Introductory Example
This tutorial steps through the process of solving a 2D flow for the Lid Driven Cavity (LDC) example using physics-informed neural networks (PINNs) from NVIDIA’s Modulus Sym. In this tutorial, you will learn how to:
generate a 2D geometry using Modulus Sym’ geometry module;
set up the boundary conditions;
select the flow equations to be solved;
interpret the different losses and tune the network; and
do basic post-processing.
The tutorial assumes that you have successfully downloaded the Modulus Sym repository.
Problem Description
The geometry for the problem is shown in Fig. 3. The domain is a square cavity whose sides are each 0.1 m long. We define the center of the square as the origin of a Euclidean coordinate frame, with the x direction going left to right (increasing to the right), and the y direction going down to up (increasing up). The left, right, and bottom sides of the square domain are stationary walls, while the top wall moves in the x direction to the right at 1 \(m/s\).
An important quantity for fluid flow problems is the Reynolds number, a unitless quantity that helps describe whether flow will be more laminar (sheet-like) or turbulent. The Reynolds number is a function of the flow speed, the “characteristic length” of the problem (in this case, the cavity height), and the kinematic velocity (which we will define below). For this problem, we have chosen these quantities so that the Reynolds number is 10, indicating a more laminar flow.
Fig. 3 Lid driven cavity geometry
Case Setup
We first summarize the key concepts and how they relate to Modulus Sym’ features. (For a more detailed discussion, please see Basic methodology.) Solving any physics-driven simulation that is defined by differential equations requires information about the domain of the problem and its governing equations and boundary conditions. Users can define the domain using Modulus Sym’ Constructive Solid Geometry (CSG) module, the STL module, or data from external sources like text files in comma-separated values (CSV) format, NumPy files, or HDF5 files. Once you have this geometry or point cloud, it can be sub-sampled into two sets: points on the boundaries to satisfy the boundary conditions, and interior regions to minimize the PDE/ODE residuals.
The python script for this problem can be found at examples/ldc/ldc_2d.py
Importing the required packages
Start by importing required packages for creating the geometry and neural network, and plotting the results.
# See the License for the specific language governing permissions and
# limitations under the License.
import os
import warnings
from sympy import Symbol, Eq, Abs
import modulus.sym
from modulus.sym.hydra import to_absolute_path, instantiate_arch, ModulusConfig
from modulus.sym.solver import Solver
from modulus.sym.domain import Domain
from modulus.sym.geometry.primitives_2d import Rectangle
from modulus.sym.domain.constraint import (
PointwiseBoundaryConstraint,
PointwiseInteriorConstraint,
)
from modulus.sym.domain.validator import PointwiseValidator
from modulus.sym.domain.inferencer import PointwiseInferencer
from modulus.sym.key import Key
from modulus.sym.eq.pdes.navier_stokes import NavierStokes
from modulus.sym.utils.io import (
csv_to_dict,
ValidatorPlotter,
InferencerPlotter,
Creating a PDE Node
The LDC example uses the 2D steady-state incompressible Navier-Stokes equations to model fluid flow. The Navier-Stokes equations are a system of coupled partial differential equations (PDEs) that describe the flow velocity and pressure at every point in the domain. The two independent variables of the problem represent position: \(x\) and \(y\). We will solve for three variables: \(u\) is the flow velocity in the \(x\) direction, \(v\) is the flow velocity in the \(y\) direction, and \(p\) is the pressure at a given point. The incompressible Navier-Stokes equations have two parameters: the kinematic velocity \(\nu\), and the density of the fluid \(\rho\). Modulus Sym can solve problems with nonconstant \(\nu\) and \(\rho\), but we leave them constant to keep this example simple.
If we assume that the density is a constant and rescale so that \(\rho\) is 1, then the equations take the following form.
(1)\[\begin{split}\begin{aligned}
\frac{\partial u}{\partial x} + \frac{\partial v}{\partial y} &= 0\\
u\frac{\partial u}{\partial x} + v\frac{\partial u}{\partial y} &= -\frac{\partial p}{\partial x} + \nu \left(\frac{\partial^2 u}{\partial x^2} + \frac{\partial^2 u}{\partial y^2} \right)\\
u\frac{\partial v}{\partial x} + v\frac{\partial v}{\partial y} &= -\frac{\partial p}{\partial y} + \nu \left(\frac{\partial^2 v}{\partial x^2} + \frac{\partial^2 v}{\partial y^2} \right)\end{aligned}\end{split}\]
The first equation, the continuity equation, expresses that the flow is incompressible (mathematically, that the flow is “divergence free”). The second and third equations are the momentum or momentum balance equations.
Line 27 of the example shows how we call the NavierStokes
function
to tell Modulus Sym that we want to solve the Navier-Stokes equations.
We set the kinematic viscosity nu=0.01
and the density rho=1.0
.
We set time=False
because this is a steady-state problem (time is not a variable),
and dim=2
because this is a 2D problem.
The function returns a list of Node
objects,
which we will need to keep for later.
)
@modulus.sym.main(config_path="conf", config_name="config")
def run(cfg: ModulusConfig) -> None:
Creating a Neural Network Node
We will create a neural network to approximate the solution of the Navier-Stokes equations for the given boundary conditions. The neural network will have two inputs \(x, y\) and three outputs \(u, v, p\).
Modulus Sym comes with several different neural network architectures. Different architectures may perform better or worse on different problems. “Performance” may refer to any combination of time to solution, total memory use, or efficiency when scaling out on a cluster of parallel computers. For simplicity and not necessarily for best performance, we will use a fully connected neural network in this example.
We create the neural network by calling Modulus Sym’ instantiate_arch
function.
The input_keys
argument specifies the inputs,
and the output_keys
argument the outputs.
We specify each input or output as a Key
object
whose string label is the same as the label of the corresponding Symbol
object.
For example, the input Key("x")
on line 29
refers to the Symbol("x")
later in the file, on line 39.
A Key
class is used for describing inputs and outputs used for graph unroll/evaluation.
The most basic key is just a string that is used
to represent the name of inputs or outputs of the model.
Setting cfg=cfg.arch.fully_connected
selects the default
FullyConnectedArch
neural network architecture.
This tells Modulus Sym to use a multi-layer perceptron (MLP) neural network with 6 layers.
Each layer contains 512 perceptrons
and uses the “swish” (also known as SiLU) activation function.
All these parameters – e.g., the number of layers,
the number of perceptrons in each layer,
and the activation function to use for each layer –
are user configurable.
For this example, the default values are known to work,
though they might not be optimal.
The example shows the complete process
of first creating the PDE node ns
,
then creating the neural network node flow_net
,
and finally creating a list nodes
of all these nodes.
# make list of nodes to unroll graph on
ns = NavierStokes(nu=0.01, rho=1.0, dim=2, time=False)
flow_net = instantiate_arch(
input_keys=[Key("x"), Key("y")],
output_keys=[Key("u"), Key("v"), Key("p")],
cfg=cfg.arch.fully_connected,
)
Once all the PDEs and architectures are defined, we will create a list of nodes to pass to different constraints that need to be satisfied for this problem. The constraints include equations, residuals, and boundary conditions.
Using Hydra to Configure Modulus Sym
Hydra configuration files are at the heart of using Modulus Sym. Each configuration file is a text file in YAML format. Most of Modulus Sym’ features can be customized through Hydra. More information can be found in Modulus Sym Configuration.
We show the configuration file for this example below.
# SPDX-FileCopyrightText: Copyright (c) 2023 - 2024 NVIDIA CORPORATION & AFFILIATES.
# SPDX-FileCopyrightText: All rights reserved.
# SPDX-License-Identifier: Apache-2.0
#
# Licensed under the Apache License, Version 2.0 (the "License");
# you may not use this file except in compliance with the License.
# You may obtain a copy of the License at
#
# http://www.apache.org/licenses/LICENSE-2.0
#
# Unless required by applicable law or agreed to in writing, software
# distributed under the License is distributed on an "AS IS" BASIS,
# WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied.
# See the License for the specific language governing permissions and
# limitations under the License.
defaults:
- modulus_default
- arch:
- fully_connected
- scheduler: tf_exponential_lr
- optimizer: adam
- loss: sum
- _self_
scheduler:
decay_rate: 0.95
decay_steps: 4000
training:
rec_validation_freq: 1000
rec_inference_freq: 2000
rec_monitor_freq: 1000
rec_constraint_freq: 2000
max_steps: 10000
batch_size:
TopWall: 1000
NoSlip: 1000
Interior: 4000
graph:
func_arch: true
We now create the geometry for the LDC example problem. “Geometry” refers to the physical shapes of the domain and its boundaries. The geometry can be created either before or after creating the PDE and the neural network. Modulus Sym lets users create the geometry in different ways. For this example, we will use Modulus Sym’ CSG module. The CSG module supports a wide variety of primitive shapes. In 2D, these shapes include rectangles, circles, triangles, infinite channels, and lines. In 3D, they include spheres, cones, cuboids, infinite channels, planes, cylinders, tori, tetrahedra, and triangular prisms. Users can construct more complicated geometries by combining these primitives using operations like addition, subtraction, and intersection. Please see the API documentation for more details on each shape as well as updates on newly added geometries.
We begin by defining the required symbolic variables for the geometry and then
generating the 2D square geometry by using the Rectangle
geometry object.
In Modulus Sym, a Rectangle
is defined using the coordinates for two opposite
corner points.
The symbolic variable will be used to later sub-sample the geometry to create
different boundaries, interior regions, etc. while defining constraints.
Lines 36-40 of the example show the process of defining a simple geometry.
)
nodes = ns.make_nodes() + [flow_net.make_node(name="flow_network")]
# add constraints to solver
# make geometry
height = 0.1
width = 0.1
x, y = Symbol("x"), Symbol("y")
To visualize the geometry, you can sample either on the boundary or in
the interior of the geometry. One such way is shown below where the
sample_boundary
method samples points on the boundary of the
geometry. The sample_boundary
can be replaced by sample_interior
to sample points in the interior of the geometry.
The var_to_polyvtk function will generate a .vtp
point cloud file for
the geometry. This file can be viewed using tools like ParaView or any other
point cloud plotting software.
samples = geo.sample_boundary(1000)
var_to_polyvtk(samples, './geo')
The geometry module also features functionality like
translate
and rotate
to generate shapes in arbitrary
orientation. The use of these will be covered in upcoming tutorials.
Setting up the Domain
The Domain
object contains the PDE and its boundary conditions,
as well as the Validator
and Inferencer
objects in this example.
Modulus Sym calls the PDE and its boundary conditions “constraints.”
The PDE, in particular, constrains the outputs on the interior of the domain.
The Domain
and the configuration options both in turn
will be used to create an instance of the Solver
class.
Lines 42-43 of the example show how to create a Domain
object.
We will add constraints separately, later in the example.
x, y = Symbol("x"), Symbol("y")
rec = Rectangle((-width / 2, -height / 2), (width / 2, height / 2))
# make ldc domain
Apart from constraints, you can add various other utilities to the Domain
such as monitors, validation data, or points on which to do inference.
Each of these is covered in detail in this example.
Adding constraints to the Domain
can be thought of as adding specific
constraints to the neural network optimization problem. For this physics-driven
problem, these constraints are the boundary conditions and equation residuals.
The goal is to satisfy the boundary conditions exactly,
and have the interior (PDE) residual (a measure of the error) go to zero.
The constraints can be specified within
Modulus Sym using classes like PointwiseBoundaryConstrant
and PointwiseInteriorConstraint
.
Modulus Sym then constructs a loss function –
a measure of the neural network’s approximation error –
from the constraints.
By default, Modulus Sym will use L2 (sum of squares) loss, but it is possible to change this.
The optimizer will train the neural network by minimizing the loss function.
This way of specifying the constraints is called soft constraints.
In what follows, we will explain how to specify the constraints.
Boundary Constraints
To create a boundary condition constraint in Modulus Sym, first sample the points on that part of the geometry, then specify the nodes you want to evaluate on those points, and finally assign them the desired true values.
“Sample the points” refers to creating a set of points that live on that part of the geometry. The “nodes” here refer to the list of PDE and neural network nodes created on line 33 of the example. Some examples and documentation will use in place of “evaluate,” a phrase like “unroll the nodes” on “unroll the graph on the list of nodes.” “Unroll” means “construct the computational graph on the list of nodes.”
That last point calls for some elaboration.
Each Constraint
takes in a list of Node
s
with each Node
having a list of input and output Key
s.
The inputs to the Constraint
are just the coordinates (x and y in this example)
and the output is a loss value. As part of computing the loss value,
the Constraint
might have a model that computes intermediate quantities.
In this example, the interior Constraint
requires derivatives of the output with respect to the input
in order to compute residuals of the continuity and momentum equations.
The loss value comes from the sum of squares of those residuals.
Internally, Modulus Sym needs to figure out how to evaluate the model and the PDE
and compute the required intermediate quantities (the derivatives, for example).
This amounts to connecting nodes (quantities to compute)
with edges (methods for combining quantities to compute other quantities)
to create a “computational graph” for that Constraint
.
This process is what we typically refer to as “unrolling the graph”.
We sample a boundary by using a PointwiseBoundaryConstraint
object.
This will sample the entire boundary of the geometry you specify in the geometry
argument
when creating the object.
For this example, once you set geometry=rec
, all the sides of the rectangle are sampled.
A particular boundary of the geometry can be sub-sampled by using the criteria
argument.
This can be any symbolic function defined using the sympy
library.
For example, to sample the top wall, wet set criteria=Eq(y,height/2)
.
The constraint’s outvar
argument specifies the desired values
for the boundary condition as a dictionary.
For example, outvar={"u": 1.0, "v": 0.0}
says that
the value of the u
output is 1.0 on that boundary,
and the value of the v
output is 0.0 on that boundary.
The constraint’s batch_size
argument specifies the number of points to sample on each boundary.
The
criteria
argument is optional. With nocriteria
, all the boundaries in the geometry are sampled.The network directory will only show the points sampled in a single batch. However, the total points used in the training can be computed by further multiplying the batch size by
batch_per_epoch
parameter. The default value of this is set to 1000. In the example above, the total points sampled on the Top BC will be \(1000 \times 1000 = 1000000\).
For the LDC problem, we define the top wall with a \(u\) velocity equal to 1 \(m/s\) in the \(+ve\) x-direction, and define the velocity on all other walls as stationary (\(u,v = 0\)). Fig. 4 shows that this can give rise to sharp discontinuities, wherein the \(u\) velocity jumps sharply from \(0\) to \(1.0\). As outlined in the theory explanation Spatial Weighting of Losses (SDF weighting), this sharp discontinuity can be avoided by specifying the weighting for this boundary such that the weight of the loss varies continuously and is 0 on the boundaries. You can use the function \(1.0 - 20.0|x|\) as shown in Fig. 4 for this purpose. Similar to the advantages of weighting losses for equations (see Fig. 28), eliminating such discontinuities speeds up convergence and improves accuracy.
Weights to any variables can be specified as an input to the
lambda_weighting
parameter.
Fig. 4 Weighting the sharp discontinuities in the boundary condition
PDE Constraints
This example problem’s PDEs need to be enforced on all the points in the interior of the geometry to achieve the desired solution. Analogously to the boundaries, this requires first sampling the points inside the required geometry, then specifying the nodes to evaluate on those points, and finally assigning them the true values that you want for them.
We use the PointwiseInteriorConstraint
class
to sample points in the interior of a geometry.
Its outvar
argument specifies the equations to solve as a dictionary.
For the 2D LDC case, the continuity equation and the
momentum equations in \(x\) and \(y\) directions are needed.
Therefore, the dictionary has keys for 'continuity'
, 'momentum_x'
and 'momentum_y'
.
Each of these keys has the corresponding value 0.
This represents the desired residual for these keys at the chosen points
(in this case, the entire interior of the LDC geometry).
A nonzero value is allowed, and behaves as a custom forcing or source term.
More examples of this can be found in the later chapters of this User Guide.
To see how the equation keys are defined, you can look at
the Modulus Sym source or see the API documentation (modulus/eq/pdes/navier_stokes.py
).
As an example, the definition of 'continuity'
is presented here.
...
# set equations
self.equations = {}
self.equations['continuity'] = rho.diff(t) + (rho*u).diff(x) + (rho*v).diff(y) + (rho*w).diff(z)
...
The equations below show the part of the loss function corresponding to each of the three equations in the system of PDEs.
(2)\[L_{continuity}= \frac{V}{N} \sum_{i=0}^{N} ( 0 - continuity(x_i,y_i))^2\]
(3)\[L_{momentum_{x}}= \frac{V}{N} \sum_{i=0}^{N} ( 0 - momentum_{x}(x_i,y_i))^2\]
(4)\[L_{momentum_{y}}= \frac{V}{N} \sum_{i=1}^{n} (0 - momentum_{y}(x_i, y_i))^2\]
The bounds
parameter determines the range for sampling the values
for variables \(x\) and \(y\). The lambda_weighting
parameter is used to
determine the weights for different losses. In this problem, you will weight
each equation at each point by its distance from the boundary by using
the Signed Distance Field (SDF) of the geometry. This implies that the
points away from the boundary have a larger weight compared to the ones
closer to the boundary. This weighting leads to faster convergence
since it avoids discontinuities at the boundaries
(see section Spatial Weighting of Losses (SDF weighting)).
The lambda_weighting
parameter is optional. If not specified,
the loss for each equation/boundary variable at each point is weighted
equally.
# make ldc domain
ldc_domain = Domain()
# top wall
top_wall = PointwiseBoundaryConstraint(
nodes=nodes,
geometry=rec,
outvar={"u": 1.0, "v": 0},
batch_size=cfg.batch_size.TopWall,
lambda_weighting={"u": 1.0 - 20 * Abs(x), "v": 1.0}, # weight edges to be zero
criteria=Eq(y, height / 2),
)
ldc_domain.add_constraint(top_wall, "top_wall")
# no slip
no_slip = PointwiseBoundaryConstraint(
nodes=nodes,
geometry=rec,
outvar={"u": 0, "v": 0},
batch_size=cfg.batch_size.NoSlip,
criteria=y < height / 2,
)
ldc_domain.add_constraint(no_slip, "no_slip")
# interior
interior = PointwiseInteriorConstraint(
nodes=nodes,
geometry=rec,
outvar={"continuity": 0, "momentum_x": 0, "momentum_y": 0},
batch_size=cfg.batch_size.Interior,
lambda_weighting={
"continuity": Symbol("sdf"),
"momentum_x": Symbol("sdf"),
"momentum_y": Symbol("sdf"),
},
)
Adding Validation Node
“Validation” means comparing the approximate solution computed by Modulus Sym
with data representing results obtained by some other method.
The results could come from any combination of simulation or experiment.
This section shows how to
set up such a validation domain in Modulus Sym. Here, we use results from
OpenFOAM, an open-source computational fluid dynamics (CFD) solver
that discretizes the Navier-Stokes equations on a mesh
and solves them using nonlinear and linear solvers not based on neural networks.
Results can be imported into Modulus Sym from any of various standard file formats,
including .csv
, .npz
, or .vtk
.
Modulus Sym requires that the data be converted into a dictionary of NumPy variables for input and output.
For a .csv
file, this can be done using the csv_to_dict
function.
The validation data is then added to the domain using PointwiseValidator
.
The dictionary of generated NumPy arrays for input and output variables is used as an input.
)
ldc_domain.add_constraint(interior, "interior")
# add validator
file_path = "openfoam/cavity_uniformVel0.csv"
if os.path.exists(to_absolute_path(file_path)):
mapping = {"Points:0": "x", "Points:1": "y", "U:0": "u", "U:1": "v", "p": "p"}
openfoam_var = csv_to_dict(to_absolute_path(file_path), mapping)
openfoam_var["x"] += -width / 2 # center OpenFoam data
openfoam_var["y"] += -height / 2 # center OpenFoam data
openfoam_invar_numpy = {
key: value for key, value in openfoam_var.items() if key in ["x", "y"]
}
openfoam_outvar_numpy = {
key: value for key, value in openfoam_var.items() if key in ["u", "v"]
}
openfoam_validator = PointwiseValidator(
nodes=nodes,
invar=openfoam_invar_numpy,
true_outvar=openfoam_outvar_numpy,
batch_size=1024,
plotter=ValidatorPlotter(),
)
We create a Solver
with the configuration options cfg
and the Domain
that we just finished setting up.
We then call the solve()
method on the Solver
to solve the problem.
f"Directory{file_path}does not exist. Will skip adding validators. Please download the additional files from NGC https://catalog.ngc.nvidia.com/orgs/nvidia/teams/modulus/resources/modulus_sym_examples_supplemental_materials"
)
# make solver
The file set up for Modulus Sym is now complete. You are now ready to solve the CFD simulation using Modulus Sym’ neural network solver.
Training the model
Executing the Python script will train the neural network.
python ldc_2d.py
The console should print the losses at each step. You can also use Tensorboard to monitor the losses graphically as training progresses. We will explain how to set up and use Tensorboard below.
Setting up Tensorboard
Tensorboard is a great tool for visualization of machine learning experiments. To visualize the various training and validation losses, Tensorboard can be set up as follows:
In a separate terminal window, navigate to the working directory of the example (
examples/ldc/
in this case)Type in the following command on the command line:
tensorboard --logdir=./ --port=7007
Specify the port you want to use. This example uses
7007
. Once running, the command prompt shows the url that you will use to display the results.To view results, open a web browser and go to the url shown by the command prompt. An example would be: http://localhost:7007/#scalars. A window as shown in Fig. 5 should open up in the browser window.
The Tensorboard window displays the various losses at each step
during the training. The AdamOptimizer
loss is the total loss computed
by the network. The loss_continuity
, loss_momentum_x
and
loss_momentum_y
determine the loss computed for the continuity and
Navier-Stokes equations in the \(x\) and \(y\) directions, respectively. The loss_u
and loss_v
determine how well the boundary conditions are satisfied (soft
constraints).
Fig. 5 Tensorboard Interface.
Output Files
The checkpoint directory is saved based on the results recording frequency
specified as the 'rec_results_freq'
configuration option. The network directory folder
(in this case 'outputs/'
) contains the following
important files/directories.
optim_checkpoint.pth
,flow_network.pth
: Optimizer checkpoint and flow network saved during training.constraints
: This directory contains the data computed on the points added to the domain usingadd_constraint()
. The data are stored as.vtp
files, which can be viewed using visualization tools like Paraview. You will see the true and predicted values of all the nodes that were passed to thenodes
argument of the constraint. For example, the./constraints/Interior.vtp
will have the variables forpred_continuity
andtrue_continuity
representing the network predicted and the true value set forcontinuity
. Figure Fig. 6 shows the comparison between true and computed continuity. This directory is useful to see how well the boundary conditions and equations are being satisfied at the sampled points.
Fig. 6 Visualization using Paraview. Left: Continuity as specified in the domain definition. Right: Computed continuity after training.
validators:
This directory contains the data computed on the points added in the domain usingadd_validator()
. This domain is more useful for validating the data with respect to a reference solution. The data are stored as.vtp
and.npz
files (based on thesave_filetypes
configuration option). The.vtp
files can be viewed using visualization tools like Paraview. The.vtp
and.npz
files in this directory will report predicted, true (validation data), pred (model’s inference) on the chosen points. For example, the./validators/validator.vtp
contains variables liketrue_u
,true_v
,true_p
, andpred_u
,pred_v
,pred_p
corresponding to the true and the network predicted values for the variables \(u\), \(y\), and \(p\). Figure Fig. 7 shows the comparison between true and Modulus Sym predicted values of such variables.
Fig. 7 Comparison with OpenFOAM results
Monitor Node
Modulus Sym allows you to monitor desired quantities by plotting them every
fixed number of iterations in Tensorboard as the simulation progresses,
and analyze convergence based on the relative changes in the
monitored quantities. A PointwiseMonitor
can be used to create such an
feature. Examples of such quantities can be point values of variables,
surface averages, volume averages or any derived quantities that can be
formed using the variables being solved.
The flow variables are available as PyTorch tensors. You can perform tensor operations to create any desired derived variable of your choice. The code below shows the monitors for continuity and momentum imbalance in the interior.
The points to sample can be selected using the sample_interior
and sample_boundary
methods.
...
# add monitors
global_monitor = PointwiseMonitor(
rec.sample_interior(4000, bounds={x: (-width/2, width/2), y: (-height/2, height/2)}),
output_names=["continuity", "momentum_x", "momentum_y"],
metrics={
"mass_imbalance": lambda var: torch.sum(
var["area"] * torch.abs(var["continuity"])
),
"momentum_imbalance": lambda var: torch.sum(
var["area"]
* (torch.abs(var["momentum_x"]) + torch.abs(var["momentum_y"]))
),
},
nodes=nodes,
)
ldc_domain.add_monitor(global_monitor)
Fig. 8 LDC Monitors in Tensorboard
Inferencer Node
Modulus Sym also allows you to plot the results on arbitrary domains. You can then monitor these domains
in Paraview or Tensorboard itself. More details on how to add Modulus Sym information to Tensorboard can be
found in TensorBoard in Modulus Sym. The code below shows use of PointwiseInferencer
.
)
ldc_domain.add_validator(openfoam_validator)
# add inferencer data
grid_inference = PointwiseInferencer(
nodes=nodes,
invar=openfoam_invar_numpy,
output_names=["u", "v", "p"],
batch_size=1024,
plotter=InferencerPlotter(),
Fig. 9 LDC Inference in Tensorboard