PBC Layer

docs/source/_rst/_code.rst

@@ -68,6 +68,7 @@ Layers
     Spectral convolution <layers/spectral.rst>
     Fourier layers <layers/fourier.rst>
     Continuous convolution <layers/convolution.rst>
+    Coordinates embeddings <layers/embedding.rst>
 
 
 Equations and Operators

docs/source/_rst/_tutorial.rst

@@ -21,7 +21,7 @@ Physics Informed Neural Networks
    Two dimensional Poisson problem using Extra Features Learning<tutorials/tutorial2/tutorial.rst>
    Two dimensional Wave problem with hard constraint<tutorials/tutorial3/tutorial.rst>
    Resolution of a 2D Poisson inverse problem<tutorials/tutorial7/tutorial.rst>
-
+   Periodic Boundary Conditions for Helmotz Equation<tutorials/tutorial9/tutorial.rst>
 
 Neural Operator Learning
 ------------------------

docs/source/_rst/layers/embedding.rst

@@ -0,0 +1,8 @@
+Coordinates embeddings
+======================
+.. currentmodule:: pina.model.layers.embedding
+
+.. autoclass:: PBCEmbedding
+    :members:
+    :show-inheritance:
+

docs/source/_rst/layers/pod.rst

@@ -0,0 +1,15 @@
+Spectral Convolution
+======================
+.. currentmodule:: pina.model.layers.spectral
+
+.. autoclass:: SpectralConvBlock1D
+    :members:
+    :show-inheritance:
+
+.. autoclass:: SpectralConvBlock2D
+    :members:
+    :show-inheritance:
+
+.. autoclass:: SpectralConvBlock3D
+    :members:
+    :show-inheritance:

docs/source/_rst/tutorials/tutorial9/tutorial.rst

@@ -0,0 +1,226 @@
+Tutorial: One dimensional Helmotz equation using Periodic Boundary Conditions
+=============================================================================
+
+This tutorial presents how to solve with Physics-Informed Neural
+Networks (PINNs) a one dimensional Helmotz equation with periodic
+boundary conditions (PBC). We will train with standard PINN’s training
+by augmenting the input with periodic expasion as presented in `An
+expert’s guide to training physics-informed neural
+networks <https://arxiv.org/abs/2308.08468>`__.
+
+First of all, some useful imports.
+
+.. code:: ipython3
+
+    import torch
+    import matplotlib.pyplot as plt
+
+    from pina import Condition, Plotter
+    from pina.problem import SpatialProblem
+    from pina.operators import laplacian
+    from pina.model import FeedForward
+    from pina.model.layers import PeriodicBoundaryEmbedding  # The PBC module
+    from pina.solvers import PINN
+    from pina.trainer import Trainer
+    from pina.geometry import CartesianDomain
+    from pina.equation import Equation
+
+The problem definition
+----------------------
+
+The one-dimensional Helmotz problem is mathematically written as:
+
+.. math::
+
+
+   \begin{cases}
+   \frac{d^2}{dx^2}u(x) - \lambda u(x) -f(x) &=  0 \quad x\in(0,2)\\
+   u^{(m)}(x=0) - u^{(m)}(x=2) &= 0 \quad m\in[0, 1, \cdots]\\
+   \end{cases}
+
+In this case we are asking the solution to be :math:`C^{\infty}`
+periodic with period :math:`2`, on the inifite domain
+:math:`x\in(-\infty, \infty)`. Notice that the classical PINN would need
+inifinite conditions to evaluate the PBC loss function, one for each
+derivative, which is of course infeasable… A possible solution,
+diverging from the original PINN formulation, is to use *coordinates
+augmentation*. In coordinates augmentation you seek for a coordinates
+transformation :math:`v` such that :math:`x\rightarrow v(x)` such that
+the periodicity condition $ u^{(m)}(x=0) - u^{(m)}(x=2) = 0
+:raw-latex:`\quad `m:raw-latex:`\in[0, 1, \cdots] `$ is satisfied.
+
+For demonstration porpuses the problem specifics are
+:math:`\lambda=-10\pi^2`, and
+:math:`f(x)=-6\pi^2\sin(3\pi x)\cos(\pi x)` which gives a solution that
+can be computed analytically :math:`u(x) = \sin(\pi x)\cos(3\pi x)`.
+
+.. code:: ipython3
+
+    class Helmotz(SpatialProblem):
+        output_variables = ['u']
+        spatial_domain = CartesianDomain({'x': [0, 2]})
+
+        def helmotz_equation(input_, output_):
+            x = input_.extract('x')
+            u_xx = laplacian(output_, input_, components=['u'], d=['x'])
+            f = - 6.*torch.pi**2 * torch.sin(3*torch.pi*x)*torch.cos(torch.pi*x)
+            lambda_ = - 10. * torch.pi ** 2
+            return u_xx - lambda_ * output_ - f
+
+        # here we write the problem conditions
+        conditions = {
+            'D': Condition(location=spatial_domain,
+                           equation=Equation(helmotz_equation)),
+        }
+
+        def helmotz_sol(self, pts):
+            return torch.sin(torch.pi * pts) * torch.cos(3. * torch.pi * pts)
+
+        truth_solution = helmotz_sol
+
+    problem = Helmotz()
+
+    # let's discretise the domain
+    problem.discretise_domain(200, 'grid', locations=['D'])
+
+As usual the Helmotz problem is written in **PINA** code as a class. The
+equations are written as ``conditions`` that should be satisfied in the
+corresponding domains. The ``truth_solution`` is the exact solution
+which will be compared with the predicted one. We used latin hypercube
+sampling for choosing the collocation points.
+
+Solving the problem with a Periodic Network
+-------------------------------------------
+
+Any :math:`\mathcal{C}^{\infty}` periodic function
+:math:`u : \mathbb{R} \rightarrow \mathbb{R}` with period
+:math:`L\in\mathbb{N}` can be constructed by composition of an arbitrary
+smooth function :math:`f : \mathbb{R}^n \rightarrow \mathbb{R}` and a
+given smooth periodic function
+:math:`v : \mathbb{R} \rightarrow \mathbb{R}^n` with period :math:`L`,
+that is :math:`u(x) = f(v(x))`. The formulation is generalizable for
+arbitrary dimension, see `A method for representing periodic functions
+and enforcing exactly periodic boundary conditions with deep neural
+networks <https://arxiv.org/pdf/2007.07442>`__.
+
+In our case, we rewrite
+:math:`v(x) = \left[1, \cos\left(\frac{2\pi}{L} x\right), \sin\left(\frac{2\pi}{L} x\right)\right]`,
+i.e the coordinates augmentation, and
+:math:`f(\cdot) = NN_{\theta}(\cdot)` i.e. a neural network. The
+resulting neural network obtained by composing :math:`f` with :math:`v`
+gives the PINN approximate solution, that is
+:math:`u(x) \approx u_{\theta}(x)=NN_{\theta}(v(x))`.
+
+In **PINA** this translates in using the ``PeriodicBoundaryEmbedding`` layer for
+:math:`v`, and any ``pina.model`` for :math:`NN_{\theta}`. Let’s see it
+in action!
+
+.. code:: ipython3
+
+    # we encapsulate all modules in a torch.nn.Sequential container
+    model = torch.nn.Sequential(PeriodicBoundaryEmbedding(input_dimension=1,
+                                             periods=2),
+                                FeedForward(input_dimensions=3, # output of PeriodicBoundaryEmbedding = 3 * input_dimension
+                                            output_dimensions=1,
+                                            layers=[10, 10]))
+
+As simple as that! Notice in higher dimension you can specify different
+periods for all dimensions using a dictionary,
+e.g. ``periods={'x':2, 'y':3, ...}`` would indicate a periodicity of
+:math:`2` in :math:`x`, :math:`3` in :math:`y`, and so on…
+
+We will now sole the problem as usually with the ``PINN`` and
+``Trainer`` class.
+
+.. code:: ipython3
+
+    pinn = PINN(problem=problem, model=model)
+    trainer = Trainer(pinn, max_epochs=5000, accelerator='cpu', enable_model_summary=False) # we train on CPU and avoid model summary at beginning of training (optional)
+    trainer.train()
+
+
+.. parsed-literal::
+
+    GPU available: True (mps), used: False
+    TPU available: False, using: 0 TPU cores
+    IPU available: False, using: 0 IPUs
+    HPU available: False, using: 0 HPUs
+
+.. parsed-literal::
+
+    `Trainer.fit` stopped: `max_epochs=5000` reached.
+
+
+.. parsed-literal::
+
+    Epoch 4999: 100%|██████████| 1/1 [00:00<00:00, 155.47it/s, v_num=20, D_loss=0.0123, mean_loss=0.0123]
+
+
+We are going to plot the solution now!
+
+.. code:: ipython3
+
+    pl = Plotter()
+    pl.plot(pinn)
+
+
+
+.. image:: tutorial_files/tutorial_11_0.png
+
+
+Great, they overlap perfectly! This seeams a good result, considering
+the simple neural network used to some this (complex) problem. We will
+now test the neural network on the domain :math:`[-4, 4]` without
+retraining. In principle the periodicity should be present since the
+:math:`v` function ensures the periodicity in :math:`(-\infty, \infty)`.
+
+.. code:: ipython3
+
+    # plotting solution
+    with torch.no_grad():
+        # Notice here we put [-4, 4]!!!
+        new_domain = CartesianDomain({'x' : [0, 4]})
+        x = new_domain.sample(1000, mode='grid')
+        fig, axes = plt.subplots(1, 3, figsize=(15, 5))
+        # Plot 1
+        axes[0].plot(x, problem.truth_solution(x), label=r'$u(x)$', color='blue')
+        axes[0].set_title(r'True solution $u(x)$')
+        axes[0].legend(loc="upper right")
+        # Plot 2
+        axes[1].plot(x, pinn(x), label=r'$u_{\theta}(x)$', color='green')
+        axes[1].set_title(r'PINN solution $u_{\theta}(x)$')
+        axes[1].legend(loc="upper right")
+        # Plot 3
+        diff = torch.abs(problem.truth_solution(x) - pinn(x))
+        axes[2].plot(x, diff, label=r'$|u(x) - u_{\theta}(x)|$', color='red')
+        axes[2].set_title(r'Absolute difference $|u(x) - u_{\theta}(x)|$')
+        axes[2].legend(loc="upper right")
+        # Adjust layout
+        plt.tight_layout()
+        # Show the plots
+        plt.show()
+
+
+
+.. image:: tutorial_files/tutorial_13_0.png
+
+
+It is pretty clear that the network is periodic, with also the error
+following a periodic pattern. Obviusly a longer training, and a more
+expressive neural network could improve the results!
+
+What’s next?
+------------
+
+Nice you have completed the one dimensional Helmotz tutorial of
+**PINA**! There are multiple directions you can go now:
+
+1. Train the network for longer or with different layer sizes and assert
+   the finaly accuracy
+
+2. Apply the ``PeriodicBoundaryEmbedding`` layer for a time-dependent problem (see
+   reference in the documentation)
+
+3. Exploit extrafeature training ?
+
+4. Many more…

pina/model/layers/__init__.py

@@ -9,6 +9,7 @@
     "FourierBlock2D",
     "FourierBlock3D",
     "PODBlock",
+    "PeriodicBoundaryEmbedding"
 ]
 
 from .convolution_2d import ContinuousConvBlock
@@ -20,3 +21,4 @@
 )
 from .fourier import FourierBlock1D, FourierBlock2D, FourierBlock3D
 from .pod import PODBlock
+from .embedding import PeriodicBoundaryEmbedding