)
(Gilmer et al., 2017) to represent ˆ F as
[Equation]
where x N ( i ) − x i = { x j − x i : j ∈ N ( i ) } and θ denote parameters of the MPNN.
This formulation assumes the absence of position-dependent quantities in ˆ F , but models based on this formulation are invariant to translations and rotations of Ω , which makes generalization to systems with different node positions feasible, and prevents overﬁtting by memorizing position-speciﬁc dynamics.
We use MPNNs, which is a type of spatial-based GNNs, due to their ﬂexibility and computational efﬁciency.
The main alternative – spectral-based GNNs – have relatively poor scaling with the number of nodes and learn global, or domain-dependent, ﬁlters due to the need to perform eigenvalue decomposition of the Laplacian matrix.
2. M ESSAGE PASSING NEURAL NETWORKS
Let a graph G =
( V, E ) contain nodes V
= { x i } Ni =1 , deﬁned by the measurement positions, and undirected edges E = { e ij } , and assume each node and edge are associated with a node feature v i and an edge feature e ij , respectively.
We use the node neighborhood N ( i ) to deﬁne edges.
Neighbors for each node were selected by applying Delaunay triangulation to the measurement positions.
Two nodes were considered to be neighbors if they lie on the same edge of at least one triangle (Figure 1).
Delaunay triangulation has such useful properties as maximizing the minimum angle within each triangle in the triangulation and containing the nearest neighbor of each node which helps to obtain a good quality discretization of Ω .
In message passing graph neural networks we propagate a latent state for K ≥ 1 graph layers, where each layer k consists of ﬁrst aggregating messages m ( k ) i for each node i , and then updating the corresponding node states h ( k ) i ,
[Equation]
where ⊕ denotes a permutation invariant aggregation function (e.g. sum, mean, max), and φ ( k ) , γ ( k ) are differentiable functions parameterized by deep neural networks.
At any time τ , we initialise the latent states h (0) i
= v i
=
u i ( τ ) and node features to the current state u
i ( τ ) of the system.
We deﬁne edge features e ij :=
x j − x i as location differences.
Finally, we use the node states at the last graph layer of the MPNN to evaluate the PDE surrogate
[Equation]
which is used to solve Equation 3 for the estimated states ˆ u ( t )
=
(ˆ u ( x 1 , t ) , . . .
, ˆ u ( x N , t )) .
2. A DJOINT METHOD FOR LEARNING CONTINUOUS - TIME MPNN SURROGATES
Parameters of ˆ F θ are deﬁned by θ which is the union of parameters of functions φ ( k ) , γ ( k ) , k = 1 , . . .
, K in the MPNN.
We ﬁt θ by minimizing the mean squared error between the observed states ( y ( t 0 ) , . . .
, y ( t M )) and the estimated states (ˆ u ( t 0 ) , . . , ˆ
[Equation]
While discrete-time neural PDE models evaluate the system state only at measurement time points, more accurate continuous-time solution for the estimated state generally requires many more evaluations of the system state.
If an adaptive solver is used to obtain the estimated states, the number of time steps performed by the solver might be signiﬁcantly larger than M .
The amount of memory required to evaluate the gradient of L ( θ ) by backpropagation scales linearly with the number of solver time steps.
This typically makes backpropagation infeasible due to large memory requirements.
We use an alternative approach, which allows computing the gradient for memory cost, which is independent from the number of the solver time steps.
The approach was presented in Chen et al.
(2018) for neural ODEs and is based on the adjoint method (Pontryagin, 2018).
The adjoint method consists of a single forward ODE pass 3 until state ˆ u ( t M ) at the ﬁnal time t M , and subsequent backward ODE pass solving the gradients.
The backward pass is performed by ﬁrst solving the adjoint equation
[Equation]
[Equation]
for the adjoint variables λ from t =
t M until t = 0 with λ ( t M )
= 0 , and then computing
[Equation]
to obtain the ﬁnal gradient.
E XPERIMENTS
We evaluate our model’s performance in learning the dynamics of known physical systems.
We compare to state-of-the-art competing methods, and begin by performing ablation studies to measure how our model’s performance depends on measurement grid sizes, interval between observations, irregular sampling, amount of data and amount of noise.
[Figure]
3. C ONVECTION - DIFFUSION ABLATION STUDIES
The convection-diffusion equation is a partial differential equation that can be used to model a variety of physical phenomena related to the transfer of particles, energy, and other physical quantities inside a physical system.
The transfer occurs due to two processes: convection and diffusion.
The convection-diffusion equation is deﬁned as
[Equation]
where u is the concentration of some quantity of interest (full problem speciﬁcation and setup are in
Appendix A).
Quality of the model’s predictions was evaluated using the relative error between the observed states y ( t i ) and the estimated states ˆ u ( t i ) :
[Equation]
In all following experiments, unless otherwise stated, the training data contains 24 simulations on the time interval [0 , 0 . 2] sec and the test data contains 50 simulations on the time interval [0 , 0 . 6] sec.
Different grid sizes.
This experiment tests our model’s capability to learn from data with different density of observation points.
The time step was set to 0 .
02 sec resulting in 11 training time points per simulation.
The number of observation points x i (and consequently nodes in the GNN) was set to 3000 , 1500 and 750 .
The resulting grids are shown in the ﬁrst column of Figure 2b.
Figure 2 shows relative test errors and models’ predictions.
The performance of the model decreases with the number of nodes in the grid.
Nonetheless, even with the smallest grid, the model was able to learn a reasonably accurate approximation of the system’s dynamics and generalize beyond the training time interval.
Different measurement time interval.
As will be shown in the following experiments, models with a constant time step are sensitive to the length of the time interval between observations.
While showing good performance when the time step is small, such models fail to generalize if the time step is increased.
This experiment shows our model’s ability to learn from data with relatively large time intervals between observations.
We used 11 , 4 and 2 evenly spaced time points for training.
The number of nodes was set to 3000 .
Figure 3 shows relative test errors and models’ predictions.
The model is able to recover the continuous-time dynamics of the system even when trained with four time point per simulation.
Increasing the frequency of observation does not signiﬁcantly improve the performance.
An example of a training simulation with four time points is shown in Figure 11.
Irregular time step.
Observations used for training might not be recorded with a constant time step.
This might cause trouble for models that are built with this assumption.
This experiment tests our model’s ability to learn from data observed at random points in time.
[Figure]
The model is trained on two time grids.
The ﬁrst time grid has a constant time step 0 .
02 sec.
The second grid is the same as the ﬁrst one but with each time point perturbed by noise (cid:15) ∼ N (0 , ( 0 . 026 ) 2 ) .
This gives a time grid with an irregular time step.
The time step for test data was set to 0 .
01 sec.
The number of nodes was set to 3000 .
Relative test errors are shown in Figure 4.
In both cases the model achieves similar performance.
This demonstrates the continuous-time nature of our model as training and predictions are not restricted to evenly spaced time grids as with most other methods.
None of the previous methods that learn free form (i.e., neural network parameterised)
PDEs can be trained with data that is sampled irregularly over time.
Different amount of data.
In this experiment, the model is trained on 1, 5, 10 and 24 simulations.
The test data contains 50 simulations.
The time step was set to 0 .
01 sec.
The number of nodes was set to 3000 .
Relative test errors are shown in Figure 5.
Performance of the model improves as the amount of training data increases.
It should be noted that despite using more data, the relative error does not converge to zero.
Varying amount of additive noise.
We apply additive noise (cid:15) ∼ N (0 , σ 2 ) to training data with σ set to 0.01, 0.02, and 0.04 while the largest magnitude of the observed states is 1.
The time step was set to 0.01 sec.
The number of nodes was set to 3000.
Noise was added only to the training data.
The relative test errors are shown in Figure 6.
The model’s performance decreases as σ grows but even at σ = 0 .
it remains quite high.
3. B ENCHMARK METHOD COMPARISON
The proposed model was compared to two models presented in the literature: PDE-Net (Long et al., 2017) and DPGN (Seo & Liu, 2019a).
PDE-Net is based on a convolutional neural network and employs a constant timestepping scheme resembling the Euler method.
DPGN is based on a graph neural network and implements timestepping as an evolution map in the latent space.
We used the PDE-Net implementation provided in Long et al.
(2017) except that we pass ﬁlter values through an MLP consisting of 2 hidden layers 60 neurons each and tanh nonlinearities which helps to improve stability and performance of the model.
We use 5 × 5 ﬁlters without moment constraints.
The number of δt -blocks was set to the number of time steps in the training data.
The maximum PDE order was set to 4 .
Our implementation of DPGN followed that from Seo & Liu (2019a) with latent diffusivity α = 0 .
The number of parameters in all models was close to 20k.
The training data contains 24 simulations on the time interval [0 , 0 . 2]
sec with the following time steps: 0 . 01 , 0 .
02 and 0 .
04 sec.
The test data contains 50 simulations on the time interval [0 , 0 . 6] sec with the same time steps.
The data was generated on a 50 × 50 regular grid as
PDE-net cannot be applied to arbitrary spatial grids.
The performance of the models was evaluated using the relative error averaged over time.
Mean relative test errors of the models are shown in Figure 7.
The ﬁgure shows that performance of the discretetime models is strongly dependent on the time step while performance of the continuous-time model remains at the same level.
At the smallest time step, PDE-Net, which is a CNN-based model, outperforms other models which are based on message massing neural networks.
This might indicate that MPNNs is not an optimal choice for representing ˆ F θ for this particular PDE system, or that the MPNN surrogate model that we have chosen could be further improved by e.g. increasing its capacity.
Yet again, our MPNN model is applicable to arbitrary space discretizations, whereas CNNs-based models are limited to regular grids.
Importance of relative positional information.
We test our model with and without relative node positions that are encoded as the edge features in our MPNN on grids with a different number of nodes.
Smaller number of nodes results in higher distance variability between neighboring nodes (Figure 12) which should increase the dependence of the model accuracy on the relative spatial information.
By removing spatial information from our model, we recover GNODE.
The models were tested on the heat (Appendix B) and convection-diffusion equations.
A full description of the experiment is in Appendix D.
The results are shown in Figure 8.
Surprisingly, GNODE shows good results on the purely diffusive heat equation.
Nonetheless, the performance of
GNODE noticeably differs from that of our model that includes the spatial information.
Furthermore, the performance difference almost doubles as the number of nodes is decreased from 100% to 50%.
[Figure] [Figure] When applied to the convection-diffusion equation, GNODE fail to learn the dynamics irrespective of the number of nodes.
This can be explained by the presence of the convective term which transports the ﬁeld in a speciﬁc direction thus making positional information particularly important for accurately predicting changes in the ﬁeld.
3. O THER DYNAMICAL SYSTEMS
The model was tested on two more dynamical systems in order to evaluate its ability to work with a wider range of problems.
We selected the heat equation and the Burgers’ equations for that purpose.
The heat equation is one of the simplest PDEs while the Burgers’ equations are more complex than the convection-diffusion equation due to the presence of nonlinear convective terms.
The increase in the problems’ difﬁculty allows to trace the change in the model’s performance as we move from simpler to more complex dynamics while keeping the number of model parameters ﬁxed.
Heat equation.
The heat equation describes the behavior of diffusive systems.
The equation is deﬁned as ∂u∂t =
D ∇ 2 u , where u is the temperature ﬁeld (see Appendix B for details).
Figureshows relative errors and model predictions for a random test case.
The heat equation describes simpler dynamics than the convection diffusion equation which allowed the model to achieve slightly smaller test errors.
Burgers’ equations.
The Burgers’ equations is a system of two coupled nonlinear PDEs.
It describes the behavior of dissipative systems with nonlinear propagation effects.
The equations are deﬁned in a vector form as ∂ u ( x,y,t ) ∂t
=
D ∇ 2 u ( x, y, t ) − u ( x, y, t ) · ∇ u ( x, y, t ) , where u is the velocity vector ﬁeld (see Appendix C for details).
For visualization and error measurement purposes, the velocity vector ﬁeld is converted to a scalar ﬁeld deﬁned by the velocity magnitude at each node.
Figure 10 shows relative errors and model predictions for a random test case.
The Burgers’ equations describe more complex dynamics than the previous two cases which is reﬂected in higher relative test errors.
Visual comparison of the true and predicted states shows that the model was able to achieve sufﬁcient accuracy at approximating the unknown dynamics.
C ONCLUSION
We present a continuous-time model of dynamical systems whose behavior is governed by PDEs.
The model accurately recovers the system’s dynamics even when observation points are sparse and the data is recorded at irregular time intervals.
Comparison with discrete-time models reveals the advantage of continuous-time models for datasets with larger time intervals between observations, which is typical for real-world applications where measurements can be either tedious or costly, or both.
Discretization of the coordinate domain with the method of lines provides a general modeling framework in which arbitrary surrogate functions can be used for approximating ˆ F .
The continuoustime nature of the model enables the use of various time integrators ranging from the Euler method to highly accurate adaptive methods.
This allows to optimize the choice of the surrogate function and time integration scheme depending on the structure of the data
A C ONVECTION - DIFFUSION ABLATION STUDIES
The convection-diffusion equation is a partial differential equation that can be used to model a variety of physical phenomena related to the transfer of particles, energy and other physical quantities inside a physical system.
The transfer occurs due to two processes: convection and diffusion.
Training and testing data was obtained by solving the following initial-boundary value problem on Ω = 2 π ] × [
2 π ] with periodic boundary conditions:
[Equation]
where the diffusion coefﬁcient D was set to 0 .
25 and the velocity ﬁeld v was set to (5 . 0 , 2 . 0) T .
The initial conditions u 0 ( x, y ) were generated as follows:
[Equation]
where N = 4 and λ kl , γ kl ∼ N (0 , 1) .
The generated data contains N s simulations.
Each simulation contains values of u ( x, y, t ) at time points ( t 1 , . .
. , t M ) and locations ( x 1 , . . .
, x N ) , where x n = ( x n , y n ) .
Numerical solutions that represent the true dynamics were obtained using the backward
Euler solver with the time step of 0 .
seconds on a computational grid with 4100 nodes.
Training and testing data used in the following experiments is downsampled from these solutions.
Quality of the model’s predictions was evaluated using the relative error between the observed states y ( t i ) and the estimated states ˆ u ( t i ) :
[Equation]
The model used for all following experiments contains a single graph layer.
The mean was selected as the aggregation function.
Functions φ (1) ( u i , · ) and γ (1) ( u i , u j − u i , x
j − x i ) were represented by multilayer perceptrons with 3 hidden layers and hyperbolic tangent activation functions.
Input/output sizes for φ (1) and γ (1) were set to 4/40 and 41/1 respectively.
The number of hidden neurons was set to 60.
This gives approximately 20k trainable parameters.
We followed the implementation of the adjoint method and ODE solvers from torchdiffeq
Python package (Chen et al., 2018).
In all following experiments, adaptive-order implicit Adams solver was used with rtol and atol set to 1 .
· 10 − 7 .
Rprop (Riedmiller & Braun, 1992) optimizer was used with learning rate set to 1 .
· 10 − 6 and batch size set to 24.
B H EAT EQUATION EXPERIMENT
Training and testing data was obtained by solving the following initial-boundary value problem on Ω = (0 , 1) × (0 , 1) with Dirichlet boundary conditions:
[Equation]
where ∂ Ω denotes the boundaries of Ω and diffusion coefﬁcient D was set to 0 .
The initial conditions u 0 ( x, y ) were generated as follows:
[Equation]
where N = 10 and λ kl , γ kl ∼ N (0 , 1) .
The generated data contains N s simulations.
Each simulation contains values of u ( x, y, t ) at time points ( t 1 , . .
. , t M ) and locations ( x 1 , . . .
, x N ) , where x n = ( x n , y n ) .
Numerical solutions that represent the true dynamics were obtained using the backward
Euler solver with the time step of 0 .
0001 seconds on a computational grid with 4100 nodes.
Training and testing data used in the experiments with the heat equation is downsampled from these solutions.
The model used for all experiments with the heat equation contains a single graph layer.
The mean was selected as the aggregation function.
Functions φ (1) ( u i , · ) and γ (1) ( u i , u j − u i , x
j − x i ) were represented by multilayer perceptrons with 3 hidden layers and hyperbolic tangent activation functions.
Input/output sizes for φ (1) and γ (1) were set to 4/40 and 41/1 respectively.
The number of hidden neurons was set to 60.
This gives approximately 20k trainable parameters.
We followed the implementation of the adjoint method and ODE solvers from torchdiffeq
Python package (Chen et al., 2018).
In all following experiments, adaptive-order implicit Adams solver was used with rtol and atol set to 1 .
· 10 − 7 .
Rprop (Riedmiller & Braun, 1992) optimizer was used with learning rate set to 1 .
· 10 − 6 and batch size set to 24.
In the experiment, the training data contains 24 simulations on the time interval [0 , 0 .
1] sec with time step 0 .
005 sec resulting in 21 time point.
The test data contains 50 simulations on the time interval [0 , 0 .
3] sec with the same time step.
The number of observation points x i was set to 4100 .
C B URGERS ’ EQUATIONS EXPERIMENT
Training and testing data was obtained by solving the following initial-boundary value problem on Ω = [0 , 2 π ] ×
[0 , 2 π ] with periodic boundary conditions:
[Equation]
where the diffusion coefﬁcient D was set to 0 .
The unknown function is now vector-valued.
Therefore, the initial conditions u 0 ( x, y ) for each component were generated as follows:
[Equation]
where N = 2 and λ kl , γ kl ∼ N (0 , 1)
The generated data contains N s simulations.
Each simulation contains values of u ( x, y, t ) at time points ( t 1 , . .
. , t M ) and locations ( x 1 , . . .
, x N ) , where x n = ( x n , y n ) .
Numerical solutions that represent the true dynamics were obtained using the backward
Euler solver with the time step of 0 .
seconds on a computational grid with 5446 nodes.
Training and testing data used in the experiments with the heat equation is downsampled from these solutions.
The model used for all experiments with the Burgers’ equations contains a single graph layer.
The mean was selected as the aggregation function.
Functions φ (1) ( u i , · ) and γ (1) ( u i , u j − u i , x
j − x i ) were represented by multilayer perceptrons with 3 hidden layers and hyperbolic tangent activation functions.
Input/output sizes for φ (1) and γ (1) were set to 6/40 and 41/2 respectively.
The number of hidden neurons was set to 60.
This gives approximately 20k trainable parameters.
We followed the implementation of the adjoint method and ODE solvers from torchdiffeq
Python package (Chen et al., 2018).
In all following experiments, adaptive-order implicit Adams solver was used with rtol and atol set to 1 .
· 10 − 7 .
Rprop (Riedmiller & Braun, 1992) optimizer was used with learning rate set to 1 .
· 10 − 6 and batch size set to 24.
In the experiment, the training data contains 24 simulations on the time interval [0 , 0 . 8] sec with time step 0 .
04 sec resulting in 21 time point.
The test data contains 50 simulations on the time interval [0 , 2 . 4] sec with the same time step.
The number of observation points x i was set to 5000 .
D R ELATIVE P OSITIONAL I NFORMATION E XPERIMENT
Data generation, time intervals, models and hyper parameters for this experiment are described in
Appendix B for the heat equation, and Appendix A and Section 3.1 for the convection diffusion equation.
For the heat equation, 100% of nodes corresponds to 1000 nodes while for the convection-diffusion equation it corresponds to 3000 nodes.
The number of training time points was set to 21 in both cases.
[Figure] [Figure] [Figure] [Figure]
[Figure]